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Frantz JA, Hart MB, McGinnis CL, Myers JD, Ewing KJ, Selby JB, Major KJ, Watnik AT, Sanghera JS. Measurement of the Optical Constants of Sand Samples Using Ellipsometry on Sand-Adhesive Composites. Appl Spectrosc 2024; 78:403-411. [PMID: 38385358 DOI: 10.1177/00037028241231296] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 02/23/2024]
Abstract
In order to model the propagation of light through a sand cloud, it is critical to have accurate data for the optical constants of the sand particles that comprise it. The same holds true for modeling propagation through particles of any type suspended in a medium. Few methods exist, however, to measure these quantities with high accuracy. In this paper, a characterization method based on spectroscopic ellipsometry (SE) that can be applied to a particulate material is presented. In this method, a polished disc of an adhesive compound is prepared, and its optical constants are measured. Next, a mixture of the adhesive and a sand sample is prepared and processed into a polished disc, and SE is performed. By treating the mixture as a Bruggeman effective medium, the optical constants of the particulate material are extracted. For verification of the proposed method, it is first applied to pure silica powder, demonstrating good agreement between measured optical constants and literature values. It is then applied to Arizona road dust, a standard reference material, as well as real desert sand samples. The resulting optical constant data is input into a rigorous scattering model to predict extinction coefficients for various types of sand. Modeling results are compared to spectroscopic measurements on static sand samples, demonstrating good agreement between predicted and measured spectral properties including the presence of a Christiansen feature near a wavelength of 8 µm.
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Affiliation(s)
- Jesse A Frantz
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
| | - Matthew B Hart
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
| | - Cobey L McGinnis
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
| | - Jason D Myers
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
| | - Kenneth J Ewing
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
| | | | - Kevin J Major
- Institute for Functional Materials and Devices, Lehigh University, Bethlehem, Pennsylvania, USA
| | - Abbie T Watnik
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
| | - Jasbinder S Sanghera
- Optical Sciences Division, U.S. Naval Research Laboratory, Washington, District of Columbia, USA
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2
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Kumari P, Hajduk B, Bednarski H, Jarka P, Janeczek H, Łapkowski M. Exploring the Influence of P3HT on PTCA Crystallization and Phase Behavior in Thin Films. Nanomaterials (Basel) 2023; 13:2918. [PMID: 37999272 PMCID: PMC10675274 DOI: 10.3390/nano13222918] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 09/29/2023] [Revised: 10/30/2023] [Accepted: 11/07/2023] [Indexed: 11/25/2023]
Abstract
The thermal properties and alignment of crystallinity of materials in thin films play crucial roles in the performance and reliability of various devices, especially in the fields of electronics, materials science, and engineering. The slight variations in the molecular packing of the active layer can make considerable differences in the optical and thermal properties. Herein, we aim to investigate the tuning of the physical properties of a blended thin film of n-type small organic molecules of perylene-3,4,9,10-tetracarboxylic acid (PTCA-SMs) with the mixing of the p-type polymer poly(3-hexylthiophene) (P3HT). The resulting thin films exhibit an enhanced surface crystallinity compared to the pristine material, leading to the formation of long crystallites, and these crystallites are thermally stable in the solid state, as confirmed by X-ray diffraction (XRD), atomic force microscopy (AFM), and thermal analysis using variable-temperature spectroscopic ellipsometry (VTSE) and differential scanning calorimetry (DSC). We believe that the crystalline structure of the obtained P3HT/PTCA-SMs blends is a combination of edge-on and face-on orientations, which enable the potential use of this material as an active layer in organic electronics.
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Affiliation(s)
- Pallavi Kumari
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska Str., 41-819 Zabrze, Poland; (B.H.); (H.B.); (H.J.); (M.Ł.)
| | - Barbara Hajduk
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska Str., 41-819 Zabrze, Poland; (B.H.); (H.B.); (H.J.); (M.Ł.)
| | - Henryk Bednarski
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska Str., 41-819 Zabrze, Poland; (B.H.); (H.B.); (H.J.); (M.Ł.)
| | - Paweł Jarka
- Department of Engineering Materials and Biomaterials, Silesian University of Technology, 18a Konarskiego Str., 41-100 Gliwice, Poland;
| | - Henryk Janeczek
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska Str., 41-819 Zabrze, Poland; (B.H.); (H.B.); (H.J.); (M.Ł.)
| | - Mieczysław Łapkowski
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska Str., 41-819 Zabrze, Poland; (B.H.); (H.B.); (H.J.); (M.Ł.)
- Department of Physical Chemistry and Technology of Polymers, Faculty of Chemistry, Silesian University of Technology, M. Strzody 9, 44-100 Gliwice, Poland
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3
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Liu J, Zhang Z. Polymer-Embedding Germanium Nanostrip Waveguide of High Polarization Extinction. Polymers (Basel) 2023; 15:4093. [PMID: 37896336 PMCID: PMC10610098 DOI: 10.3390/polym15204093] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Received: 09/18/2023] [Revised: 10/06/2023] [Accepted: 10/08/2023] [Indexed: 10/29/2023] Open
Abstract
Germanium (Ge) nanostrip was embedded in a polymer and studied as a waveguide. The measurements reveal that this new type of semiconductor/polymer heterogeneous waveguide exhibits strong absorption for the TE mode from 1500 nm to 2004 nm, while the propagation loss for the TM mode declines from 20.56 dB/cm at 1500 nm to 4.89 dB/cm at 2004 nm. The transmission characteristics serve as an essential tool for verifying the optical parameters (n-κ, refractive index, and extinction coefficient) of the strip, addressing the ambiguity raised by spectroscopic ellipsometry regarding highly absorbing materials. Furthermore, the observed strong absorption for the TE mode at 2004 nm is well beyond the cut-off wavelength of the crystalline bulk Ge (~1850 nm at room temperature). This redshift is modeled to manifest the narrowing of the Tauc-fitted bandgap due to the grain order effect in the amorphous Ge layer. The accurate measurement of the nanometer-scale light-absorbing strips in a waveguide form is a crucial step toward the accurate design of integrated photonic devices that utilize such components.
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Affiliation(s)
- Jinyuan Liu
- College of Information Science and Electronic Engineering, Zhejiang University, Hangzhou 310027, China;
- Laboratory of Photonic Integration, School of Engineering, Westlake University, Hangzhou 310024, China
| | - Ziyang Zhang
- Laboratory of Photonic Integration, School of Engineering, Westlake University, Hangzhou 310024, China
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4
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Shamsabadi AA, Fang H, Zhang D, Thakur A, Chen CY, Zhang A, Wang H, Anasori B, Soroush M, Gogotsi Y, Fakhraai Z. The Evolution of MXenes Conductivity and Optical Properties Upon Heating in Air. Small Methods 2023; 7:e2300568. [PMID: 37454348 DOI: 10.1002/smtd.202300568] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 05/01/2023] [Revised: 06/27/2023] [Indexed: 07/18/2023]
Abstract
MXenes, a family of 2D transition-metal carbides and nitrides, have excellent electrical conductivity and unique optical properties. However, MXenes oxidize in ambient conditions, which is accelerated upon heating. Intercalation of water also causes hydrolysis accelerating oxidation. Developing new tools to readily characterize MXenes' thermal stability can enable deeper insights into their structure-property relationships. Here, in situ spectroscopic ellipsometry (SE) is employed to characterize the optical properties of three types of MXenes (Ti3 C2 Tx , Mo2 TiC2 Tx , and Ti2 CTx ) with varied composition and atomistic structures to investigate their thermal degradation upon heating under ambient environment. It is demonstrated that changes in MXene extinction and optical conductivity in the visible and near-IR regions correlate well with the amount of intercalated water and hydroxyl termination groups and the degree of oxidation, measured using thermogravimetric analysis. Among the three MXenes, Ti3 C2 Tx and Ti2 CTx , respectively, have the highest and lowest thermal stability, indicating the role of transition-metal type, synthesis route, and the number of atomic layers in MXene flakes. These findings demonstrate the utility of SE as a powerful in situ technique for rapid structure-property relationship studies paving the way for the further design, fabrication, and property optimization of novel MXene materials.
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Affiliation(s)
- Ahmad A Shamsabadi
- Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104, USA
| | - Hui Fang
- Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104, USA
| | - Danzhen Zhang
- A.J. Drexel Nanomaterials Institute and Department of Material Science and Engineering, Drexel University, Philadelphia, PA 19104, USA
| | - Anupma Thakur
- Department of Mechanical and Energy Engineering and Integrated Nanosystems Development Institute, Purdue School of Engineering and Technology, Indiana University-Purdue University Indianapolis, Indianapolis, IN, 46202, USA
| | - Cindy Y Chen
- Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104, USA
| | - Aixi Zhang
- Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104, USA
| | - Haonan Wang
- Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104, USA
| | - Babak Anasori
- Department of Mechanical and Energy Engineering and Integrated Nanosystems Development Institute, Purdue School of Engineering and Technology, Indiana University-Purdue University Indianapolis, Indianapolis, IN, 46202, USA
- School of Materials Engineering, Purdue University, West Lafayette, IN 47907, USA
| | - Masoud Soroush
- Department of Chemical and Biological Engineering, Drexel University, Philadelphia, PA 19104, USA
| | - Yury Gogotsi
- A.J. Drexel Nanomaterials Institute and Department of Material Science and Engineering, Drexel University, Philadelphia, PA 19104, USA
| | - Zahra Fakhraai
- Department of Chemistry, University of Pennsylvania, Philadelphia, PA 19104, USA
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Plikusiene I, Maciulis V, Juciute S, Ramanavicius A, Ramanaviciene A. Study of SARS-CoV-2 Spike Protein Wild-Type and the Variants of Concern Real-Time Interactions with Monoclonal Antibodies and Convalescent Human Serum. Biosensors (Basel) 2023; 13:784. [PMID: 37622870 PMCID: PMC10452135 DOI: 10.3390/bios13080784] [Citation(s) in RCA: 4] [Impact Index Per Article: 4.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [MESH Headings] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/29/2023] [Revised: 07/25/2023] [Accepted: 07/31/2023] [Indexed: 08/26/2023]
Abstract
The spike (S) protein and its receptor-binding domain (RBD) of the coronavirus SARS-CoV-2 have been continually evolving, yielding the majority of significant missense mutations and new variants of concern. In this study, we examined how monoclonal antibodies against RBD (mAbs-SCoV2-RBD) and polyclonal antibodies present in convalescent human serum specifically interact with the S protein of wild-type and SARS-CoV-2 variants of concern (VOCs) in real time and how this can be reflected through surface mass density. Moreover, we combined two distinct, label-free measurement techniques: one based on changes in surface electromagnetic waves after reflection from the surface, and the other on changes in acoustic waves. The results demonstrated that dry surface mass density (ΓSE) of mAbs-SCoV2-RBD attached to the RBD of the S protein decreases three-fold, from 148 ng/cm2 to 46 ng/cm2, due to the B.1.351 or so-called beta mutation of coronavirus and its S protein (SCoV2-β). Consequently, the obtained wet mass ΓQCM-D resulted in values two times lower, from 319 ng/cm2 to 158 ng/cm2, and the hydration of mAbs-SCoV2-RBD/SCoV2-β immune complex was 70.88%. Conversely, when polyclonal antibodies present in convalescent human serum form immune complexes with the S protein of SARS-CoV-2 variants of concern, the ΓSE decreased from 279 ng/cm2 to 249 ng/cm2, and ΓQCM-D from 1545 ng/cm2 to 1366 ng/cm2. These results can give insights into the differences between the interaction of monoclonal and polyclonal antibodies with SARS-CoV-2 VOCs.
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Affiliation(s)
- Ieva Plikusiene
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko str. 24, LT-03225 Vilnius, Lithuania
- State Research Institute Center for Physical and Technological Sciences, Sauletekio ave. 3, LT-10257 Vilnius, Lithuania
| | - Vincentas Maciulis
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko str. 24, LT-03225 Vilnius, Lithuania
- State Research Institute Center for Physical and Technological Sciences, Sauletekio ave. 3, LT-10257 Vilnius, Lithuania
| | - Silvija Juciute
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko str. 24, LT-03225 Vilnius, Lithuania
| | - Arunas Ramanavicius
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko str. 24, LT-03225 Vilnius, Lithuania
| | - Almira Ramanaviciene
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko str. 24, LT-03225 Vilnius, Lithuania
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Ismaeel NT, Lábadi Z, Petrik P, Fried M. Investigation of Electrochromic, Combinatorial TiO 2-SnO 2 Mixed Layers by Spectroscopic Ellipsometry Using Different Optical Models. Materials (Basel) 2023; 16:4204. [PMID: 37374387 DOI: 10.3390/ma16124204] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 04/29/2023] [Revised: 05/26/2023] [Accepted: 05/29/2023] [Indexed: 06/29/2023]
Abstract
We determined the optimal composition of reactive magnetron-sputtered mixed layers of Titanium oxide and Tin oxide (TiO2-SnO2) for electrochromic purposes. We determined and mapped the composition and optical parameters using Spectroscopic Ellipsometry (SE). Ti and Sn targets were put separately from each other, and the Si-wafers on a glass substrate (30 cm × 30 cm) were moved under the two separated targets (Ti and Sn) in a reactive Argon-Oxygen (Ar-O2) gas mixture. Different optical models, such as the Bruggeman Effective Medium Approximation (BEMA) or the 2-Tauc-Lorentz multiple oscillator model (2T-L), were used to obtain the thickness and composition maps of the sample. Scanning Electron Microscopy (SEM) with Energy-Dispersive X-ray Spectroscopy (EDS) has been used to check the SE results. The performance of diverse optical models has been compared. We show that in the case of molecular-level mixed layers, 2T-L is better than EMA. The electrochromic effectiveness (the change of light absorption for the same electric charge) of mixed metal oxides (TiO2-SnO2) that are deposited by reactive sputtering has been mapped too.
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Affiliation(s)
- Noor Taha Ismaeel
- Institute of Technical Physics & Materials Science, Centre for Energy Research, Konkoly-Thege Rd. 29-33, 1121 Budapest, Hungary
- Doctoral School on Materials Sciences and Technologies, Óbuda University, 1034 Budapest, Hungary
- Institute of Laser for Postgraduate Studies, University of Baghdad, Baghdad 10070, Iraq
| | - Zoltán Lábadi
- Institute of Technical Physics & Materials Science, Centre for Energy Research, Konkoly-Thege Rd. 29-33, 1121 Budapest, Hungary
| | - Peter Petrik
- Institute of Technical Physics & Materials Science, Centre for Energy Research, Konkoly-Thege Rd. 29-33, 1121 Budapest, Hungary
- Department of Electrical Engineering, Institute of Physics, Faculty of Science and Technology, University of Debrecen, 4032 Debrecen, Hungary
| | - Miklós Fried
- Institute of Technical Physics & Materials Science, Centre for Energy Research, Konkoly-Thege Rd. 29-33, 1121 Budapest, Hungary
- Institute of Microelectronics and Technology, Óbuda University, Tavaszmezo Str. 17, 1084 Budapest, Hungary
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7
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Kenaz R, Ghosh S, Ramachandran P, Watanabe K, Taniguchi T, Steinberg H, Rapaport R. Thickness Mapping and Layer Number Identification of Exfoliated van der Waals Materials by Fourier Imaging Micro-Ellipsometry. ACS Nano 2023; 17:9188-9196. [PMID: 37155829 DOI: 10.1021/acsnano.2c12773] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/10/2023]
Abstract
As performance of van der Waals heterostructure devices is governed by the nanoscale thicknesses and homogeneity of their constituent mono- to few-layer flakes, accurate mapping of these properties with high lateral resolution becomes imperative. Spectroscopic ellipsometry is a promising optical technique for such atomically thin-film characterization due to its simplicity, noninvasive nature and high accuracy. However, the effective use of standard ellipsometry methods on exfoliated micron-scale flakes is inhibited by their tens-of-microns lateral resolution or slow data acquisition. In this work, we demonstrate a Fourier imaging spectroscopic micro-ellipsometry method with sub-5 μm lateral resolution and three orders-of-magnitude faster data acquisition than similar-resolution ellipsometers. Simultaneous recording of spectroscopic ellipsometry information at multiple angles results in a highly sensitive system, which is used for performing angstrom-level accurate and consistent thickness mapping on exfoliated mono-, bi- and trilayers of graphene, hexagonal boron nitride (hBN) and transition metal dichalcogenide (MoS2, WS2, MoSe2, WSe2) flakes. The system can successfully identify highly transparent monolayer hBN, a challenging proposition for other characterization tools. The optical microscope integrated ellipsometer can also map minute thickness variations over a micron-scale flake, revealing its lateral inhomogeneity. The prospect of adding standard optical elements to augment generic optical imaging and spectroscopy setups with accurate in situ ellipsometric mapping capability presents potential opportunities for investigation of exfoliated 2D materials.
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Affiliation(s)
- Ralfy Kenaz
- Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 9190401, Israel
| | - Saptarshi Ghosh
- Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 9190401, Israel
| | - Pradheesh Ramachandran
- Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 9190401, Israel
| | - Kenji Watanabe
- Research Center for Functional Materials, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan
| | - Takashi Taniguchi
- International Center for Materials Nanoarchitectonics, National Institute for Materials Science, 1-1 Namiki, Tsukuba 305-0044, Japan
| | - Hadar Steinberg
- Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 9190401, Israel
| | - Ronen Rapaport
- Racah Institute of Physics, The Hebrew University of Jerusalem, Jerusalem 9190401, Israel
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8
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Ermolaev GA, Vyslanko IS, Tselin AP, El-Sayed MA, Tatmyshevskiy MK, Slavich AS, Yakubovsky DI, Mironov MS, Mazitov AB, Eghbali A, Panova DA, Romanov RI, Markeev AM, Kruglov IA, Novikov SM, Vyshnevyy AA, Arsenin AV, Volkov VS. Broadband Optical Properties of Bi 2Se 3. Nanomaterials (Basel) 2023; 13:nano13091460. [PMID: 37177004 PMCID: PMC10180482 DOI: 10.3390/nano13091460] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Subscribe] [Scholar Register] [Received: 03/08/2023] [Revised: 04/18/2023] [Accepted: 04/21/2023] [Indexed: 05/15/2023]
Abstract
Materials with high optical constants are of paramount importance for efficient light manipulation in nanophotonics applications. Recent advances in materials science have revealed that van der Waals (vdW) materials have large optical responses owing to strong in-plane covalent bonding and weak out-of-plane vdW interactions. However, the optical constants of vdW materials depend on numerous factors, e.g., synthesis and transfer method. Here, we demonstrate that in a broad spectral range (290-3300 nm) the refractive index n and the extinction coefficient k of Bi2Se3 are almost independent of synthesis technology, with only a ~10% difference in n and k between synthesis approaches, unlike other vdW materials, such as MoS2, which has a ~60% difference between synthesis approaches. As a practical demonstration, we showed, using the examples of biosensors and therapeutic nanoparticles, that this slight difference in optical constants results in reproducible efficiency in Bi2Se3-based photonic devices.
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Affiliation(s)
- Georgy A Ermolaev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Ivan S Vyslanko
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Andrey P Tselin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
- Photonics and Quantum Materials Department, Skolkovo Institute of Science and Technology, 3 Nobel Str., Moscow 143026, Russia
| | - Marwa A El-Sayed
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
- Department of Physics, Faculty of Science, Menoufia University, Shebin El-Koom 32511, Egypt
| | - Mikhail K Tatmyshevskiy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Aleksandr S Slavich
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Dmitry I Yakubovsky
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Mikhail S Mironov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Arslan B Mazitov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Amir Eghbali
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Daria A Panova
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Roman I Romanov
- Department of Solid State Physics and Nanosystems, National Research Nuclear University MEPhI (Moscow Engineering Physics Institute), 31 Kashirskoe Sh., Moscow 115409, Russia
| | - Andrey M Markeev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Ivan A Kruglov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
- Center of Fundamental and Applied Research, Dukhov Research Institute of Automatics (VNIIA), 22 Suschevskaya Str., Moscow 127055, Russia
| | - Sergey M Novikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Andrey A Vyshnevyy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Aleksey V Arsenin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
- Laboratory of Advanced Functional Materials, Yerevan State University, 1 Alek Manukyan Str., Yerevan 0025, Armenia
| | - Valentyn S Volkov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
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Bordovalos A, Subedi B, Chen L, Song Z, Yan Y, Podraza NJ. Implications of Electron Transport Layer and Back Metal Contact Variations in Tin-Lead Perovskite Solar Cells Assessed by Spectroscopic Ellipsometry and External Quantum Efficiency. ACS Appl Mater Interfaces 2023; 15:19730-19740. [PMID: 37022937 DOI: 10.1021/acsami.3c01849] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/19/2023]
Abstract
The structural and optical properties of hybrid organic-inorganic metal halide perovskite solar cells are measured by spectroscopic ellipsometry to reveal an optically distinct interfacial layer among the back contact metal, charge transport, and absorber layers. Understanding how this interfacial layer impacts performance is essential for developing higher performing solar cells. This interfacial layer is modeled by Bruggeman effective medium approximations (EMAs) to contain perovskite, C60, BCP, and metal. External quantum efficiency (EQE) simulations that consider scattering, electronic losses, and the formation of nonparallel interfaces are created with input derived from ellipsometry structural-optical models and compared with experimental EQE to estimate optical losses. This nonplanar interface causes optical losses in short circuit current density (JSC) of up to 1.2 mA cm-2. A study of glass/C60/SnO2/Ag or Cu and glass/C60/BCP/Ag film stacks shows that C60 and BCP mix, but replacing BCP with SnO2 can prevent mixing between the ETLs to prevent contact between C60 and back contact metal and enable the formation of a planar interface between ETLs and back contact metals.
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Affiliation(s)
- Alexander Bordovalos
- Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo, Ohio 43606, United States
| | - Biwas Subedi
- Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo, Ohio 43606, United States
| | - Lei Chen
- Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo, Ohio 43606, United States
| | - Zhaoning Song
- Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo, Ohio 43606, United States
| | - Yanfa Yan
- Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo, Ohio 43606, United States
| | - Nikolas J Podraza
- Department of Physics and Astronomy & Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo, Ohio 43606, United States
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Shen K, Hu X, Li Z, Liao M, Zhuang Z, Ruane S, Wang Z, Li P, Micciulla S, Kasinathan N, Kalonia C, Lu JR. Competitive Adsorption of a Monoclonal Antibody and Nonionic Surfactant at the PDMS/Water Interface. Mol Pharm 2023; 20:2502-2512. [PMID: 37012645 PMCID: PMC10155179 DOI: 10.1021/acs.molpharmaceut.2c01099] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 04/05/2023]
Abstract
Interfacial adsorption of monoclonal antibodies (mAbs) can cause structural deformation and induce undesired aggregation and precipitation. Nonionic surfactants are often added to reduce interfacial adsorption of mAbs which may occur during manufacturing, storage, and/or administration. As mAbs are commonly manufactured into ready-to-use syringes coated with silicone oil to improve lubrication, it is important to understand how an mAb, nonionic surfactant, and silicone oil interact at the oil/water interface. In this work, we have coated a polydimethylsiloxane (PDMS) nanofilm onto an optically flat silicon substrate to facilitate the measurements of adsorption of a model mAb, COE-3, and a commercial nonionic surfactant, polysorbate 80 (PS-80), at the siliconized PDMS/water interface using spectroscopic ellipsometry and neutron reflection. Compared to the uncoated SiO2 surface (mimicking glass), COE-3 adsorption to the PDMS surface was substantially reduced, and the adsorbed layer was characterized by the dense but thin inner layer of 16 Å and an outer diffuse layer of 20 Å, indicating structural deformation. When PS-80 was exposed to the pre-adsorbed COE-3 surface, it removed 60 wt % of COE-3 and formed a co-adsorbed layer with a similar total thickness of 36 Å. When PS-80 was injected first or as a mixture with COE-3, it completely prevented COE-3 adsorption. These findings reveal the hydrophobic nature of the PDMS surface and confirm the inhibitory role of the nonionic surfactant in preventing COE-3 adsorption at the PDMS/water interface.
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Affiliation(s)
- Kangcheng Shen
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Xuzhi Hu
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Zongyi Li
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Mingrui Liao
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Zeyuan Zhuang
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Sean Ruane
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Ziwei Wang
- National Graphene Institute, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
| | - Peixun Li
- STFC ISIS Facility, Rutherford Appleton Laboratory, Didcot OX11 0QX, U.K
| | - Samantha Micciulla
- Institut Laue Langevin, 71 Avenue des Martyrs, CS-20156, Grenoble 38042, France
| | - Narayanan Kasinathan
- Dosage Form Design & Development, BioPharmaceutical Development, BioPharmaceuticals R&D, AstraZeneca, Cambridge CB21 6GH, U.K
| | - Cavan Kalonia
- Dosage Form Design & Development, BioPharmaceutical Development, BioPharmaceuticals R&D, AstraZeneca, Gaithersburg, Maryland 20878, United States
| | - Jian Ren Lu
- Biological Physics Laboratory, Department of Physics and Astronomy, University of Manchester, Oxford Road, Schuster Building, Manchester M13 9PL, U.K
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11
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Sygletou M, Benedetti S, di Bona A, Canepa M, Bisio F, Bellingeri E. In-Operando Optical Spectroscopy of Field-Effect-Gated Al-Doped ZnO. ACS Appl Mater Interfaces 2023; 15:3112-3118. [PMID: 36602943 DOI: 10.1021/acsami.2c16668] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/17/2023]
Abstract
Transparent conductive oxides (TCO) have the unique characteristics of combining optical transparency with high electrical conductivity; such a property makes them uniquely alluring for applications in visible and infrared photonics. One of their most interesting features is the large sensitivity of their optical response to the doping level. We performed the active electrical manipulation of the dielectric properties of aluminum-doped ZnO (AZO), a TCO-based on Earth-abundant elements. We actively tuned the optical and electric performances of AZO films by means of an applied voltage in a parallel-plate capacitor configuration, with SrTiO3 as the dielectric, and monitored the effect of charge injection/depletion by means of in-operando spectroscopic ellipsometry. Calculations of the optical response of the gated system allowed us to extract the spatially resolved variations in the dielectric function of the TCO and infer the injected/depleted charge profile at the interface.
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Affiliation(s)
- Maria Sygletou
- OPTMATLAB, Dipartimento di Fisica, Università di Genova, Via Dodecaneso 33, 16146Genova, Italy
| | | | | | - Maurizio Canepa
- OPTMATLAB, Dipartimento di Fisica, Università di Genova, Via Dodecaneso 33, 16146Genova, Italy
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12
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Zhang HT, He R, Peng L, Yang YT, Sun XJ, Zhang YS, Zheng YX, Liu BJ, Zhang RJ, Wang SY, Li J, Lee YP, Chen LY. Interpretation of Reflection and Colorimetry Characteristics of Indium-Particle Films by Means of Ellipsometric Modeling. Nanomaterials (Basel) 2023; 13:383. [PMID: 36770343 PMCID: PMC9920837 DOI: 10.3390/nano13030383] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 12/30/2022] [Revised: 01/13/2023] [Accepted: 01/16/2023] [Indexed: 06/18/2023]
Abstract
It is of great technological importance in the field of plasmonic color generation to establish and understand the relationship between optical responses and the reflectance of metallic nanoparticles. Previously, a series of indium nanoparticle ensembles were fabricated using electron beam evaporation and inspected using spectroscopic ellipsometry (SE). The multi-oscillator Lorentz-Drude model demonstrated the optical responses of indium nanoparticles with different sizes and size distributions. The reflectance spectra and colorimetry characteristics of indium nanoparticles with unimodal and bimodal size distributions were interpreted based on the SE analysis. The trends of reflectance spectra were explained by the transfer matrix method. The effects of optical constants n and k of indium on the reflectance were demonstrated by mapping the reflectance contour lines on the n-k plane. Using oscillator decomposition, the influence of different electron behaviors in various indium structures on the reflectance spectra was revealed intuitively. The contribution of each oscillator on the colorimetry characteristics, including hue, lightness and saturation, were determined and discussed from the reflectance spectral analysis.
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Affiliation(s)
- Hao-Tian Zhang
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Rong He
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Lei Peng
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Yu-Ting Yang
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Xiao-Jie Sun
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Yu-Shan Zhang
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Yu-Xiang Zheng
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
- High Tech Center for New Materials, Novel Devices and Cutting-Edge Manufacturing, Yiwu Research Institute, Fudan University, Yiwu 322000, China
| | - Bao-Jian Liu
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
- Shanghai Institute of Technical Physics, Chinese Academy of Sciences, Shanghai 200083, China
| | - Rong-Jun Zhang
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Song-You Wang
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Jing Li
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
| | - Young-Pak Lee
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
- Department of Physics, Quantum Photonic Science Research Center and RINS, Hanyang University, Seoul 04763, Republic of Korea
| | - Liang-Yao Chen
- Department of Optical Science and Engineering, School of Information Science and Technology, Fudan University, Shanghai 200433, China
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13
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Gu H, Guo Z, Huang L, Fang M, Liu S. Investigations of Optical Functions and Optical Transitions of 2D Semiconductors by Spectroscopic Ellipsometry and DFT. Nanomaterials (Basel) 2023; 13:196. [PMID: 36616106 PMCID: PMC9823946 DOI: 10.3390/nano13010196] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 12/03/2022] [Revised: 12/28/2022] [Accepted: 12/29/2022] [Indexed: 06/17/2023]
Abstract
Optical functions and transitions are essential for a material to reveal the light-matter interactions and promote its applications. Here, we propose a quantitative strategy to systematically identify the critical point (CP) optical transitions of 2D semiconductors by combining the spectroscopic ellipsometry (SE) and DFT calculations. Optical functions and CPs are determined by SE, and connected to DFT band structure and projected density of states via equal-energy and equal-momentum lines. The combination of SE and DFT provides a powerful tool to investigate the CP optical transitions, including the transition energies and positions in Brillouin zone (BZ), and the involved energy bands and carries. As an example, the single-crystal monolayer WS2 is investigated by the proposed method. Results indicate that six excitonic-type CPs can be quantitatively distinguished in optical function of the monolayer WS2 over the spectral range of 245-1000 nm. These CPs are identified as direct optical transitions from three highest valence bands to three lowest conduction bands at high symmetry points in BZ contributed by electrons in S-3p and W-5d orbitals. Results and discussion on the monolayer WS2 demonstrate the effectiveness and advantages of the proposed method, which is general and can be easily extended to other materials.
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Affiliation(s)
- Honggang Gu
- State Key Laboratory of Digital Manufacturing Equipment and Technology, Huazhong University of Science & Technology, Wuhan 430074, China
- Optics Valley Laboratory, Wuhan 430074, China
| | - Zhengfeng Guo
- State Key Laboratory of Digital Manufacturing Equipment and Technology, Huazhong University of Science & Technology, Wuhan 430074, China
- Innovation Institute, Huazhong University of Science and Technology, Wuhan 430074, China
| | - Liusheng Huang
- Innovation Institute, Huazhong University of Science and Technology, Wuhan 430074, China
| | - Mingsheng Fang
- State Key Laboratory of Digital Manufacturing Equipment and Technology, Huazhong University of Science & Technology, Wuhan 430074, China
| | - Shiyuan Liu
- State Key Laboratory of Digital Manufacturing Equipment and Technology, Huazhong University of Science & Technology, Wuhan 430074, China
- Innovation Institute, Huazhong University of Science and Technology, Wuhan 430074, China
- School of Optical and Electronic Information, Huazhong University of Science and Technology, Wuhan 430074, China
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14
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El-Sayed MA, Tselin AP, Ermolaev GA, Tatmyshevskiy MK, Slavich AS, Yakubovsky DI, Novikov SM, Vyshnevyy AA, Arsenin AV, Volkov VS. Non-Additive Optical Response in Transition Metal Dichalcogenides Heterostructures. Nanomaterials (Basel) 2022; 12:nano12244436. [PMID: 36558289 PMCID: PMC9787828 DOI: 10.3390/nano12244436] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/13/2022] [Revised: 12/04/2022] [Accepted: 12/09/2022] [Indexed: 05/27/2023]
Abstract
Van der Waals (vdW) heterostructures pave the way to achieve the desired material properties for a variety of applications. In this way, new scientific and industrial challenges and fundamental questions arise. One of them is whether vdW materials preserve their original optical response when assembled in a heterostructure. Here, we resolve this issue for four exemplary monolayer heterostructures: MoS2/Gr, MoS2/hBN, WS2/Gr, and WS2/hBN. Through joint Raman, ellipsometry, and reflectance spectroscopies, we discovered that heterostructures alter MoS2 and WS2 optical constants. Furthermore, despite the similarity of MoS2 and WS2 monolayers, their behavior in heterostructures is markedly different. While MoS2 has large changes, particularly above 3 eV, WS2 experiences modest changes in optical constants. We also detected a transformation from dark into bright exciton for MoS2/Gr heterostructure. In summary, our findings provide clear evidence that the optical response of heterostructures is not the sum of optical properties of its constituents.
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Affiliation(s)
- Marwa A. El-Sayed
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
- Department of Physics, Faculty of Science, Menoufia University, Shebin El-Koom 32511, Egypt
| | - Andrey P. Tselin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
- Photonics and Quantum Materials Department, Skolkovo Institute of Science and Technology, 3 Nobel, Moscow 143026, Russia
| | - Georgy A. Ermolaev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Mikhail K. Tatmyshevskiy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Aleksandr S. Slavich
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Dmitry I. Yakubovsky
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Sergey M. Novikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Andrey A. Vyshnevyy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Aleksey V. Arsenin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
| | - Valentyn S. Volkov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, Dolgoprudny 141700, Russia
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15
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Hegedüs N, Balázsi C, Kolonits T, Olasz D, Sáfrán G, Serényi M, Balázsi K. Investigation of the RF Sputtering Process and the Properties of Deposited Silicon Oxynitride Layers under Varying Reactive Gas Conditions. Materials (Basel) 2022; 15:ma15186313. [PMID: 36143625 PMCID: PMC9506354 DOI: 10.3390/ma15186313] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 07/23/2022] [Revised: 08/24/2022] [Accepted: 09/05/2022] [Indexed: 05/14/2023]
Abstract
In a single process run, an amorphous silicon oxynitride layer was grown, which includes the entire transition from oxide to nitride. The variation of the optical properties and the thickness of the layer was characterized by Spectroscopic Ellipsometry (SE) measurements, while the elemental composition was investigated by Energy Dispersive Spectroscopy (EDS). It was revealed that the refractive index of the layer at 632.8 nm is tunable in the 1.48-1.89 range by varying the oxygen partial pressure in the chamber. From the data of the composition of the layer, the typical physical parameters of the process were determined by applying the Berg model valid for reactive sputtering. In our modelling, a new approach was introduced, where the metallic Si target sputtered with a uniform nitrogen and variable oxygen gas flow was considered as an oxygen gas-sputtered SiN target. The layer growth method used in the present work and the revealed correlations between sputtering parameters, layer composition and refractive index, enable both the achievement of the desired optical properties of silicon oxynitride layers and the production of thin films with gradient refractive index for technology applications.
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Affiliation(s)
- Nikolett Hegedüs
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
- Doctoral School of Materials Science and Technologies, Óbuda University, Bécsi str. 96/B, 1030 Budapest, Hungary
- Guardian Orosháza Ltd., Csorvási str. 31, 5900 Oroshaza, Hungary
- Correspondence:
| | - Csaba Balázsi
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
| | - Tamás Kolonits
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
| | - Dániel Olasz
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
- Department of Materials Physics, Eötvös Loránd University, P.O. Box 32, 1518 Budapest, Hungary
| | - György Sáfrán
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
| | - Miklós Serényi
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
| | - Katalin Balázsi
- Institute for Technical Physics and Materials Science, Centre for Energy Research, Konkoly-Thege Miklós str. 29–33, 1121 Budapest, Hungary
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16
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Himcinschi C, Drechsler F, Walch DS, Bhatnagar A, Belik AA, Kortus J. Unexpected Phonon Behaviour in BiFe xCr 1-xO 3, a Material System Different from Its BiFeO 3 and BiCrO 3 Parents. Nanomaterials (Basel) 2022; 12:nano12091607. [PMID: 35564316 PMCID: PMC9100047 DOI: 10.3390/nano12091607] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/31/2022] [Revised: 05/05/2022] [Accepted: 05/05/2022] [Indexed: 02/04/2023]
Abstract
The dielectric function and the bandgap of BiFe0.5Cr0.5O3 thin films were determined from spectroscopic ellipsometry and compared with that of the parent compounds BiFeO3 and BiCrO3. The bandgap value of BiFe0.5Cr0.5O3 is lower than that of BiFeO3 and BiCrO3, due to an optical transition at ~2.27 eV attributed to a charge transfer excitation between the Cr and Fe ions. This optical transition enables new phonon modes which have been investigated using Raman spectroscopy by employing multi-wavelengths excitation. The appearance of a new Raman mode at ~670 cm−1 with a strong intensity dependence on the excitation line and its higher order scattering activation was found for both BiFe0.5Cr0.5O3 thin films and BiFexCr1−xO3 polycrystalline bulk samples. Furthermore, Raman spectroscopy was also used to investigate temperature induced structural phase transitions in BiFe0.3Cr0.7O3.
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Affiliation(s)
- Cameliu Himcinschi
- Institute of Theoretical Physics, TU Bergakademie Freiberg, D-09596 Freiberg, Germany; (F.D.); (J.K.)
- Correspondence:
| | - Felix Drechsler
- Institute of Theoretical Physics, TU Bergakademie Freiberg, D-09596 Freiberg, Germany; (F.D.); (J.K.)
| | - David Sebastian Walch
- Zentrum für Innovationskompetenz SiLi-nano, Martin-Luther-Universität Halle-Wittenberg, D-06120 Halle (Saale), Germany; (D.S.W.); (A.B.)
- Institut für Physik, Martin-Luther-Universität Halle-Wittenberg, D-06120 Halle (Saale), Germany
| | - Akash Bhatnagar
- Zentrum für Innovationskompetenz SiLi-nano, Martin-Luther-Universität Halle-Wittenberg, D-06120 Halle (Saale), Germany; (D.S.W.); (A.B.)
- Institut für Physik, Martin-Luther-Universität Halle-Wittenberg, D-06120 Halle (Saale), Germany
| | - Alexei A. Belik
- International Center for Materials Nanoarchitectonics (WPI-MANA), National Institute for Materials Science (NIMS), Namiki 1-1, Ibaraki, Tsukuba 305-0044, Japan;
| | - Jens Kortus
- Institute of Theoretical Physics, TU Bergakademie Freiberg, D-09596 Freiberg, Germany; (F.D.); (J.K.)
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17
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Tang Y, Chiabrera F, Morata A, Cavallaro A, Liedke MO, Avireddy H, Maller M, Butterling M, Wagner A, Stchakovsky M, Baiutti F, Aguadero A, Tarancón A. Ion Intercalation in Lanthanum Strontium Ferrite for Aqueous Electrochemical Energy Storage Devices. ACS Appl Mater Interfaces 2022; 14:18486-18497. [PMID: 35412787 DOI: 10.1021/acsami.2c01379] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/14/2023]
Abstract
Ion intercalation of perovskite oxides in liquid electrolytes is a very promising method for controlling their functional properties while storing charge, which opens up its potential application in different energy and information technologies. Although the role of defect chemistry in oxygen intercalation in a gaseous environment is well established, the mechanism of ion intercalation in liquid electrolytes at room temperature is poorly understood. In this study, the defect chemistry during ion intercalation of La0.5Sr0.5FeO3-δ thin films in alkaline electrolytes is studied. Oxygen and proton intercalation into the La1-xSrxFeO3-δ perovskite structure is observed at moderate electrochemical potentials (0.5 to -0.4 V), giving rise to a change in the oxidation state of Fe (as a charge compensation mechanism). The variation of the concentration of holes as a function of the intercalation potential is characterized by in situ ellipsometry, and the concentration of electron holes is indirectly quantified for different electrochemical potentials. Finally, a dilute defect chemistry model that describes the variation of defect species during ionic intercalation is developed.
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Affiliation(s)
- Yunqing Tang
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
| | - Francesco Chiabrera
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
- Department of Energy Conversion and Storage, Functional Oxides Group, Technical University of Denmark, Fysikvej 310, 233, 2800 Kongens Lyngby, Denmark
| | - Alex Morata
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
| | - Andrea Cavallaro
- Department of Materials, Imperial College London, London SW7 2AZ, U.K
| | - Maciej O Liedke
- Institute of Radiation Physics, Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
| | - Hemesh Avireddy
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
| | - Mar Maller
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
| | - Maik Butterling
- Institute of Radiation Physics, Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
| | - Andreas Wagner
- Institute of Radiation Physics, Helmholtz-Zentrum Dresden-Rossendorf, 01328 Dresden, Germany
| | - Michel Stchakovsky
- HORIBA Scientific, 14 Boulevard Thomas Gobert, Passage Jobin Yvon, CS 45002-91120 Palaiseau, France
| | - Federico Baiutti
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
- Department of Materials Chemistry, National Institute of Chemistry, Hajdrihova 19, SI-1000 Ljubljana, Slovenia
| | - Ainara Aguadero
- Department of Materials, Imperial College London, London SW7 2AZ, U.K
- Instituto de Ciencia de Materiales de Madrid, ICMM-CSIC, Sor Juana Ines de la Cruz 3, 28049 Madrid, Spain
| | - Albert Tarancón
- Department of Advanced Materials for Energy Applications, Catalonia Institute for Energy Research (IREC), Jardins de les Dones de Negre 1, 08930 Sant Adrià del Besòs, Barcelona, Spain
- ICREA, Passeig Lluís Companys 23, 08010 Barcelona, Spain
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18
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Ho IH, Chang CW, Chen YL, Chang WY, Kuo TJ, Lu YJ, Gwo S, Ahn H. Ultrathin TiN Epitaxial Films as Transparent Conductive Electrodes. ACS Appl Mater Interfaces 2022; 14:16839-16845. [PMID: 35363462 DOI: 10.1021/acsami.2c00508] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/14/2023]
Abstract
Titanium nitride (TiN), a transition-metal compound with tight covalent Ti-N bonding, has a high melting temperature and superior mechanical and chemical stabilities compared to noble metals. With a reduction in thickness, the optical transmittance of TiN films can be drastically increased, and in combination with its excellent electrical conductivity, the ultrathin and continuous TiN film can be considered as an ideal alternative of the metal oxide electrodes. However, the deposition of ultrathin and continuous metallic layer with a smooth surface morphology is a major challenge for typical deposition methods such as thermal evaporation or reactive sputtering. In particular, defects mainly related with oxygen contents and surface scattering can significantly limit the performance of ultrathin TiN films. In this work, ultrathin TiN films with 2-10 nm in thickness are grown by using the nitrogen plasma-assisted molecular-beam epitaxy (MBE) method in an ultrahigh vacuum environment. Excellent surface morphology with a root-mean-square roughness of ≤0.12 nm and a high optical transparency of 75% over the whole visible regime are achieved for ultrathin TiN epitaxial films. The dielectric properties determined by the spectroscopic ellipsometry and the electrical properties measured by the terahertz spectroscopy and the Hall effect method reveal that the percolation thickness of the TiN epitaxial film is less than 2.4 nm and its electrical conductivity is higher than 1.1 × 104 Ω-1 cm-1. These features make MBE-grown ultrathin TiN epitaxial films a good candidate for robust, low cost, and large-area transparent conductive electrodes.
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Affiliation(s)
- I Hong Ho
- Department of Photonics, College of Electrical and Computer Engineering, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
| | - Ching-Wen Chang
- Department of Physics, National Tsing-Hua University, Hsinchu 30013, Taiwan
| | - Yen-Lin Chen
- Department of Photonics, College of Electrical and Computer Engineering, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
| | - Wan-Yu Chang
- Department of Photonics, College of Electrical and Computer Engineering, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
| | - Ting-Jui Kuo
- Department of Photonics, College of Electrical and Computer Engineering, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
| | - Yu-Jung Lu
- Research Center for Applied Sciences, Academia Sinica, Taipei 11529, Taiwan
| | - Shangjr Gwo
- Department of Physics, National Tsing-Hua University, Hsinchu 30013, Taiwan
| | - Hyeyoung Ahn
- Department of Photonics, College of Electrical and Computer Engineering, National Yang Ming Chiao Tung University, Hsinchu 30010, Taiwan
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Plikusiene I, Maciulis V, Ramanavicius A, Ramanaviciene A. Spectroscopic Ellipsometry and Quartz Crystal Microbalance with Dissipation for the Assessment of Polymer Layers and for the Application in Biosensing. Polymers (Basel) 2022; 14:polym14051056. [PMID: 35267879 PMCID: PMC8915094 DOI: 10.3390/polym14051056] [Citation(s) in RCA: 4] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 02/05/2022] [Revised: 02/24/2022] [Accepted: 02/28/2022] [Indexed: 01/07/2023] Open
Abstract
Polymers represent materials that are applied in almost all areas of modern life, therefore, the characterization of polymer layers using different methods is of great importance. In this review, the main attention is dedicated to the non-invasive and label-free optical and acoustic methods, namely spectroscopic ellipsometry (SE) and quartz crystal microbalance with dissipation (QCM-D). The specific advantages of these techniques applied for in situ monitoring of polymer layer formation and characterization, biomolecule immobilization, and registration of specific interactions were summarized and discussed. In addition, the exceptional benefits and future perspectives of combined spectroscopic ellipsometry and QCM-D (SE/QCM-D) in one measurement are overviewed. Recent advances in the discussed area allow us to conclude that especially significant breakthroughs are foreseen in the complementary application of both QCM-D and SE techniques for the investigation of polymer structure and assessment of the interaction between biomolecules such as antigens and antibodies, receptors and ligands, and complementary DNA strands.
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Affiliation(s)
- Ieva Plikusiene
- Nanotechnas–Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko Str. 24, LT-03225 Vilnius, Lithuania; (V.M.); (A.R.)
- State Research Institute Centre for Physical Sciences and Technology, Sauletekio Ave. 3, LT-10257 Vilnius, Lithuania
- Correspondence: (I.P.); (A.R.)
| | - Vincentas Maciulis
- Nanotechnas–Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko Str. 24, LT-03225 Vilnius, Lithuania; (V.M.); (A.R.)
- State Research Institute Centre for Physical Sciences and Technology, Sauletekio Ave. 3, LT-10257 Vilnius, Lithuania
| | - Arunas Ramanavicius
- Nanotechnas–Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko Str. 24, LT-03225 Vilnius, Lithuania; (V.M.); (A.R.)
- State Research Institute Centre for Physical Sciences and Technology, Sauletekio Ave. 3, LT-10257 Vilnius, Lithuania
| | - Almira Ramanaviciene
- Nanotechnas–Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko Str. 24, LT-03225 Vilnius, Lithuania; (V.M.); (A.R.)
- Department of Immunology, State Research Institute Centre for Innovative Medicine, Santariskiu g. 5, LT-08406 Vilnius, Lithuania
- Correspondence: (I.P.); (A.R.)
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20
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Ermolaev GA, Yakubovsky DI, El-Sayed MA, Tatmyshevskiy MK, Mazitov AB, Popkova AA, Antropov IM, Bessonov VO, Slavich AS, Tselikov GI, Kruglov IA, Novikov SM, Vyshnevyy AA, Fedyanin AA, Arsenin AV, Volkov VS. Broadband Optical Constants and Nonlinear Properties of SnS 2 and SnSe 2. Nanomaterials (Basel) 2021; 12:nano12010141. [PMID: 35010091 PMCID: PMC8746438 DOI: 10.3390/nano12010141] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/05/2021] [Revised: 12/24/2021] [Accepted: 12/28/2021] [Indexed: 11/16/2022]
Abstract
SnS2 and SnSe2 have recently been shown to have a wide range of applications in photonic and optoelectronic devices. However, because of incomplete knowledge about their optical characteristics, the use of SnS2 and SnSe2 in optical engineering remains challenging. Here, we addressed this problem by establishing SnS2 and SnSe2 linear and nonlinear optical properties in the broad (300-3300 nm) spectral range. Coupled with the first-principle calculations, our experimental study unveiled the full dielectric tensor of SnS2 and SnSe2. Furthermore, we established that SnS2 is a promising material for visible high refractive index nanophotonics. Meanwhile, SnSe2 demonstrates a stronger nonlinear response compared with SnS2. Our results create a solid ground for current and next-generation SnS2- and SnSe2-based devices.
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Affiliation(s)
- Georgy A. Ermolaev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Dmitry I. Yakubovsky
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Marwa A. El-Sayed
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- Department of Physics, Faculty of Science, Menoufia University, Shebin El-Koom 32511, Egypt
| | - Mikhail K. Tatmyshevskiy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Arslan B. Mazitov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- Dukhov Research Institute of Automatics (VNIIA), 22 Suschevskaya St., 127055 Moscow, Russia
| | - Anna A. Popkova
- Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia; (A.A.P.); (I.M.A.); (V.O.B.); (A.A.F.)
| | - Ilya M. Antropov
- Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia; (A.A.P.); (I.M.A.); (V.O.B.); (A.A.F.)
| | - Vladimir O. Bessonov
- Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia; (A.A.P.); (I.M.A.); (V.O.B.); (A.A.F.)
| | - Aleksandr S. Slavich
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Gleb I. Tselikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Ivan A. Kruglov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- Dukhov Research Institute of Automatics (VNIIA), 22 Suschevskaya St., 127055 Moscow, Russia
| | - Sergey M. Novikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Andrey A. Vyshnevyy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Andrey A. Fedyanin
- Faculty of Physics, Lomonosov Moscow State University, 119991 Moscow, Russia; (A.A.P.); (I.M.A.); (V.O.B.); (A.A.F.)
| | - Aleksey V. Arsenin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Valentyn S. Volkov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (D.I.Y.); (M.A.E.-S.); (M.K.T.); (A.B.M.); (A.S.S.); (G.I.T.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- Correspondence: or ; Tel.: +7-926-735-93-98
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Plikusienė I, Bužavaitė-Vertelienė E, Mačiulis V, Valavičius A, Ramanavičienė A, Balevičius Z. Application of Tamm Plasmon Polaritons and Cavity Modes for Biosensing in the Combined Spectroscopic Ellipsometry and Quartz Crystal Microbalance Method. Biosensors (Basel) 2021; 11:bios11120501. [PMID: 34940258 PMCID: PMC8699563 DOI: 10.3390/bios11120501] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Received: 11/15/2021] [Revised: 11/30/2021] [Accepted: 12/04/2021] [Indexed: 06/01/2023]
Abstract
Low-cost 1D plasmonic photonic structures supporting Tamm plasmon polaritons and cavity modes were employed for optical signal enhancement, modifying the commercially available quartz crystal microbalance with dissipation (QCM-D) sensor chip in a combinatorial spectroscopic ellipsometry and quartz microbalance method. The Tamm plasmon optical state and cavity mode (CM) for the modified mQCM-D sample obtained sensitivity of ellipsometric parameters to RIU of ΨTPP = 126.78 RIU-1 and ΔTPP = 325 RIU-1, and ΨCM = 264 RIU-1 and ΔCM = 645 RIU-1, respectively. This study shows that Tamm plasmon and cavity modes exhibit about 23 and 49 times better performance of ellipsometric parameters, respectively, for refractive index sensing than standard spectroscopic ellipsometry on a QCM-D sensor chip. It should be noted that for the optical biosensing signal readout, the sensitivity of Tamm plasmon polaritons and cavity modes are comparable with and higher than the standard QCM-D sensor chip. The different origin of Tamm plasmon polaritons (TPP) and cavity mode (CM) provides further advances and can determine whether the surface (TPP) or bulk process (CM) is dominating. The dispersion relation feature of TPP, namely the direct excitation without an additional coupler, allows the possibility to enhance the optical signal on the sensing surface. To the best of our knowledge, this is the first study and application of the TPP and CM in the combinatorial SE-QCM-D method for the enhanced readout of ellipsometric parameters.
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Affiliation(s)
- Ieva Plikusienė
- State Research Institute Center for Physical Sciences and Technology, Saulėtekio av. 3, 10257 Vilnius, Lithuania; (I.P.); (E.B.-V.); (V.M.); (A.V.); (A.R.)
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko Str. 24, 03225 Vilnius, Lithuania
| | - Ernesta Bužavaitė-Vertelienė
- State Research Institute Center for Physical Sciences and Technology, Saulėtekio av. 3, 10257 Vilnius, Lithuania; (I.P.); (E.B.-V.); (V.M.); (A.V.); (A.R.)
| | - Vincentas Mačiulis
- State Research Institute Center for Physical Sciences and Technology, Saulėtekio av. 3, 10257 Vilnius, Lithuania; (I.P.); (E.B.-V.); (V.M.); (A.V.); (A.R.)
| | - Audrius Valavičius
- State Research Institute Center for Physical Sciences and Technology, Saulėtekio av. 3, 10257 Vilnius, Lithuania; (I.P.); (E.B.-V.); (V.M.); (A.V.); (A.R.)
| | - Almira Ramanavičienė
- State Research Institute Center for Physical Sciences and Technology, Saulėtekio av. 3, 10257 Vilnius, Lithuania; (I.P.); (E.B.-V.); (V.M.); (A.V.); (A.R.)
- NanoTechnas—Center of Nanotechnology and Materials Science, Faculty of Chemistry and Geosciences, Vilnius University, Naugarduko Str. 24, 03225 Vilnius, Lithuania
| | - Zigmas Balevičius
- State Research Institute Center for Physical Sciences and Technology, Saulėtekio av. 3, 10257 Vilnius, Lithuania; (I.P.); (E.B.-V.); (V.M.); (A.V.); (A.R.)
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22
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Ermolaev GA, Voronin KV, Tatmyshevskiy MK, Mazitov AB, Slavich AS, Yakubovsky DI, Tselin AP, Mironov MS, Romanov RI, Markeev AM, Kruglov IA, Novikov SM, Vyshnevyy AA, Arsenin AV, Volkov VS. Broadband Optical Properties of Atomically Thin PtS 2 and PtSe 2. Nanomaterials (Basel) 2021; 11:3269. [PMID: 34947618 PMCID: PMC8708229 DOI: 10.3390/nano11123269] [Citation(s) in RCA: 6] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 11/04/2021] [Revised: 11/21/2021] [Accepted: 11/29/2021] [Indexed: 01/31/2023]
Abstract
Noble transition metal dichalcogenides (TMDCs) such as PtS2 and PtSe2 show significant potential in a wide range of optoelectronic and photonic applications. Noble TMDCs, unlike standard TMDCs such as MoS2 and WS2, operate in the ultrawide spectral range from ultraviolet to mid-infrared wavelengths; however, their properties remain largely unexplored. Here, we measured the broadband (245-3300 nm) optical constants of ultrathin PtS2 and PtSe2 films to eliminate this gap and provide a foundation for optoelectronic device simulation. We discovered their broadband absorption and high refractive index both theoretically and experimentally. Based on first-principle calculations, we also predicted their giant out-of-plane optical anisotropy for monocrystals. As a practical illustration of the obtained optical properties, we demonstrated surface plasmon resonance biosensors with PtS2 or PtSe2 functional layers, which dramatically improves sensor sensitivity by 60 and 30%, respectively.
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Affiliation(s)
- Georgy A. Ermolaev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Kirill V. Voronin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Mikhail K. Tatmyshevskiy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Arslan B. Mazitov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- Dukhov Research Institute of Automatics (VNIIA), 22 Suschevskaya St., 127055 Moscow, Russia
| | - Aleksandr S. Slavich
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Dmitry I. Yakubovsky
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Andrey P. Tselin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Mikhail S. Mironov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Roman I. Romanov
- Moscow Engineering Physics Institute, National Research Nuclear University MEPhI, 31 Kashirskoe Sh., 115409 Moscow, Russia;
| | - Andrey M. Markeev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Ivan A. Kruglov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- Dukhov Research Institute of Automatics (VNIIA), 22 Suschevskaya St., 127055 Moscow, Russia
| | - Sergey M. Novikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Andrey A. Vyshnevyy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
| | - Aleksey V. Arsenin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- GrapheneTek, Skolkovo Innovation Center, 143026 Moscow, Russia
| | - Valentyn S. Volkov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (K.V.V.); (M.K.T.); (A.B.M.); (A.S.S.); (D.I.Y.); (A.P.T.); (M.S.M.); (A.M.M.); (I.A.K.); (S.M.N.); (A.A.V.); (A.V.A.)
- GrapheneTek, Skolkovo Innovation Center, 143026 Moscow, Russia
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Takita S, Nabok A, Lishchuk A, Smith D. Optimization of Apta-Sensing Platform for Detection of Prostate Cancer Marker PCA3. Int J Mol Sci 2021; 22:ijms222312701. [PMID: 34884504 PMCID: PMC8657731 DOI: 10.3390/ijms222312701] [Citation(s) in RCA: 3] [Impact Index Per Article: 1.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 11/01/2021] [Revised: 11/17/2021] [Accepted: 11/21/2021] [Indexed: 02/07/2023] Open
Abstract
This work is a continuation of our research into the development of simple, reliable, and cost-effective methods for the early diagnosis of prostate cancer (PCa). The proposed method is based on the electrochemical detection of the PCA3 biomarker of PCa (long non-coded RNA transcript expressed in urine) using a specific aptamer labeled with a redox group (methylene blue). The electrochemical measurements (cyclic voltammograms) obtained from electrodes functionalized with the aptamer were complemented in this work by another biosensing technique: total internal reflection ellipsometry (TIRE). In addition to proving the concept of the detection of PCA3 in low concentrations down to 90 pM, this study improved our understanding of the processes by which PCA3 binds to its specific aptamer. The high specificity of the binding of PCA3 to the aptamer was assessed by studying the binding kinetics, which yielded an affinity constant (KD) of 2.58 × 10−9 M. Additional XPS measurements confirmed the strong covalent binding of aptamers to gold and showed spectral features associated with PCA3 to aptamer binding.
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Affiliation(s)
- Sarra Takita
- Materials and Engineering Research Institute, Sheffield Hallam University, Sheffield S1 1WB, UK;
| | - Alexei Nabok
- Materials and Engineering Research Institute, Sheffield Hallam University, Sheffield S1 1WB, UK;
- Correspondence: ; Tel.: +44-114-2256905
| | - Anna Lishchuk
- Department of Chemistry, The University of Sheffield, Sheffield S3 7HF, UK;
| | - David Smith
- Biomolecular Research Centre, Sheffield Hallam University, Sheffield S1 1WB, UK;
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Kaya H, Ngo D, Hahn SH, Li M, He H, Yedikardeş B, Sökmen İ, Pester CW, Podraza NJ, Gin S, Kim SH. Estimating Internal Stress of an Alteration Layer Formed on Corroded Boroaluminosilicate Glass through Spectroscopic Ellipsometry Analysis. ACS Appl Mater Interfaces 2021; 13:50470-50480. [PMID: 34643085 DOI: 10.1021/acsami.1c10134] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/13/2023]
Abstract
Aqueous corrosion of glass may result in the formation of an alteration layer in the glass surface of which chemical composition and network structure are different from those of the bulk glass. Since corrosion occurs far below the glass-transition temperature, the alteration layer cannot fully relax to the new structure with the lowest possible energy. Molecular dynamics simulations suggested that such a network will contain highly strained chemical bonds, which can be manifested as a stress in the alteration layer. Common techniques to measure stress in thin films or surface layers were found inadequate for thick monolithic glass samples corroded in water. Here, we explored the use of spectroscopic ellipsometry to test the presence of internal stress in the alteration layer formed by aqueous corrosion of glass. A procedure for analyses of spectroscopic ellipsometry data to determine birefringence in the alteration layer was developed. Findings with the established fitting procedure suggested that a stress builds up in the corroded surface layer of a boroaluminosilicate glass if there is a change in relative humidity, pH, or electrolyte concentration of the environment to which the glass surface is exposed. A similar process may occur in other types of glass, and it may affect the surface properties of corroded glass objects.
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Affiliation(s)
- Huseyin Kaya
- Department of Materials Science and Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
| | - Dien Ngo
- Department of Chemical Engineering and Materials Research Institute, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
| | - Seung Ho Hahn
- Department of Mechanical Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
| | - Mingxiao Li
- Department of Chemical Engineering and Materials Research Institute, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
| | - Hongtu He
- Department of Chemical Engineering and Materials Research Institute, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
- Key Laboratory of Testing Technology for Manufacturing Process, Ministry of Education, Southwest University of Science and Technology, Mianyang, Sichuan 621010, China
| | - Beyza Yedikardeş
- Şişecam Science and Technology Center, Şişecam Str., No:2 Çayırova, Kocaeli 41400, Turkey
| | - İlkay Sökmen
- Şişecam Science and Technology Center, Şişecam Str., No:2 Çayırova, Kocaeli 41400, Turkey
| | - Christian W Pester
- Department of Materials Science and Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
- Department of Chemical Engineering and Materials Research Institute, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
- Department of Chemistry, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
| | - Nikolas J Podraza
- Department of Physics and Astronomy, The University of Toledo, Toledo, Ohio 43606, United States
- Wright Center for Photovoltaics Innovation and Commercialization, The University of Toledo, Toledo, Ohio 43606, United States
| | - Stephane Gin
- CEA, DES, ISEC, DE2D, University of Montpellier, Marcoule, Bagnols sur Cèze F-30207, France
| | - Seong H Kim
- Department of Materials Science and Engineering, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
- Department of Chemical Engineering and Materials Research Institute, The Pennsylvania State University, University Park, Pennsylvania 16802, United States
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Toma O, Antohe VA, Panaitescu AM, Iftimie S, Răduţă AM, Radu A, Ion L, Antohe Ş. Effect of RF Power on the Physical Properties of Sputtered ZnSe Nanostructured Thin Films for Photovoltaic Applications. Nanomaterials (Basel) 2021; 11:nano11112841. [PMID: 34835604 PMCID: PMC8624428 DOI: 10.3390/nano11112841] [Citation(s) in RCA: 7] [Impact Index Per Article: 2.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 07/02/2021] [Revised: 10/21/2021] [Accepted: 10/22/2021] [Indexed: 01/16/2023]
Abstract
Zinc selenide (ZnSe) thin films were deposited by RF magnetron sputtering in specific conditions, onto optical glass substrates, at different RF plasma power. The prepared ZnSe layers were afterwards subjected to a series of structural, morphological, optical and electrical characterizations. The obtained results pointed out the optimal sputtering conditions to obtain ZnSe films of excellent quality, especially in terms of better optical properties, lower superficial roughness, reduced micro-strain and a band gap value closer to the one reported for the ZnSe bulk semiconducting material. Electrical characterization were afterwards carried out by measuring the current–voltage (I-V) characteristics at room temperature, of prepared “sandwich”-like Au/ZnSe/Au structures. The analysis of I-V characteristics have shown that at low injection levels there is an Ohmic conduction, followed at high injection levels, after a well-defined transition voltage, by a Space Charge Limited Current (SCLC) in the presence of an exponential trap distribution in the band gap of the ZnSe thin films. The results obtained from all the characterization techniques presented, demonstrated thus the potential of ZnSe thin films sputtered under optimized RF plasma conditions, to be used as alternative environmentally-friendly Cd-free window layers within photovoltaic cells manufacturing.
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Affiliation(s)
- Ovidiu Toma
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
| | - Vlad-Andrei Antohe
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
- Institute of Condensed Matter and Nanosciences (IMCN), Université catholique de Louvain (UCLouvain), Place Croix du Sud 1, B-1348 Louvain-la-Neuve, Belgium
| | - Ana-Maria Panaitescu
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
| | - Sorina Iftimie
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
| | - Ana-Maria Răduţă
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
| | - Adrian Radu
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
| | - Lucian Ion
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
| | - Ştefan Antohe
- Faculty of Physics, R&D Center for Materials and Electronic & Optoelectronic Devices (MDEO), University of Bucharest, Atomiştilor Street 405, 077125 Măgurele, Romania; (O.T.); (V.-A.A.); (A.-M.P.); (S.I.); (A.-M.R.); (A.R.); (L.I.)
- Academy of Romanian Scientists, Splaiul Independenţei 54, 050094 Bucharest, Romania
- Correspondence:
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Alaani MAR, Koirala P, Phillips AB, Liyanage GK, Awni RA, Sapkota DR, Ramanujam B, Heben MJ, O’Leary SK, Podraza NJ, Collins RW. Optical Properties of Magnesium-Zinc Oxide for Thin Film Photovoltaics. Materials (Basel) 2021; 14:ma14195649. [PMID: 34640041 PMCID: PMC8510442 DOI: 10.3390/ma14195649] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 08/07/2021] [Revised: 09/20/2021] [Accepted: 09/23/2021] [Indexed: 12/28/2022]
Abstract
Motivated by their utility in CdTe-based thin film photovoltaics (PV) devices, an investigation of thin films of the magnesium-zinc oxide (MgxZn1−xO or MZO) alloy system was undertaken applying spectroscopic ellipsometry (SE). Dominant wurtzite phase MZO thin films with Mg contents in the range 0 ≤ x ≤ 0.42 were deposited on room temperature soda lime glass (SLG) substrates by magnetron co-sputtering of MgO and ZnO targets followed by annealing. The complex dielectric functions ε of these films were determined and parameterized over the photon energy range from 0.73 to 6.5 eV using an analytical model consisting of two critical point (CP) oscillators. The CP parameters in this model are expressed as polynomial functions of the best fitting lowest CP energy or bandgap E0 = Eg, which in turn is a quadratic function of x. As functions of x, both the lowest energy CP broadening and the Urbach parameter show minima for x ~ 0.3, which corresponds to a bandgap of 3.65 eV. As a result, it is concluded that for this composition and bandgap, the MZO exhibits either a minimum concentration of defects in the bulk of the crystallites or a maximum in the grain size, an observation consistent with measured X-ray diffraction line broadenings. The parametric expression for ε developed here is expected to be useful in future mapping and through-the-glass SE analyses of partial and complete PV device structures incorporating MZO.
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Affiliation(s)
- Mohammed A. Razooqi Alaani
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
- Correspondence: (M.A.R.A.); (N.J.P.); (R.W.C.)
| | - Prakash Koirala
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Adam B. Phillips
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Geethika K. Liyanage
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Rasha A. Awni
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Dhurba R. Sapkota
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Balaji Ramanujam
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Michael J. Heben
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
| | - Stephen K. O’Leary
- School of Engineering, The University of British Columbia Okanagan, 3333 University Way, Kelowna, BC V1V 1V7, Canada;
| | - Nikolas J. Podraza
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
- Correspondence: (M.A.R.A.); (N.J.P.); (R.W.C.)
| | - Robert W. Collins
- Wright Center for Photovoltaics Innovation & Commercialization, Department of Physics & Astronomy, University of Toledo, Toledo, OH 43606, USA; (P.K.); (A.B.P.); (G.K.L.); (R.A.A.); (D.R.S.); (B.R.); (M.J.H.)
- Correspondence: (M.A.R.A.); (N.J.P.); (R.W.C.)
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Liu CP, Li ZH, Egbo KO, Kwok CK, Lv XH, Ho CY, Wang Y, Yu KM. Effects of oxygen flow ratio and thermal annealing on defect evolution of aluminum doped zinc oxide thin films by reactive DC magnetron sputtering. J Phys Condens Matter 2021; 33:465703. [PMID: 34412043 DOI: 10.1088/1361-648x/ac1f50] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/06/2021] [Accepted: 08/19/2021] [Indexed: 06/13/2023]
Abstract
Al doped ZnO (AZO) is a promising transparent conducting oxide to replace the expensive Sn doped In2O3(ITO). Understanding the formation and evolution of defects in AZO is essential for its further improvement. Here, we synthesize transparent conducting AZO thin films by reactive DC magnetron sputtering. The effects of oxygen flow ratio as well as the rapid thermal annealing (RTA) in different conditions on their structural and optoelectrical properties were investigated by a variety of analytical techniques. We find that AZO thin films grown in O-rich conditions exhibit inferior optoelectrical performance as compared with those grown in Zn-rich conditions, possibly due to the formation of excessive native acceptor defects and/or secondary phases (e.g. Al2O3). Temperature-dependent Hall measurements indicate that mobilities of these highly degenerate AZO films withN> 1020 cm-3are primarily limited by ionized and neutral impurities, while films with relatively lowN∼ 1019 cm-3exhibit a temperature-activated mobility owing to the grain-barrier scattering. AsNincreases, the optical band gap of AZO thin film increases as a result of Burstein-Moss shift and band gap narrowing. RTA treatments under appropriate conditions (i.e. at 500 °C for 60 s in Ar) can further improve the electrical properties of AZO thin film, with low resistivity of ∼6.2 × 10-4Ω cm achieved, while RTA at high temperature with longer time can lead to the formation of substantial sub-gap defect states and thus lowers the electron mobility. X-ray photoelectron spectroscopy provides further evidence on the variation of Al (Zn) content at the surface of AZO thin films with different processing conditions.
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Affiliation(s)
- Chao Ping Liu
- Research Center for Advanced Optics and Photoelectronics, Department of Physics, College of Science, Shantou University, Shantou, Guangdong 515063, People's Republic of China
| | - Zhan Hua Li
- Research Center for Advanced Optics and Photoelectronics, Department of Physics, College of Science, Shantou University, Shantou, Guangdong 515063, People's Republic of China
| | - Kingsley O Egbo
- Department of Physics, City University of Hong Kong, 83 Tat Chee Ave., Kowloon, Hong Kong Special Administrative Region of China
| | - Cheuk Kai Kwok
- Department of Physics, City University of Hong Kong, 83 Tat Chee Ave., Kowloon, Hong Kong Special Administrative Region of China
| | - Xiao Hu Lv
- Research Center for Advanced Optics and Photoelectronics, Department of Physics, College of Science, Shantou University, Shantou, Guangdong 515063, People's Republic of China
| | - Chun Yuen Ho
- Department of Physics, City University of Hong Kong, 83 Tat Chee Ave., Kowloon, Hong Kong Special Administrative Region of China
| | - Ying Wang
- Department of Physics, City University of Hong Kong, 83 Tat Chee Ave., Kowloon, Hong Kong Special Administrative Region of China
| | - Kin Man Yu
- Department of Physics, City University of Hong Kong, 83 Tat Chee Ave., Kowloon, Hong Kong Special Administrative Region of China
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Buchkov K, Todorov R, Terziyska P, Gospodinov M, Strijkova V, Dimitrov D, Marinova V. Anisotropic Optical Response of WTe 2 Single Crystals Studied by Ellipsometric Analysis. Nanomaterials (Basel) 2021; 11:2262. [PMID: 34578578 DOI: 10.3390/nano11092262] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 06/17/2021] [Revised: 08/19/2021] [Accepted: 08/27/2021] [Indexed: 11/23/2022]
Abstract
In this paper we report the crystal growth conditions and optical anisotropy properties of Tungsten ditelluride (WTe2) single crystals. The chemical vapor transport (CVT) method was used for the synthesis of large WTe2 crystals with high crystallinity and surface quality. These were structurally and morphologically characterized by means of X-ray diffraction, optical profilometry and Raman spectroscopy. Through spectroscopic ellipsometry analysis, based on the Tauc–Lorentz model, we identified a high refractive index value (~4) and distinct tri-axial anisotropic behavior of the optical constants, which opens prospects for surface plasmon activity, revealed by the dielectric function. The anisotropic physical nature of WTe2 shows practical potential for low-loss light modulation at the 2D nanoscale level.
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Simandan ID, Sava F, Buruiana AT, Galca AC, Becherescu N, Burducea I, Mihai C, Velea A. Influence of Deposition Method on the Structural and Optical Properties of Ge 2Sb 2Te 5. Materials (Basel) 2021; 14:3663. [PMID: 34209141 PMCID: PMC8269865 DOI: 10.3390/ma14133663] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 06/11/2021] [Revised: 06/25/2021] [Accepted: 06/27/2021] [Indexed: 11/16/2022]
Abstract
Ge2Sb2Te5 (GST-225) is a chalcogenide material with applications in nonvolatile memories. However, chalcogenide material properties are dependent on the deposition technique. GST-225 thin films were prepared using three deposition methods: magnetron sputtering (MS), pulsed laser deposition (PLD) and a deposition technique that combines MS and PLD, namely MSPLD. In the MSPLD technique, the same bulk target is used for sputtering but also for PLD at the same time. The structural and optical properties of the as-deposited and annealed thin films were characterized by Rutherford backscattering spectrometry, X-ray reflectometry, X-ray diffraction, Raman spectroscopy and spectroscopic ellipsometry. MS has the advantage of easily leading to fully amorphous films and to a single crystalline phase after annealing. MS also produces the highest optical contrast between the as-deposited and annealed films. PLD leads to the best stoichiometric transfer, whereas the annealed MSPLD films have the highest mass density. All the as-deposited films obtained with the three methods have a similar optical bandgap of approximately 0.7 eV, which decreases after annealing, mostly in the case of the MS sample. This study reveals that the properties of GST-225 are significantly influenced by the deposition technique, and the proper method should be selected when targeting a specific application. In particular, for electrical and optical phase change memories, MS is the best suited deposition method.
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Affiliation(s)
- Iosif-Daniel Simandan
- National Institute of Materials Physics, Atomistilor 405A, 077125 Magurele, Romania; (I.-D.S.); (F.S.); (A.-T.B.); (A.-C.G.); (C.M.)
| | - Florinel Sava
- National Institute of Materials Physics, Atomistilor 405A, 077125 Magurele, Romania; (I.-D.S.); (F.S.); (A.-T.B.); (A.-C.G.); (C.M.)
| | - Angel-Theodor Buruiana
- National Institute of Materials Physics, Atomistilor 405A, 077125 Magurele, Romania; (I.-D.S.); (F.S.); (A.-T.B.); (A.-C.G.); (C.M.)
| | - Aurelian-Catalin Galca
- National Institute of Materials Physics, Atomistilor 405A, 077125 Magurele, Romania; (I.-D.S.); (F.S.); (A.-T.B.); (A.-C.G.); (C.M.)
| | | | - Ion Burducea
- Horia Hulubei National Institute of Physics & Nuclear Engineering, 077125 Magurele, Romania;
| | - Claudia Mihai
- National Institute of Materials Physics, Atomistilor 405A, 077125 Magurele, Romania; (I.-D.S.); (F.S.); (A.-T.B.); (A.-C.G.); (C.M.)
| | - Alin Velea
- National Institute of Materials Physics, Atomistilor 405A, 077125 Magurele, Romania; (I.-D.S.); (F.S.); (A.-T.B.); (A.-C.G.); (C.M.)
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Katzenmeier L, Carstensen L, Schaper SJ, Müller-Buschbaum P, Bandarenka AS. Characterization and Quantification of Depletion and Accumulation Layers in Solid-State Li + -Conducting Electrolytes Using In Situ Spectroscopic Ellipsometry. Adv Mater 2021; 33:e2100585. [PMID: 33955614 DOI: 10.1002/adma.202100585] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 01/22/2021] [Revised: 03/08/2021] [Indexed: 06/12/2023]
Abstract
The future of mobility depends on the development of next-generation battery technologies, such as all-solid-state batteries. As the ionic conductivity of solid Li+ -conductors can, in some cases, approach that of liquid electrolytes, a significant remaining barrier faced by solid-state electrolytes (SSEs) is the interface formed at the anode and cathode materials, with chemical instability and physical resistances arising. The physical properties of space charge layers (SCLs), a widely discussed phenomenon in SSEs, are still unclear. In this work, spectroscopic ellipsometry is used to characterize the accumulation and depletion layers. An optical model is developed to quantify their thicknesses and corresponding concentration changes. It is shown that the Li+ -depleted layer (≈190 nm at 1 V) is thinner than the accumulation layer (≈320 nm at 1 V) in a glassy lithium-ion-conducting glass ceramic electrolyte (a trademark of Ohara Corporation). The in situ approach combining electrochemistry and optics resolves the ambiguities around SCL formation. It opens up a wide field of optical measurements on SSEs, allowing various experimental studies in the future.
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Affiliation(s)
- Leon Katzenmeier
- Physics of Energy Conversion and Storage Department of Physics, Technische Universität München, James-Franck-Str. 1, Garching, 85748, Germany
- Bayerisches Zentrum für Angewandte Energieforschung, Magdalene-Schoch-Str. 3, Würzburg, 97074, Germany
| | - Leif Carstensen
- Physics of Energy Conversion and Storage Department of Physics, Technische Universität München, James-Franck-Str. 1, Garching, 85748, Germany
| | - Simon J Schaper
- Lehrstuhl für Funktionelle Materielien Physik-Department, Technische Universität München, James-Franck-Str. 1, Garching, 85748, Germany
| | - Peter Müller-Buschbaum
- Lehrstuhl für Funktionelle Materielien Physik-Department, Technische Universität München, James-Franck-Str. 1, Garching, 85748, Germany
- Heinz Maier-Leibnitz Zentrum (MLZ), Technische Universität München, Lichtenbergstr. 1, Garching, 85748, Germany
| | - Aliaksandr S Bandarenka
- Physics of Energy Conversion and Storage Department of Physics, Technische Universität München, James-Franck-Str. 1, Garching, 85748, Germany
- e-conversion Excellence Cluster, Lichtenbergstr. 4, Garching, 85748, Germany
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31
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Ermolaev GA, El-Sayed MA, Yakubovsky DI, Voronin KV, Romanov RI, Tatmyshevskiy MK, Doroshina NV, Nemtsov AB, Voronov AA, Novikov SM, Markeev AM, Tselikov GI, Vyshnevyy AA, Arsenin AV, Volkov VS. Optical Constants and Structural Properties of Epitaxial MoS 2 Monolayers. Nanomaterials (Basel) 2021; 11:nano11061411. [PMID: 34071775 PMCID: PMC8227853 DOI: 10.3390/nano11061411] [Citation(s) in RCA: 4] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 05/03/2021] [Revised: 05/23/2021] [Accepted: 05/25/2021] [Indexed: 11/18/2022]
Abstract
Two-dimensional layers of transition-metal dichalcogenides (TMDs) have been widely studied owing to their exciting potential for applications in advanced electronic and optoelectronic devices. Typically, monolayers of TMDs are produced either by mechanical exfoliation or chemical vapor deposition (CVD). While the former produces high-quality flakes with a size limited to a few micrometers, the latter gives large-area layers but with a nonuniform surface resulting from multiple defects and randomly oriented domains. The use of epitaxy growth can produce continuous, crystalline and uniform films with fewer defects. Here, we present a comprehensive study of the optical and structural properties of a single layer of MoS2 synthesized by molecular beam epitaxy (MBE) on a sapphire substrate. For optical characterization, we performed spectroscopic ellipsometry over a broad spectral range (from 250 to 1700 nm) under variable incident angles. The structural quality was assessed by optical microscopy, atomic force microscopy, scanning electron microscopy, and Raman spectroscopy through which we were able to confirm that our sample contains a single-atomic layer of MoS2 with a low number of defects. Raman and photoluminescence spectroscopies revealed that MBE-synthesized MoS2 layers exhibit a two-times higher quantum yield of photoluminescence along with lower photobleaching compared to CVD-grown MoS2, thus making it an attractive candidate for photonic applications.
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Affiliation(s)
- Georgy A. Ermolaev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Marwa A. El-Sayed
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
- Department of Physics, Faculty of Science, Menoufia University, Shebin El-Koom 32511, Egypt
| | - Dmitry I. Yakubovsky
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Kirill V. Voronin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
- Skolkovo Institute of Science and Technology, 3 Nobel Street, 143026 Moscow, Russia
| | - Roman I. Romanov
- Moscow Engineering Physics Institute, National Research Nuclear University MEPhI, 31 Kashirskoe Sh., 115409 Moscow, Russia;
| | - Mikhail K. Tatmyshevskiy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Natalia V. Doroshina
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Anton B. Nemtsov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Artem A. Voronov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Sergey M. Novikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Andrey M. Markeev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Gleb I. Tselikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Andrey A. Vyshnevyy
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
| | - Aleksey V. Arsenin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
- GrapheneTek, Skolkovo Innovation Center, 143026 Moscow, Russia
| | - Valentyn S. Volkov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology, 9 Institutsky Lane, 141700 Dolgoprudny, Russia; (G.A.E.); (M.A.E.-S.); (D.I.Y.); (K.V.V.); (M.K.T.); (N.V.D.); (A.B.N.); (A.A.V.); (S.M.N.); (A.M.M.); (G.I.T.); (A.A.V.); (A.V.A.)
- GrapheneTek, Skolkovo Innovation Center, 143026 Moscow, Russia
- Correspondence: ; Tel.: +7-926-735-93-98
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El-Sayed MA, Ermolaev GA, Voronin KV, Romanov RI, Tselikov GI, Yakubovsky DI, Doroshina NV, Nemtsov AB, Solovey VR, Voronov AA, Novikov SM, Vyshnevyy AA, Markeev AM, Arsenin AV, Volkov VS. Optical Constants of Chemical Vapor Deposited Graphene for Photonic Applications. Nanomaterials (Basel) 2021; 11:1230. [PMID: 34066979 DOI: 10.3390/nano11051230] [Citation(s) in RCA: 11] [Impact Index Per Article: 3.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Key Words] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 04/12/2021] [Revised: 04/22/2021] [Accepted: 04/25/2021] [Indexed: 11/17/2022]
Abstract
Graphene is a promising building block material for developing novel photonic and optoelectronic devices. Here, we report a comprehensive experimental study of chemical-vapor deposited (CVD) monolayer graphene’s optical properties on three different substrates for ultraviolet, visible, and near-infrared spectral ranges (from 240 to 1000 nm). Importantly, our ellipsometric measurements are free from the assumptions of additional nanometer-thick layers of water or other media. This issue is critical for practical applications since otherwise, these additional layers must be included in the design models of various graphene photonic, plasmonic, and optoelectronic devices. We observe a slight difference (not exceeding 5%) in the optical constants of graphene on different substrates. Further, the optical constants reported here are very close to those of graphite, which hints on their applicability to multilayer graphene structures. This work provides reliable data on monolayer graphene’s optical properties, which should be useful for modeling and designing photonic devices with graphene.
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Nizioł J, Gondek E, Karasiński P. Changes in Optical Parameters of SiO 2:TiO 2 Films Obtained by Sol-Gel Method Observed as a Result of Thermal Treatment. Materials (Basel) 2021; 14:2290. [PMID: 33925144 DOI: 10.3390/ma14092290] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/16/2021] [Revised: 04/14/2021] [Accepted: 04/23/2021] [Indexed: 11/21/2022]
Abstract
The research focused on materials having potential applications in technology of planar evanescent wave sensors. Four samples of binary SiO2:TiO2 thin films having different titania content were manufactured through the sol-gel method and dip-coating technique on polished silicon substrates. The samples were subjected to repeated heating/cooling protocols. Simultaneously, their optical parameters were monitored by spectroscopic ellipsometry as they evolved under varying temperature. Subsequent analysis confirmed linear dependence of refractive index on titania content, at least in vis-NIR wavelengths, as well as a low value of the thermal expansion coefficient. It was shown that the thickness of SiO2:TiO2 films decreased as a result of annealing processes, which may be a consequence of reduced porosity.
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Wei W, Peng Y, Wang J, Farooq Saleem M, Wang W, Li L, Wang Y, Sun W. Temperature Dependence of Stress and Optical Properties in AlN Films Grown by MOCVD. Nanomaterials (Basel) 2021; 11:nano11030698. [PMID: 33802171 PMCID: PMC7999848 DOI: 10.3390/nano11030698] [Citation(s) in RCA: 6] [Impact Index Per Article: 2.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 02/14/2021] [Revised: 03/04/2021] [Accepted: 03/05/2021] [Indexed: 11/16/2022]
Abstract
AlN epilayers were grown on a 2-inch [0001] conventional flat sapphire substrate (CSS) and a nano-patterned sapphire substrate (NPSS) by metalorganic chemical vapor deposition. In this work, the effect of the substrate template and temperature on stress and optical properties of AlN films has been studied by using Raman spectroscopy, X-ray diffraction (XRD), transmission electron microscopy (TEM), UV-visible spectrophotometer and spectroscopic ellipsometry (SE). The AlN on NPSS exhibits lower compressive stress and strain values. The biaxial stress decreases from 1.59 to 0.60 GPa for AlN on CSS and from 0.90 to 0.38 GPa for AlN on NPSS sample in the temperature range 80-300 K, which shows compressive stress. According to the TEM data, the stress varies from tensile on the interface to compressive on the surface. It can be deduced that the nano-holes provide more channels for stress relaxation. Nano-patterning leads to a lower degree of disorder and stress/strain relaxes by the formation of the nano-hole structure between the interface of AlN epilayers and the substrate. The low crystal disorder and defects in the AlN on NPSS is confirmed by the small Urbach energy values. The variation in bandgap (Eg) and optical constants (n, k) with temperature are discussed in detail. Nano-patterning leads to poor light transmission due to light scattering, coupling, and trapping in nano-holes.
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Affiliation(s)
- Wenwang Wei
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
| | - Yi Peng
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
| | - Jiabin Wang
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
| | - Muhammad Farooq Saleem
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
| | - Wen Wang
- Advanced Micro-Fabrication Equipment Inc., Shanghai 201201, China;
| | - Lei Li
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
| | - Yukun Wang
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
| | - Wenhong Sun
- Research Center for Optoelectronic Materials and Devices, School of Physical Science & Technology, College of Chemistry and Chemical Engineering, Guangxi University, Nanning 530004, China; (W.W.); (Y.P.); (J.W.); (M.F.S.); (L.L.); (Y.W.)
- Guangxi Key Laboratory of Processing for Non-Ferrous Metallic and Featured Materials, Guangxi University, Nanning 530004, China
- Correspondence:
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Subedi B, Song Z, Chen C, Li C, Ghimire K, Junda MM, Subedi I, Yan Y, Podraza NJ. Optical and Electronic Losses Arising from Physically Mixed Interfacial Layers in Perovskite Solar Cells. ACS Appl Mater Interfaces 2021; 13:4923-4934. [PMID: 33470116 DOI: 10.1021/acsami.0c16364] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.7] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/12/2023]
Abstract
Perovskite solar cell device performance is affected by optical and electronic losses. To minimize these losses in solar cells, it is important to identify their sources. Here, we report the optical and electronic losses arising from physically mixed interfacial layers between the adjacent component materials in highly efficient two terminal (2T) all-perovskite tandem, single-junction wide-bandgap, and single-junction narrow-bandgap perovskite-based solar cells. Physically mixed interfacial layers as the sources of optical and electronic losses are identified from spectroscopic ellipsometry measurements and data analysis followed by comparisons of simulated and measured external quantum efficiency spectra. Parasitic absorbance in the physically mixed regions between silver metal electrical contacts and electron transport layers (ETLs) near the back contact and a physical mixture of commercial indium tin oxide and hole transport layers (HTL) near the front electrical contact lead to substantial optical loss. A lower-density void + perovskite nucleation layer formed during perovskite deposition at the interface between the perovskite absorber layer and the HTL causes electronic losses because of incomplete collection of photogenerated carriers likely originating from poor coverage and passivation of the initially nucleating grains.
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Affiliation(s)
- Biwas Subedi
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Zhaoning Song
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Cong Chen
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Chongwen Li
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Kiran Ghimire
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Maxwell M Junda
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Indra Subedi
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Yanfa Yan
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
| | - Nikolas J Podraza
- Department of Physics and Astronomy and the Wright Center for Photovoltaics Innovation and Commercialization, University of Toledo, Toledo 43606, Ohio, United States
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Janicek P, Putri M, Kim KH, Lee HJ, Bouska M, Šlang S, Lee HY. Spectroscopic Ellipsometry Characterization of As-Deposited and Annealed Non-Stoichiometric Indium Zinc Tin Oxide Thin Film. Materials (Basel) 2021; 14:578. [PMID: 33530567 DOI: 10.3390/ma14030578] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/21/2020] [Revised: 01/10/2021] [Accepted: 01/18/2021] [Indexed: 11/24/2022]
Abstract
A spectroscopic ellipsometry study on as-deposited and annealed non-stoichiometric indium zinc tin oxide thin films of four different compositions prepared by RF magnetron sputtering was conducted. Multi-sample analysis with two sets of samples sputtered onto glass slides and silicon wafers, together with the analysis of the samples onto each substrate separately, was utilized for as-deposited samples. Annealed samples onto the glass slides were also analyzed. Spectroscopic ellipsometry in a wide spectral range (0.2–6 eV) was used to determine optical constants (refractive index n and extinction coefficient k) of these films. Parameterized semiconductor oscillator function, together with Drude oscillator, was used as a model dielectric function. Geometrical parameters (layer thickness and surface roughness) and physical parameters (direct optical bandgap, free carrier concentration, mobility, and specific electrical resistivity) were determined from spectroscopic ellipsometry data modeling. Specific electrical resistivity determined from the Drude oscillator corresponds well with the results from electrical measurements. Change in the optical bandgap, visible especially for annealed samples, corresponds with the change of free carrier concentration (Moss–Burstein effect). Scanning electron microscope did not reveal any noticeable annealing-induced change in surface morphology.
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Colin J, Jamnig A, Furgeaud C, Michel A, Pliatsikas N, Sarakinos K, Abadias G. In Situ and Real-Time Nanoscale Monitoring of Ultra-Thin Metal Film Growth Using Optical and Electrical Diagnostic Tools. Nanomaterials (Basel) 2020; 10:E2225. [PMID: 33182409 PMCID: PMC7697846 DOI: 10.3390/nano10112225] [Citation(s) in RCA: 14] [Impact Index Per Article: 3.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 10/03/2020] [Revised: 10/30/2020] [Accepted: 11/03/2020] [Indexed: 01/08/2023]
Abstract
Continued downscaling of functional layers for key enabling devices has prompted the development of characterization tools to probe and dynamically control thin film formation stages and ensure the desired film morphology and functionalities in terms of, e.g., layer surface smoothness or electrical properties. In this work, we review the combined use of in situ and real-time optical (wafer curvature, spectroscopic ellipsometry) and electrical probes for gaining insights into the early growth stages of magnetron-sputter-deposited films. Data are reported for a large variety of metals characterized by different atomic mobilities and interface reactivities. For fcc noble-metal films (Ag, Cu, Pd) exhibiting a pronounced three-dimensional growth on weakly-interacting substrates (SiO2, amorphous carbon (a-C)), wafer curvature, spectroscopic ellipsometry, and resistivity techniques are shown to be complementary in studying the morphological evolution of discontinuous layers, and determining the percolation threshold and the onset of continuous film formation. The influence of growth kinetics (in terms of intrinsic atomic mobility, substrate temperature, deposition rate, deposition flux temporal profile) and the effect of deposited energy (through changes in working pressure or bias voltage) on the various morphological transition thicknesses is critically examined. For bcc transition metals, like Fe and Mo deposited on a-Si, in situ and real-time growth monitoring data exhibit transient features at a critical layer thickness of ~2 nm, which is a fingerprint of an interface-mediated crystalline-to-amorphous phase transition, while such behavior is not observed for Ta films that crystallize into their metastable tetragonal β-Ta allotropic phase. The potential of optical and electrical diagnostic tools is also explored to reveal complex interfacial reactions and their effect on growth of Pd films on a-Si or a-Ge interlayers. For all case studies presented in the article, in situ data are complemented with and benchmarked against ex situ structural and morphological analyses.
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Affiliation(s)
- Jonathan Colin
- Institut Pprime, UPR 3346, CNRS-Université de Poitiers-ENSMA, 11 Boulevard Marie et Pierre Curie, TSA 41123, CEDEX 9, 86073 Poitiers, France; (J.C.); (A.J.); (C.F.); (A.M.)
| | - Andreas Jamnig
- Institut Pprime, UPR 3346, CNRS-Université de Poitiers-ENSMA, 11 Boulevard Marie et Pierre Curie, TSA 41123, CEDEX 9, 86073 Poitiers, France; (J.C.); (A.J.); (C.F.); (A.M.)
- Nanoscale Engineering Division, Department of Physics, Chemistry and Biology, Linköping University, SE 581 83 Linköping, Sweden;
| | - Clarisse Furgeaud
- Institut Pprime, UPR 3346, CNRS-Université de Poitiers-ENSMA, 11 Boulevard Marie et Pierre Curie, TSA 41123, CEDEX 9, 86073 Poitiers, France; (J.C.); (A.J.); (C.F.); (A.M.)
| | - Anny Michel
- Institut Pprime, UPR 3346, CNRS-Université de Poitiers-ENSMA, 11 Boulevard Marie et Pierre Curie, TSA 41123, CEDEX 9, 86073 Poitiers, France; (J.C.); (A.J.); (C.F.); (A.M.)
| | - Nikolaos Pliatsikas
- Nanoscale Engineering Division, Department of Physics, Chemistry and Biology, Linköping University, SE 581 83 Linköping, Sweden;
| | - Kostas Sarakinos
- Nanoscale Engineering Division, Department of Physics, Chemistry and Biology, Linköping University, SE 581 83 Linköping, Sweden;
| | - Gregory Abadias
- Institut Pprime, UPR 3346, CNRS-Université de Poitiers-ENSMA, 11 Boulevard Marie et Pierre Curie, TSA 41123, CEDEX 9, 86073 Poitiers, France; (J.C.); (A.J.); (C.F.); (A.M.)
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Labadi Z, Kalas B, Saftics A, Illes L, Jankovics H, Bereczk-Tompa É, Sebestyén A, Tóth É, Kakasi B, Moldovan C, Firtat B, Gartner M, Gheorghe M, Vonderviszt F, Fried M, Petrik P. Sensing Layer for Ni Detection in Water Created by Immobilization of Bioengineered Flagellar Nanotubes on Gold Surfaces. ACS Biomater Sci Eng 2020; 6:3811-3820. [PMID: 33463317 DOI: 10.1021/acsbiomaterials.0c00280] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Journal Information] [Subscribe] [Scholar Register] [Indexed: 01/31/2023]
Abstract
The environmental monitoring of Ni is targeted at a threshold limit value of 0.34 μM, as set by the World Health Organization. This sensitivity target can usually only be met by time-consuming and expensive laboratory measurements. There is a need for inexpensive, field-applicable methods, even if they are only used for signaling the necessity of a more accurate laboratory investigation. In this work, bioengineered, protein-based sensing layers were developed for Ni detection in water. Two bacterial Ni-binding flagellin variants were fabricated using genetic engineering, and their applicability as Ni-sensitive biochip coatings was tested. Nanotubes of mutant flagellins were built by in vitro polymerization. A large surface density of the nanotubes on the sensor surface was achieved by covalent immobilization chemistry based on a dithiobis(succimidyl propionate) cross-linking method. The formation and density of the sensing layer was monitored and verified by spectroscopic ellipsometry and atomic force microscopy. Cyclic voltammetry (CV) measurements revealed a Ni sensitivity below 1 μM. It was also shown that, even after two months of storage, the used sensors can be regenerated and reused by rinsing in a 10 mM solution of ethylenediaminetetraacetic acid at room temperature.
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Affiliation(s)
- Zoltan Labadi
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary
| | - Benjamin Kalas
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary
| | - Andras Saftics
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary
| | - Levente Illes
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary
| | - Hajnalka Jankovics
- Research Institute of Biomolecular and Chemical Engineering, University of Pannonia, Veszprém 8200, Hungary
| | - Éva Bereczk-Tompa
- Research Institute of Biomolecular and Chemical Engineering, University of Pannonia, Veszprém 8200, Hungary
| | - Anett Sebestyén
- Research Institute of Biomolecular and Chemical Engineering, University of Pannonia, Veszprém 8200, Hungary
| | - Éva Tóth
- Research Institute of Biomolecular and Chemical Engineering, University of Pannonia, Veszprém 8200, Hungary
| | - Balázs Kakasi
- Research Institute of Biomolecular and Chemical Engineering, University of Pannonia, Veszprém 8200, Hungary
| | - Carmen Moldovan
- National Institute for Research & Development in Microtechnologies, Bucharest 077190, Romania
| | - Bogdan Firtat
- National Institute for Research & Development in Microtechnologies, Bucharest 077190, Romania
| | - Mariuca Gartner
- "Ilie Murgulescu" Institute of Physical Chemistry of the Romanian Academy, Bucharest 060021, Romania
| | | | - Ferenc Vonderviszt
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary.,Research Institute of Biomolecular and Chemical Engineering, University of Pannonia, Veszprém 8200, Hungary
| | - Miklos Fried
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary.,Institute of Microelectronics and Technology, Óbuda University, Budapest 1034, Hungary
| | - Peter Petrik
- Institute of Technical Physics and Materials Science, Centre for Energy Research, Budapest 1121, Hungary
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Hajduk B, Bednarski H, Domański M, Jarząbek B, Trzebicka B. Thermal Transitions in P3HT:PC60BM Films Based on Electrical Resistance Measurements. Polymers (Basel) 2020; 12:E1458. [PMID: 32629756 PMCID: PMC7407113 DOI: 10.3390/polym12071458] [Citation(s) in RCA: 5] [Impact Index Per Article: 1.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/21/2020] [Revised: 06/26/2020] [Accepted: 06/27/2020] [Indexed: 01/20/2023] Open
Abstract
In this paper, we present research on thermal transition temperature determination in poly (3-hexylthiophene-2,5-diyl) (P3HT), [6,6]-phenyl-C61-butyric acid methyl ester (PC60BM), and their blends, which are materials that are conventionally used in organic optoelectronics. Here, for the first time the results of electrical resistance measurements are explored to detect thermal transitions temperatures, such as glass transition Tg and cold crystallization Tcc of the film. To confirm these results, the variable-temperature spectroscopic ellipsometry studies of the same samples were performed. The thermal transitions temperatures obtained with electrical measurements are well suited to phase diagram, constructed on the basis of ellipsometry in our previous work. The data presented here prove that electrical resistance measurements alone are sufficient for qualitative thermal analysis, which lead to the identification of characteristic temperatures in P3HT:PC60BM films. Based on the carried studies, it can be expected that the determination of thermal transition temperatures by means of electrical resistance measurements will also apply to other semi-conducting polymer films.
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Affiliation(s)
- Barbara Hajduk
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska str., 41-819 Zabrze, Poland; (H.B.); (M.D.); (B.J.)
| | | | | | | | - Barbara Trzebicka
- Centre of Polymer and Carbon Materials, Polish Academy of Sciences, 34 Marie Curie-Skłodowska str., 41-819 Zabrze, Poland; (H.B.); (M.D.); (B.J.)
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Chi Sin Tang, Xinmao Yin, Ming Yang, Di Wu, Jing Wu, Lai Mun Wong, Changjian Li, Shi Wun Tong, Yung‐Huang Chang, Fangping Ouyang, Yuan Ping Feng, Shi Jie Wang, Dongzhi Chi, Mark B. H. Breese, Wenjing Zhang, Andrivo Rusydi, Andrew T. S. Wee. Transition‐Metal Dichalcogenides: Anisotropic Collective Charge Excitations in Quasimetallic 2D Transition‐Metal Dichalcogenides (Adv. Sci. 10/2020). Adv Sci (Weinh) 2020; 7:2070055. [ DOI: 10.1002/advs.202070055] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [What about the content of this article? (0)] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/13/2023]
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Tang CS, Yin X, Yang M, Wu D, Wu J, Wong LM, Li C, Tong SW, Chang Y, Ouyang F, Feng YP, Wang SJ, Chi D, Breese MBH, Zhang W, Rusydi A, Wee ATS. Anisotropic Collective Charge Excitations in Quasimetallic 2D Transition-Metal Dichalcogenides. Adv Sci (Weinh) 2020; 7:1902726. [PMID: 32440469 PMCID: PMC7237846 DOI: 10.1002/advs.201902726] [Citation(s) in RCA: 2] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 10/01/2019] [Revised: 02/11/2020] [Accepted: 03/13/2020] [Indexed: 06/11/2023]
Abstract
The quasimetallic 1T' phase 2D transition-metal dichalcogenides (TMDs) consist of 1D zigzag metal chains stacked periodically along a single axis. This gives rise to its prominent physical properties which promises the onset of novel physical phenomena and applications. Here, the in-plane electronic correlations are explored, and new mid-infrared plasmon excitations in 1T' phase monolayer WSe2 and MoS2 are observed using optical spectroscopies. Based on an extensive first-principles study which analyzes the charge dynamics across multiple axes of the atomic-layered systems, the collective charge excitations are found to disperse only along the direction perpendicular to the chains. Further analysis reveals that the interchain long-range coupling is responsible for the coherent 1D charge dynamics and the spin-orbit coupling affects the plasmon frequency. Detailed investigation of these charge collective modes in 2D-chained systems offers opportunities for novel device applications and has implications for the underlying mechanism that governs superconductivity in 2D TMD systems.
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Affiliation(s)
- Chi Sin Tang
- Department of PhysicsFaculty of ScienceNational University of SingaporeS12 Science Drive 3Singapore117551Singapore
- NUS Graduate School for Integrative Sciences and EngineeringNational University of Singapore21 Lower Kent RidgeSingapore119077Singapore
| | - Xinmao Yin
- Department of PhysicsFaculty of ScienceNational University of SingaporeS12 Science Drive 3Singapore117551Singapore
- Singapore Synchrotron Light Source (SSLS)National University of Singapore5 Research LinkSingapore117603Singapore
| | - Ming Yang
- Institute of Materials Research and Engineering (IMRE)A*STAR (Agency for Science, Technology and Research)2 Fusionopolis Way, InnovisSingapore138634Singapore
| | - Di Wu
- International Collaborative Laboratory of 2D Materials for Optoelectronics Science and TechnologyShenzhen UniversityShenzhen518060China
- School of Physics and ElectronicsCentral South UniversityNo. 932, South Lushan RoadChangshaHunan410083China
| | - Jing Wu
- Institute of Materials Research and Engineering (IMRE)A*STAR (Agency for Science, Technology and Research)2 Fusionopolis Way, InnovisSingapore138634Singapore
| | - Lai Mun Wong
- Institute of Materials Research and Engineering (IMRE)A*STAR (Agency for Science, Technology and Research)2 Fusionopolis Way, InnovisSingapore138634Singapore
| | - Changjian Li
- Department of Materials Science & EngineeringNational University of Singapore9 Engineering Drive 1Singapore117575Singapore
| | - Shi Wun Tong
- Institute of Materials Research and Engineering (IMRE)A*STAR (Agency for Science, Technology and Research)2 Fusionopolis Way, InnovisSingapore138634Singapore
| | - Yung‐Huang Chang
- Bachelor Program in Interdisciplinary StudiesNational Yunlin University of Science and Technology123 University Road, Section 3DouliouYunlin64002Taiwan
| | - Fangping Ouyang
- School of Physics and ElectronicsCentral South UniversityNo. 932, South Lushan RoadChangshaHunan410083China
| | - Yuan Ping Feng
- Department of PhysicsFaculty of ScienceNational University of SingaporeS12 Science Drive 3Singapore117551Singapore
| | - Shi Jie Wang
- Institute of Materials Research and Engineering (IMRE)A*STAR (Agency for Science, Technology and Research)2 Fusionopolis Way, InnovisSingapore138634Singapore
| | - Dongzhi Chi
- Institute of Materials Research and Engineering (IMRE)A*STAR (Agency for Science, Technology and Research)2 Fusionopolis Way, InnovisSingapore138634Singapore
| | - Mark B. H. Breese
- Department of PhysicsFaculty of ScienceNational University of SingaporeS12 Science Drive 3Singapore117551Singapore
- Singapore Synchrotron Light Source (SSLS)National University of Singapore5 Research LinkSingapore117603Singapore
| | - Wenjing Zhang
- International Collaborative Laboratory of 2D Materials for Optoelectronics Science and TechnologyShenzhen UniversityShenzhen518060China
| | - Andrivo Rusydi
- Department of PhysicsFaculty of ScienceNational University of SingaporeS12 Science Drive 3Singapore117551Singapore
- Singapore Synchrotron Light Source (SSLS)National University of Singapore5 Research LinkSingapore117603Singapore
| | - Andrew T. S. Wee
- Department of PhysicsFaculty of ScienceNational University of SingaporeS12 Science Drive 3Singapore117551Singapore
- NUS Graduate School for Integrative Sciences and EngineeringNational University of Singapore21 Lower Kent RidgeSingapore119077Singapore
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Tatarkin DE, Yakubovsky DI, Ermolaev GA, Stebunov YV, Voronov AA, Arsenin AV, Volkov VS, Novikov SM. Surface-Enhanced Raman Spectroscopy on Hybrid Graphene/Gold Substrates near the Percolation Threshold. Nanomaterials (Basel) 2020; 10:E164. [PMID: 31963496 PMCID: PMC7022774 DOI: 10.3390/nano10010164] [Citation(s) in RCA: 14] [Impact Index Per Article: 3.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Grants] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 12/19/2019] [Revised: 01/14/2020] [Accepted: 01/14/2020] [Indexed: 11/21/2022]
Abstract
Graphene is a promising platform for surface-enhanced Raman spectroscopy (SERS)-active substrates, primarily due to the possibility of quenching photoluminescence and fluorescence. Here we study ultrathin gold films near the percolation threshold fabricated by electron-beam deposition on monolayer CVD graphene. The advantages of such hybrid graphene/gold substrates for surface-enhanced Raman spectroscopy are discussed in comparison with conventional substrates without the graphene layer. The percolation threshold is determined by independent measurements of the sheet resistance and effective dielectric constant by spectroscopic ellipsometry. The surface morphology of the ultrathin gold films is analyzed by the use of scanning electron microscopy (SEM) and atomic force microscopy (AFM), and the thicknesses of the films in addition to the quartz-crystal mass-thickness sensor are also measured by AFM. We experimentally demonstrate that the maximum SERS signal is observed near and slightly below the percolation threshold. In this case, the region of maximum enhancement of the SERS signal can be determined using the figure of merit (FOM), which is the ratio of the real and imaginary parts of the effective dielectric permittivity of the films. SERS measurements on hybrid graphene/gold substrates with the dye Crystal Violet show an enhancement factor of ~105 and also demonstrate the ability of graphene to quench photoluminescence by an average of ~60%.
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Affiliation(s)
- Dmitry E. Tatarkin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
| | - Dmitry I. Yakubovsky
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
| | - Georgy A. Ermolaev
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
- Skolkovo Institute of Science and Technology, 121205 Moscow, Russia
| | - Yury V. Stebunov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
| | - Artem A. Voronov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
| | - Aleksey V. Arsenin
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
| | - Valentyn S. Volkov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
| | - Sergey M. Novikov
- Center for Photonics and 2D Materials, Moscow Institute of Physics and Technology (MIPT), 141700 Dolgoprudny, Russia; (D.I.Y.); or (Y.V.S.); (A.A.V.); (A.V.A.); (V.S.V.)
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Mukherjee S, Attiaoui A, Bauer M, Moutanabbir O. 3D Atomic Mapping of Interfacial Roughness and Its Spatial Correlation Length in Sub-10 nm Superlattices. ACS Appl Mater Interfaces 2020; 12:1728-1736. [PMID: 31808669 DOI: 10.1021/acsami.9b13802] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/10/2023]
Abstract
The interfacial abruptness and uniformity in heterostructures are critical to control their electronic and optical properties. With this perspective, this work demonstrates the three-dimensional (3D) atomic-level mapping of the roughness and uniformity of buried epitaxial interfaces in Si/SiGe superlattices with a layer thickness in the 1.5-7.5 nm range. Herein, 3D atom-by-atom maps were acquired and processed to generate isoconcentration surfaces highlighting local fluctuations in content at each interface. These generated surfaces were subsequently utilized to map the interfacial roughness and its spatial correlation length. The analysis revealed that the root-mean-squared roughness of the buried interfaces in the investigated superlattices is sensitive to the growth temperature with a value varying from 0.17 ± 0.02 to 0.26 ± 0.03 nm in the temperature range of 500-650 °C. The estimated horizontal correlation lengths were found to be 8.11 ± 0.5 nm at 650 °C and 10.09 ± 0.6 nm at 500 °C. Additionally, reducing the growth temperature was found to improve the interfacial abruptness, with a 30% smaller interfacial width is obtained at 500 °C. This behavior is attributed to the thermally activated atomic exchange at the surface during the heteroepitaxy. Finally, by testing different optical models with increasing levels of interfacial complexity, it is demonstrated that the observed atomic-level roughening at the interface must be accounted for to accurately describe the optical response of Si/SiGe heterostructures.
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Affiliation(s)
- Samik Mukherjee
- Department of Engineering Physics , École Polytechnique de Montréal , C. P. 6079, Succ. Centre-Ville , Montreal , Québec H3C 3A7 , Canada
| | - Anis Attiaoui
- Department of Engineering Physics , École Polytechnique de Montréal , C. P. 6079, Succ. Centre-Ville , Montreal , Québec H3C 3A7 , Canada
| | - Matthias Bauer
- Applied Materials Inc. , 974 E. Arques Avenue , Sunnyvale , California 94085 , United States
| | - Oussama Moutanabbir
- Department of Engineering Physics , École Polytechnique de Montréal , C. P. 6079, Succ. Centre-Ville , Montreal , Québec H3C 3A7 , Canada
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44
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Tang CS, Yin X, Yang M, Wu D, Birowosuto MD, Wu J, Li C, Hettiarachchi C, Chin XY, Chang YH, Ouyang F, Dang C, Pennycook SJ, Feng YP, Wang S, Chi D, Breese MBH, Zhang W, Rusydi A, Wee ATS. Three-Dimensional Resonant Exciton in Monolayer Tungsten Diselenide Actuated by Spin-Orbit Coupling. ACS Nano 2019; 13:14529-14539. [PMID: 31702890 DOI: 10.1021/acsnano.9b08385] [Citation(s) in RCA: 0] [Impact Index Per Article: 0] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/10/2023]
Abstract
The intricate features of many-body interactions and spin-orbit coupling play a significant role in numerous physical phenomena. Particularly in two-dimensional transition metal dichalcogenides (2D-TMDs), excitonic dynamics are a key phenomenon that promises opportunities for diverse range of device applications. Here, we report the direct observation of a visible-range three-dimensional resonant exciton and its associated charged exciton in monolayer tungsten diselenide, as compared to monolayer molybdenum disulfide. A comprehensive experimental study that includes high-resolution TEM, Raman, high-resolution spectroscopic ellipsometry over a wide temperature range down to 4 K, high-energy temperature, and excitation power-dependent photoluminescence spectroscopy has been conducted. It is supported by first-principles calculations to unravel the influence of spin-orbit coupling in the formation of the resonant exciton and to identify its in-plane and out-of-plane features. Furthermore, we study the impact of temperature and thickness on the spin-orbit coupling strength in 2D-TMDs. This work is crucial in creating a platform in the fundamental understanding of high-energy resonant exciton in layered two-dimensional systems and that such high-energy optoelectronic features make them an increasingly attractive candidate for novel electronic and optoelectronic applications particularly in the aspects of solar cells and light-emitting diodes via the manipulation of excitonic states.
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Affiliation(s)
- Chi Sin Tang
- Department of Physics, Faculty of Science , National University of Singapore , Singapore 117542 , Singapore
- NUS Graduate School for Integrative Sciences and Engineering , National University of Singapore , Singapore 117456 , Singapore
| | - Xinmao Yin
- Department of Physics, Faculty of Science , National University of Singapore , Singapore 117542 , Singapore
- Singapore Synchrotron Light Source (SSLS) , National University of Singapore , Singapore 117603 , Singapore
| | - Ming Yang
- Institute of Materials Research and Engineering, A*STAR (Agency for Science, Technology and Research) , 2 Fusionopolis Way , Singapore 138634 , Singapore
| | - Di Wu
- International Collaborative Laboratory of 2D Materials for Optoelectronics Science and Technology , Shenzhen University , Shenzhen 518060 , China
- School of Physics and Electronics , Central South University , No. 932, South Lushan Road , Changsha , Hunan Province 410083 , China
| | - Muhammad Danang Birowosuto
- CINTRA UMI CNRS/NTU/THALES 3288, Research Techno Plaza , 50 Nanyang Drive, Border X Block, Level 6 , Singapore 637553 , Singapore
- School of Electrical and Electronic Engineering , Nanyang Technological University , 50 Nanyang Avenue , Singapore 639798 , Singapore
| | - Jing Wu
- Institute of Materials Research and Engineering, A*STAR (Agency for Science, Technology and Research) , 2 Fusionopolis Way , Singapore 138634 , Singapore
| | - Changjian Li
- Department of Materials Science & Engineering , National University of Singapore , 9 Engineering Drive 1 , Singapore 117575 , Singapore
| | - Chathuranga Hettiarachchi
- School of Electrical and Electronic Engineering , Nanyang Technological University , 50 Nanyang Avenue , Singapore 639798 , Singapore
| | - Xin Yu Chin
- CINTRA UMI CNRS/NTU/THALES 3288, Research Techno Plaza , 50 Nanyang Drive, Border X Block, Level 6 , Singapore 637553 , Singapore
| | - Yung-Huang Chang
- Bachelor Program in Interdisciplinary Studies , National Yunlin University of Science and Technology , 123 University Road, Section 3 , Douliou , Yunlin 64002 , Taiwan
| | - Fangping Ouyang
- School of Physics and Electronics , Central South University , No. 932, South Lushan Road , Changsha , Hunan Province 410083 , China
| | - Cuong Dang
- CINTRA UMI CNRS/NTU/THALES 3288, Research Techno Plaza , 50 Nanyang Drive, Border X Block, Level 6 , Singapore 637553 , Singapore
- School of Electrical and Electronic Engineering , Nanyang Technological University , 50 Nanyang Avenue , Singapore 639798 , Singapore
| | - Stephen J Pennycook
- Department of Materials Science & Engineering , National University of Singapore , 9 Engineering Drive 1 , Singapore 117575 , Singapore
| | - Yuan Ping Feng
- Department of Physics, Faculty of Science , National University of Singapore , Singapore 117542 , Singapore
| | - Shijie Wang
- Institute of Materials Research and Engineering, A*STAR (Agency for Science, Technology and Research) , 2 Fusionopolis Way , Singapore 138634 , Singapore
| | - Dongzhi Chi
- Institute of Materials Research and Engineering, A*STAR (Agency for Science, Technology and Research) , 2 Fusionopolis Way , Singapore 138634 , Singapore
| | - Mark B H Breese
- Department of Physics, Faculty of Science , National University of Singapore , Singapore 117542 , Singapore
- Singapore Synchrotron Light Source (SSLS) , National University of Singapore , Singapore 117603 , Singapore
| | - Wenjing Zhang
- International Collaborative Laboratory of 2D Materials for Optoelectronics Science and Technology , Shenzhen University , Shenzhen 518060 , China
| | - Andrivo Rusydi
- Department of Physics, Faculty of Science , National University of Singapore , Singapore 117542 , Singapore
- Singapore Synchrotron Light Source (SSLS) , National University of Singapore , Singapore 117603 , Singapore
- NUS Graduate School for Integrative Sciences and Engineering , National University of Singapore , Singapore 117456 , Singapore
| | - Andrew T S Wee
- Department of Physics, Faculty of Science , National University of Singapore , Singapore 117542 , Singapore
- Singapore Synchrotron Light Source (SSLS) , National University of Singapore , Singapore 117603 , Singapore
- NUS Graduate School for Integrative Sciences and Engineering , National University of Singapore , Singapore 117456 , Singapore
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Kumar L, Horechyy A, Bittrich E, Nandan B, Uhlmann P, Fery A. Amphiphilic Block Copolymer Micelles in Selective Solvents: The Effect of Solvent Selectivity on Micelle Formation. Polymers (Basel) 2019; 11:E1882. [PMID: 31739558 DOI: 10.3390/polym11111882] [Citation(s) in RCA: 15] [Impact Index Per Article: 3.0] [Reference Citation Analysis] [What about the content of this article? (0)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 05/30/2019] [Revised: 10/23/2019] [Accepted: 11/11/2019] [Indexed: 12/15/2022] Open
Abstract
We investigated the micellar behavior of a series of asymmetric polystyrene-block-poly(4-vinylpyridine) (PS-b-P4VP) block copolymers in different P4VP-selective alcoholic solvents. The micellar behavior was further correlated with the spectroscopic ellipsometry results obtained on swelling of PS and P4VP polymer films in the corresponding solvent vapors. The time-resolved (in situ) dynamic light scattering (DLS) measurements, in combination with (ex situ) electron microscopy imaging, revealed information about the aggregation state of PS-b-P4VP BCP in different alcohols and the effect of heat treatment. The ellipsometry measurements allowed us to estimate the difference in solvent selectivity toward PS/P4VP pair. Both DLS and ellipsometric studies suggested that less polar alcohols (i.e., 1-propanol, 1-butanol, and 1-pentanol) are likely to be close to each other in terms of their selectivity toward PS/P4VP pair, whereas more polar ethanol and methanol show the highest and the lowest affinity toward P4VP, respectively.
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46
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Dong BX, Liu Z, Misra M, Strzalka J, Niklas J, Poluektov OG, Escobedo FA, Ober CK, Nealey PF, Patel SN. Structure Control of a π-Conjugated Oligothiophene-Based Liquid Crystal for Enhanced Mixed Ion/Electron Transport Characteristics. ACS Nano 2019; 13:7665-7675. [PMID: 31194507 DOI: 10.1021/acsnano.9b01055] [Citation(s) in RCA: 12] [Impact Index Per Article: 2.4] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 05/21/2023]
Abstract
Developing soft materials with both ion and electron transport functionalities is of broad interest for energy-storage and bioelectronics applications. Rational design of these materials requires a fundamental understanding of interactions between ion and electron conducting blocks along with the correlation between the microstructure and the conduction characteristics. Here, we investigate the structure and mixed ionic/electronic conduction in thin films of a liquid crystal (LC) 4T/PEO4, which consists of an electronically conducting quarterthiophene (4T) block terminated at both ends by ionically conducting oligoethylenoxide (PEO4) blocks. Using a combined experimental and simulation approach, 4T/PEO4 is shown to self-assemble into smectic, ordered, or disordered phases upon blending the materials with the ionic dopant bis(trifluoromethane)sulfonimide lithium (LiTFSI) under different LiTFSI concentrations. Interestingly, at intermediate LiTFSI concentration, ordered 4T/PEO4 exhibits an electronic conductivity as high as 3.1 × 10-3 S/cm upon being infiltrated with vapor of the 2,3,5,6-tetrafluoro-7,7,8,8-tetracyanoquinodimethane (F4TCNQ) molecular dopant while still maintaining its ionic conducting functionality. This electronic conductivity is superior by an order of magnitude to the previously reported electronic conductivity of vapor co-deposited 4T/F4TCNQ blends. Our findings demonstrate that structure and electronic transport in mixed conduction materials could be modulated by the presence of the ion transporting component and will have important implications for other more complex mixed ionic/electronic conductors.
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Affiliation(s)
- Ban Xuan Dong
- Pritzker School of Molecular Engineering , University of Chicago , Chicago , Illinois 60637 , United States
| | | | | | | | | | | | | | | | - Paul F Nealey
- Pritzker School of Molecular Engineering , University of Chicago , Chicago , Illinois 60637 , United States
| | - Shrayesh N Patel
- Pritzker School of Molecular Engineering , University of Chicago , Chicago , Illinois 60637 , United States
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47
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Bulai G, Pompilian O, Gurlui S, Nemec P, Nazabal V, Cimpoesu N, Chazallon B, Focsa C. Ge-Sb-Te Chalcogenide Thin Films Deposited by Nanosecond, Picosecond, and Femtosecond Laser Ablation. Nanomaterials (Basel) 2019; 9:E676. [PMID: 31052395 PMCID: PMC6567795 DOI: 10.3390/nano9050676] [Citation(s) in RCA: 9] [Impact Index Per Article: 1.8] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 03/23/2019] [Revised: 04/18/2019] [Accepted: 04/23/2019] [Indexed: 12/20/2022]
Abstract
Ge-Sb-Te thin films were obtained by ns-, ps-, and fs-pulsed laser deposition (PLD) in various experimental conditions. The thickness of the samples was influenced by the Nd-YAG laser wavelength, fluence, target-to-substrate distance, and deposition time. The topography and chemical analysis results showed that the films deposited by ns-PLD revealed droplets on the surface together with a decreased Te concentration and Sb over-stoichiometry. Thin films with improved surface roughness and chemical compositions close to nominal values were deposited by ps- and fs-PLD. The X-ray diffraction and Raman spectroscopy results showed that the samples obtained with ns pulses were partially crystallized while the lower fluences used in ps- and fs-PLD led to amorphous depositions. The optical parameters of the ns-PLD samples were correlated to their structural properties.
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Affiliation(s)
- Georgiana Bulai
- Integrated Centre for Environmental Science Studies in the North-East Development Region-CERNESIM, "Al. I. Cuza" University of Iasi, 700506 Iasi, Romania.
| | - Oana Pompilian
- Université de Lille, CNRS, UMR 8523-PhLAM-Physique des Lasers, Atomes et Molécules, CERLA-Centre d'Etudes et de Recherches Lasers et Applications, Lille F-59000, France.
- National Institute for Lasers, Plasma and Radiation Physics, RO-077125 Magurele-Bucharest, Romania.
| | - Silviu Gurlui
- Faculty of Physics, "Al. I. Cuza" University of Iasi, 700506 Iasi, Romania.
| | - Petr Nemec
- Faculty of Chemical Technology, University of Pardubice, 53210 Pardubice, Czech Republic.
| | - Virginie Nazabal
- Faculty of Chemical Technology, University of Pardubice, 53210 Pardubice, Czech Republic.
- Université de Rennes 1, CNRS, ISCR (Institut des Sciences Chimiques de Rennes)⁻UMR 6226, F-35000 Rennes, France.
| | - Nicanor Cimpoesu
- Faculty of Materials Science and Engineering, "Gheorghe Asachi" Technical University of Iasi, 700050 Iasi, Romania.
| | - Bertrand Chazallon
- Université de Lille, CNRS, UMR 8523-PhLAM-Physique des Lasers, Atomes et Molécules, CERLA-Centre d'Etudes et de Recherches Lasers et Applications, Lille F-59000, France.
| | - Cristian Focsa
- Université de Lille, CNRS, UMR 8523-PhLAM-Physique des Lasers, Atomes et Molécules, CERLA-Centre d'Etudes et de Recherches Lasers et Applications, Lille F-59000, France.
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48
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Jeon N, Lightcap I, Mandia DJ, Martinson ABF. Plasma-Enhanced Atomic Layer Deposition of TiAlN: Compositional and Optoelectronic Tunability. ACS Appl Mater Interfaces 2019; 11:11602-11611. [PMID: 30821951 DOI: 10.1021/acsami.8b21461] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.2] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
Titanium nitride (TiN) is a unique refractory plasmonic material, the nanocomposites and alloys of which provide further opportunities to tailor its optical and photonic properties. We prepare TiAlN films of continuously variable compositions through the systematic variation of TiN versus AlN cycle ratio in plasma-enhanced atomic layer deposition (PEALD) and investigate the resulting thin-film composition, crystallinity, and optical properties. The resulting properties of TiAlN films are not simple linear combinations of the TiN and AlN films, which exhibit distinct metallic and dielectric properties, but instead are dramatically influenced by the local chemical environment of neighboring constituents. In situ spectroscopic ellipsometry further enables measurement of the varying optical properties of TiAlN films, which evolve over 10 s of nm of film thickness. The tunable optoelectronic properties of TiAlN films enable durable coatings of variable electrical resistance as well as high-temperature diffusion barriers and optical coatings with application to selective solar absorbers and emitters.
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Affiliation(s)
| | - Ian Lightcap
- Center for Sustainable Energy at Notre Dame , University of Notre Dame , Notre Dame , Indiana 46556 , United States
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Cechalova B, Branecky M, Klapetek P, Cech V. Optical Properties of Oxidized Plasma-Polymerized Organosilicones and Their Correlation with Mechanical and Chemical Parameters. Materials (Basel) 2019; 12:ma12030539. [PMID: 30759719 PMCID: PMC6384779 DOI: 10.3390/ma12030539] [Citation(s) in RCA: 8] [Impact Index Per Article: 1.6] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 01/16/2019] [Revised: 01/31/2019] [Accepted: 02/06/2019] [Indexed: 11/22/2022]
Abstract
Pure tetravinylsilane and its oxygen mixture were used to deposit oxidized plasma polymer films at various effective power (0.1–10 W) and various oxygen fractions (0–0.71) using RF pulsed plasma. The optical properties (refractive index, extinction coefficient, band gap) of the deposited films were investigated by spectroscopic ellipsometry (230–830 nm) using an optical model and Tauc‒Lorentz parametrization. Analyses of chemical and mechanical properties of films allowed for the interpretation of changes in optical properties with deposition conditions. The refractive index was revealed to increase with enhanced effective power due to the increased crosslinking of the plasma polymer network but decreased when increasing the oxygen fraction due to the decrease of polymer crosslinking as the number of carbon bonds in the plasma polymer network was eliminated. A very strong positive correlation was found between the Young’s modulus and the refractive index for oxidized plasma polymer films. The optical properties of films correlated with their chemical properties for the specific deposition conditions used in this study. The band gap (1.9–2.9 eV) was assumed to be widened due to the increased concentration of vinyl groups in oxidized plasma polymer films.
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Affiliation(s)
- Bozena Cechalova
- CEITEC, Brno University of Technology, Purkynova 123, 612 00 Brno, Czech Republic.
| | - Martin Branecky
- Institute of Materials Chemistry, Faculty of Chemistry, Brno University of Technology, Purkynova 118, 612 00 Brno, Czech Republic.
| | - Petr Klapetek
- Czech Metrology Institute, Okruzni 31, 638 00 Brno, Czech Republic.
| | - Vladimir Cech
- Institute of Materials Chemistry, Faculty of Chemistry, Brno University of Technology, Purkynova 118, 612 00 Brno, Czech Republic.
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Li Z, Pan F, Li R, Pambou E, Hu X, Ruane S, Ciumac D, Li P, Welbourn RJL, Webster JRP, Bishop SM, Narwal R, van der Walle CF, Lu JR. Coadsorption of a Monoclonal Antibody and Nonionic Surfactant at the SiO 2/Water Interface. ACS Appl Mater Interfaces 2018; 10:44257-44266. [PMID: 30500160 DOI: 10.1021/acsami.8b16832] [Citation(s) in RCA: 3] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [What about the content of this article? (0)] [Affiliation(s)] [Abstract] [Key Words] [MESH Headings] [Track Full Text] [Subscribe] [Scholar Register] [Indexed: 06/09/2023]
Abstract
During the formulation of therapeutic monoclonal antibodies (mAbs), nonionic surfactants are commonly added to attenuate structural rearrangement caused by adsorption/desorption at interfaces during processing, shipping, and storage. We examined the adsorption of a mAb (COE-3) at the SiO2/water interface in the presence of pentaethylene glycol monododecyl ether (C12E5), polysorbate 80 (PS80-20EO), and a polysorbate 80 analogue with seven ethoxylates (PS80-7EO). Spectroscopic ellipsometry was used to follow COE-3 dynamic adsorption, and neutron reflection was used to determine interfacial structure and composition. Neither PS80-20EO nor C12E5 had a notable affinity for COE-3 or the interface under the conditions studied and thus did not prevent COE-3 adsorption. In contrast, PS80-7EO did coadsorb but did not influence the dynamic process or the equilibrated amount of absorbed COE-3. Near equilibration, COE-3 underwent structural rearrangement and PS80-7EO started to bind the COE-3 interfacial layer and subsequently formed a well-defined surfactant bilayer via self-assembly. The resultant interfacial layer comprised an inner mAb layer of about 70 Å thickness and an outer surfactant layer of a further 70 Å, with distinct transitional regions across the mAb-surfactant and surfactant-bulk water boundaries. Once formed, such interfacial layers were very robust and worked to prevent further mAb adsorption, desorption, and structural rearrangement. Such robust interfacial layers could be anticipated to exist for formulated mAbs stored in type II glass vials; further research is required to understand the behavior of these layers for siliconized glass syringes.
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Affiliation(s)
- Zongyi Li
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Fang Pan
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Ruiheng Li
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Elias Pambou
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Xuzhi Hu
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Sean Ruane
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Daniela Ciumac
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
| | - Peixun Li
- ISIS Neutron Facility , STFC , Chilton , Didcot OX11 0QZ , U.K
| | | | | | - Steven M Bishop
- MedImmune LLC , Gaithersburg , Maryland 20878 , United States
| | | | | | - Jian Ren Lu
- Biological Physics Laboratory, School of Physics and Astronomy , University of Manchester , Oxford Road, Schuster Building , Manchester M13 9PL , U.K
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