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Osorio HM, Martín S, López MC, Marqués-González S, Higgins SJ, Nichols RJ, Low PJ, Cea P. Electrical characterization of single molecule and Langmuir-Blodgett monomolecular films of a pyridine-terminated oligo(phenylene-ethynylene) derivative. BEILSTEIN JOURNAL OF NANOTECHNOLOGY 2015; 6:1145-57. [PMID: 26171291 PMCID: PMC4464395 DOI: 10.3762/bjnano.6.116] [Citation(s) in RCA: 5] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Subscribe] [Scholar Register] [Received: 12/16/2014] [Accepted: 04/13/2015] [Indexed: 05/27/2023]
Abstract
Monolayer Langmuir-Blodgett (LB) films of 1,4-bis(pyridin-4-ylethynyl)benzene (1) together with the "STM touch-to-contact" method have been used to study the nature of metal-monolayer-metal junctions in which the pyridyl group provides the contact at both molecule-surface interfaces. Surface pressure vs area per molecule isotherms and Brewster angle microscopy images indicate that 1 forms true monolayers at the air-water interface. LB films of 1 were fabricated by deposition of the Langmuir films onto solid supports resulting in monolayers with surface coverage of 0.98 × 10(-9) mol·cm(-2). The morphology of the LB films that incorporate compound 1 was studied using atomic force microscopy (AFM). AFM images indicate the formation of homogeneous, monomolecular films at a surface pressure of transference of 16 mN·m(-1). The UV-vis spectra of the Langmuir and LB films reveal that 1 forms two dimensional J-aggregates. Scanning tunneling microscopy (STM), in particular the "STM touch-to-contact" method, was used to determine the electrical properties of LB films of 1. From these STM studies symmetrical I-V curves were obtained. A junction conductance of 5.17 × 10(-5) G 0 results from the analysis of the pseudolinear (ohmic) region of the I-V curves. This value is higher than that of the conductance values of LB films of phenylene-ethynylene derivatives contacted by amines, thiols, carboxylate, trimethylsilylethynyl or acetylide groups. In addition, the single molecule I-V curve of 1 determined using the I(s) method is in good agreement with the I-V curve obtained for the LB film, and both curves fit well with the Simmons model. Together, these results not only indicate that the mechanism of transport through these metal-molecule-metal junctions is non-resonant tunneling, but that lateral interactions between molecules within the LB film do not strongly influence the molecule conductance. The results presented here complement earlier studies of single molecule conductance of 1 using STM-BJ methods, and support the growing evidence that the pyridyl group is an efficient and effective anchoring group in sandwiched metal-monolayer-metal junctions prepared under a number of different conditions.
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Affiliation(s)
- Henrry Marcelo Osorio
- Departamento de Química Física, Facultad de Ciencias, Universidad de Zaragoza, 50009 Zaragoza, Spain
- Instituto de Nanociencia de Aragón (INA), Edificio I+D, Campus Rio Ebro, Universidad de Zaragoza, C/Mariano Esquillor s/n, 50017 Zaragoza, Spain
- Laboratorio de Microscopias Avanzadas (LMA) C/Mariano Esquilor s/n, Campus Rio Ebro, 50018 Zaragoza, Spain
| | - Santiago Martín
- Departamento de Química Física, Facultad de Ciencias, Universidad de Zaragoza, 50009 Zaragoza, Spain
- Instituto de Ciencia de Materiales de Aragón (ICMA), Universidad de Zaragoza-CSIC, 50009 Zaragoza, Spain
| | - María Carmen López
- Departamento de Química Física, Facultad de Ciencias, Universidad de Zaragoza, 50009 Zaragoza, Spain
- Instituto de Nanociencia de Aragón (INA), Edificio I+D, Campus Rio Ebro, Universidad de Zaragoza, C/Mariano Esquillor s/n, 50017 Zaragoza, Spain
| | | | - Simon J Higgins
- Department of Chemistry, University of Liverpool, Crown Street, Liverpool L69 7ZD, United Kingdom
| | - Richard J Nichols
- Department of Chemistry, University of Liverpool, Crown Street, Liverpool L69 7ZD, United Kingdom
| | - Paul J Low
- Department of Chemistry, University of Durham, Durham DH1 3LE, United Kingdom
- School of Chemistry and Biochemistry, University of Western Australia, Crawley 6009, WA, Australia
| | - Pilar Cea
- Departamento de Química Física, Facultad de Ciencias, Universidad de Zaragoza, 50009 Zaragoza, Spain
- Instituto de Nanociencia de Aragón (INA), Edificio I+D, Campus Rio Ebro, Universidad de Zaragoza, C/Mariano Esquillor s/n, 50017 Zaragoza, Spain
- Laboratorio de Microscopias Avanzadas (LMA) C/Mariano Esquilor s/n, Campus Rio Ebro, 50018 Zaragoza, Spain
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Sun CL, Liao Q, Li T, Li J, Jiang JQ, Xu ZZ, Wang XD, Shen R, Bai DC, Wang Q, Zhang SX, Fu HB, Zhang HL. Rational design of small indolic squaraine dyes with large two-photon absorption cross section. Chem Sci 2014; 6:761-769. [PMID: 28936317 PMCID: PMC5590541 DOI: 10.1039/c4sc02165g] [Citation(s) in RCA: 45] [Impact Index Per Article: 4.1] [Reference Citation Analysis] [Abstract] [Track Full Text] [Download PDF] [Figures] [Journal Information] [Subscribe] [Scholar Register] [Received: 07/21/2014] [Accepted: 10/07/2014] [Indexed: 01/12/2023] Open
Abstract
Small organic dyes with large two-photon absorption (TPA) cross sections (δ) are more desirable in many applications compared with large molecules. Herein, we proposed a facile theoretical method for the fast screening of small organic molecules as potential TPA dyes. This method is based on a theoretical analysis to the natural transition orbitals (NTOs) directly associated with the TPA transition. Experimental results on the small indolic squaraine dyes (ISD) confirmed that their TPA cross sections is strongly correlated to the delocalization degree of the NTOs of the S2 excited states. Aided by this simple and intuitive method, we have successfully designed and synthesized a small indolic squaraine dye (ISD) with a remarkable δ value above 8000 GM at 780 nm. The ISD dye also exhibits a high singlet oxygen generation quantum yield about 0.90. The rationally designed TPA dye was successfully applied in both two-photon excited fluorescence cell imaging and in vivo cerebrovascular blood fluid tracing.
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Affiliation(s)
- Chun-Lin Sun
- State Key Laboratory of Applied Organic Chemistry (SKLAOC) , College of Chemistry and Chemical Engineering , Lanzhou University , Lanzhou 73000 , P. R. China .
| | - Qing Liao
- Beijing National Laboratory for Molecular Sciences (BNLMS) Institute of Chemistry , Chinese Academy of Sciences , Beijing 100190 , P. R. China
| | - Ting Li
- School of Life Sciences , Lanzhou University , Lanzhou 73000 , P. R. China
| | - Jun Li
- State Key Laboratory of Applied Organic Chemistry (SKLAOC) , College of Chemistry and Chemical Engineering , Lanzhou University , Lanzhou 73000 , P. R. China .
| | - Jian-Qiao Jiang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC) , College of Chemistry and Chemical Engineering , Lanzhou University , Lanzhou 73000 , P. R. China .
| | - Zhen-Zhen Xu
- Beijing National Laboratory for Molecular Sciences (BNLMS) Institute of Chemistry , Chinese Academy of Sciences , Beijing 100190 , P. R. China
| | - Xue-Dong Wang
- Beijing National Laboratory for Molecular Sciences (BNLMS) Institute of Chemistry , Chinese Academy of Sciences , Beijing 100190 , P. R. China
| | - Rong Shen
- School of Basic Medical Sciences , Lanzhou University , Lanzhou 730000 , P. R. China
| | - De-Cheng Bai
- School of Basic Medical Sciences , Lanzhou University , Lanzhou 730000 , P. R. China
| | - Qiang Wang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC) , College of Chemistry and Chemical Engineering , Lanzhou University , Lanzhou 73000 , P. R. China .
| | - Sheng-Xiang Zhang
- School of Life Sciences , Lanzhou University , Lanzhou 73000 , P. R. China
| | - Hong-Bing Fu
- Beijing National Laboratory for Molecular Sciences (BNLMS) Institute of Chemistry , Chinese Academy of Sciences , Beijing 100190 , P. R. China.,Department of Chemistry , Capital Normal University , Beijing 100048 , P. R. China
| | - Hao-Li Zhang
- State Key Laboratory of Applied Organic Chemistry (SKLAOC) , College of Chemistry and Chemical Engineering , Lanzhou University , Lanzhou 73000 , P. R. China .
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