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Dimension-Dependent Phenomenological Model of Excitonic Electric Dipole in InGaAs Quantum Dots. NANOMATERIALS 2022; 12:nano12040719. [PMID: 35215046 PMCID: PMC8876956 DOI: 10.3390/nano12040719] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.5] [Reference Citation Analysis] [Abstract] [Key Words] [Track Full Text] [Download PDF] [Figures] [Subscribe] [Scholar Register] [Received: 01/24/2022] [Revised: 02/13/2022] [Accepted: 02/18/2022] [Indexed: 12/22/2022]
Abstract
Permanent electric dipole is a key property for effective control of semiconductor quantum-dot-based sources of quantum light. For theoretical prediction of that, complex geometry-dependent quantum simulations are necessary. Here, we use k·p simulations of exciton transition in InGaAs quantum dots to derive a simple geometry-dependent analytical model of dipole. Our model, discussed here, enables reasonably good estimation of the electric dipole, caused in quantum dot by the elastic strain, including an externally induced one. Due to its apparent simplicity, not necessitating elaborate and time-consuming simulations, it might after experimental verification serve as a preferred choice for experimentalists enabling them to make quick estimates of built-in and induced electric dipole in quantum dots.
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Singer C, Goetz A, Prasad AS, Becker M, Rothhardt M, Skoff SM. Thermal tuning of a fiber-integrated Fabry-Pérot cavity. OPTICS EXPRESS 2021; 29:28778-28786. [PMID: 34615000 DOI: 10.1364/oe.433094] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Track Full Text] [Subscribe] [Scholar Register] [Received: 06/03/2021] [Accepted: 08/06/2021] [Indexed: 06/13/2023]
Abstract
Here, we present the thermal tuning capability of an alignment-free, fiber-integrated Fabry-Pérot cavity. The two mirrors are made of fiber Bragg gratings that can be individually temperature stabilized and tuned. We show the temperature tuning of the resonance wavelength of the cavity without any degradation of the finesse and the tuning of the individual stop bands of the fiber Bragg gratings. This not only permits for the cavity's finesse to be optimized post-fabrication but also makes this cavity applicable as a narrowband filter with a FWHM spectral width of 0.07 ± 0.02 pm and a suppression of more than -15 dB that can be wavelength tuned. Further, in the field of quantum optics, where strong light-matter interactions are desirable, quantum emitters can be coupled to such a cavity and the cavity effect can be reversibly omitted and re-established. This is particularly useful when working with solid-state quantum emitters where such a reference measurement is often not possible once an emitter has been permanently deposited inside a cavity.
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Gajjela RSR, Hendriks AL, Douglas JO, Sala EM, Steindl P, Klenovský P, Bagot PAJ, Moody MP, Bimberg D, Koenraad PM. Structural and compositional analysis of (InGa)(AsSb)/GaAs/GaP Stranski-Krastanov quantum dots. LIGHT, SCIENCE & APPLICATIONS 2021; 10:125. [PMID: 34127643 PMCID: PMC8203795 DOI: 10.1038/s41377-021-00564-z] [Citation(s) in RCA: 1] [Impact Index Per Article: 0.3] [Reference Citation Analysis] [Abstract] [Key Words] [Grants] [Track Full Text] [Figures] [Subscribe] [Scholar Register] [Received: 12/14/2020] [Revised: 05/12/2021] [Accepted: 05/24/2021] [Indexed: 06/12/2023]
Abstract
We investigated metal-organic vapor phase epitaxy grown (InGa)(AsSb)/GaAs/GaP Stranski-Krastanov quantum dots (QDs) with potential applications in QD-Flash memories by cross-sectional scanning tunneling microscopy (X-STM) and atom probe tomography (APT). The combination of X-STM and APT is a very powerful approach to study semiconductor heterostructures with atomic resolution, which provides detailed structural and compositional information on the system. The rather small QDs are found to be of truncated pyramid shape with a very small top facet and occur in our sample with a very high density of ∼4 × 1011 cm-2. APT experiments revealed that the QDs are GaAs rich with smaller amounts of In and Sb. Finite element (FE) simulations are performed using structural data from X-STM to calculate the lattice constant and the outward relaxation of the cleaved surface. The composition of the QDs is estimated by combining the results from X-STM and the FE simulations, yielding ∼InxGa1 - xAs1 - ySby, where x = 0.25-0.30 and y = 0.10-0.15. Noticeably, the reported composition is in good agreement with the experimental results obtained by APT, previous optical, electrical, and theoretical analysis carried out on this material system. This confirms that the InGaSb and GaAs layers involved in the QD formation have strongly intermixed. A detailed analysis of the QD capping layer shows the segregation of Sb and In from the QD layer, where both APT and X-STM show that the Sb mainly resides outside the QDs proving that Sb has mainly acted as a surfactant during the dot formation. Our structural and compositional analysis provides a valuable insight into this novel QD system and a path for further growth optimization to improve the storage time of the QD-Flash memory devices.
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Affiliation(s)
- Raja S R Gajjela
- Department of Applied Physics, Eindhoven University of Technology, 5612 AZ, Eindhoven, The Netherlands.
| | - Arthur L Hendriks
- Department of Applied Physics, Eindhoven University of Technology, 5612 AZ, Eindhoven, The Netherlands
| | - James O Douglas
- Department of Materials, University of Oxford, Parks Road, Oxford, OX1 3PH, UK
| | - Elisa M Sala
- Center for Nanophotonics, Institute for Solid State Physics, TechnischeUniversität Berlin, Hardenbergstr. 36, 10623, Berlin, Germany
- EPSRC National Epitaxy Facility, The University of Sheffield, North Campus, Broad Lane, Sheffield, S3 7HQ, UK
| | - Petr Steindl
- Department of Condensed Matter Physics, Faculty of Science, Masaryk University, Kotlářská267/2, 61137, Brno, Czech Republic
- Huygens-Kamerlingh Onnes Laboratory, Leiden University, P.O. Box 9504 2300 RA, Leiden, Netherlands
| | - Petr Klenovský
- Department of Condensed Matter Physics, Faculty of Science, Masaryk University, Kotlářská267/2, 61137, Brno, Czech Republic
- Czech Metrology Institute, Okružní 31, 63800, Brno, Czech Republic
| | - Paul A J Bagot
- Department of Materials, University of Oxford, Parks Road, Oxford, OX1 3PH, UK
| | - Michael P Moody
- Department of Materials, University of Oxford, Parks Road, Oxford, OX1 3PH, UK
| | - Dieter Bimberg
- Center for Nanophotonics, Institute for Solid State Physics, TechnischeUniversität Berlin, Hardenbergstr. 36, 10623, Berlin, Germany
- "Bimberg Chinese-German Center for Green Photonics" Changchun Institute of Optics, Fine Mechanics and Physics, Chinese Academy of Sciences at CIOMP, 13033, Changchun, China
| | - Paul M Koenraad
- Department of Applied Physics, Eindhoven University of Technology, 5612 AZ, Eindhoven, The Netherlands
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