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Journal articles on the topic 'Coupled quantum well photodiodes; Excitons'

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1

Zrenner, A., P. Leeb, J. Schäfer, G. Böhm, G. Weimann, J. M. Worlock, L. T. Florez, and J. P. Harbison. "Indirect excitons in coupled quantum well structures." Surface Science 263, no. 1-3 (February 1992): 496–501. http://dx.doi.org/10.1016/0039-6028(92)90396-n.

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2

Stroucken, T., A. Knorr, P. Thomas, and S. W. Koch. "Coherent dynamics of radiatively coupled quantum-well excitons." Physical Review B 53, no. 4 (January 15, 1996): 2026–33. http://dx.doi.org/10.1103/physrevb.53.2026.

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3

Guo, C. L., K. K. Law, J. Stellato, L. A. Coldren, Y. J. Ding, S. Li, J. B. Khurgin, C. T. Law, and A. E. Kaplan. "Strong excitonic nonlinearity in a P-I-N photodiode incorporating narrow asymmetric coupled quantum wells." Optics Letters 16, no. 12 (June 15, 1991): 949. http://dx.doi.org/10.1364/ol.16.000949.

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4

Cruz, H. "Dynamics of indirect excitons in a coupled quantum-well pair." Journal of Applied Physics 113, no. 15 (April 21, 2013): 153706. http://dx.doi.org/10.1063/1.4801808.

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5

Vörös, Z., V. Hartwell, D. W. Snoke, L. Pfeiffer, and K. West. "Considerations on equilibration of two-dimensional excitons in coupled quantum well structures." Journal of Physics: Condensed Matter 19, no. 29 (June 11, 2007): 295216. http://dx.doi.org/10.1088/0953-8984/19/29/295216.

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6

Stone, R. J., J. G. Michels, S. L. Wong, C. T. Foxon, R. J. Nicholas, and A. M. Fox. "Detection of terahertz radiation by hot electron effects in coupled quantum well photodiodes." Applied Physics Letters 69, no. 23 (December 2, 1996): 3569–71. http://dx.doi.org/10.1063/1.117248.

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7

SNOKE, D. W., V. NEGOITA, D. HACKWORTH, and K. EBERL. "ANOMALOUS SPECTRAL SHIFTS OF INDIRECT EXCITONS IN COUPLED GaAs QUANTUM WELLS." International Journal of Modern Physics B 15, no. 28n30 (December 10, 2001): 3606–10. http://dx.doi.org/10.1142/s0217979201008251.

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We have studied the energy shifts of indirect excitons consisting of an electron in one quantum well and a hole in an adjacent quantum well. Several surprising effects occur: (1) a very strong blue shift with increasing intensity of resonant laser excitation, (2) a very strong red shift with weak magnetic field, and (3) very low-frequency (sub-Hz) fluctuations of the spectral position at high excitation density. We discuss the effect of screening by carriers excited in the substrate material.
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8

Chen, Y. J., Emil S. Koteles, B. S. Elman, and C. A. Armiento. "Effect of electric fields on excitons in a coupled double-quantum-well structure." Physical Review B 36, no. 8 (September 15, 1987): 4562–65. http://dx.doi.org/10.1103/physrevb.36.4562.

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9

Zhao, Q. X., T. Westgaard, B. O. Fimland, and K. Johannessen. "Acceptor-bound excitons in GaAs/AlxGa1−xAs symmetric coupled-double-quantum-well structures." Physical Review B 45, no. 19 (May 15, 1992): 11346–49. http://dx.doi.org/10.1103/physrevb.45.11346.

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10

Panzarini, G., L. C. Andreani, A. Armitage, D. Baxter, M. S. Skolnick, J. S. Roberts, V. N. Astratov, M. A. Kaliteevski, A. V. Kavokin, and M. R. Vladimirova. "Polariton Dispersion and Polarisation Splitting for Quantum Well Excitons in Single and Coupled Microcavities." physica status solidi (a) 164, no. 1 (November 1997): 91–94. http://dx.doi.org/10.1002/1521-396x(199711)164:1<91::aid-pssa91>3.0.co;2-l.

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11

Toropov, A. A., I. V. Sedova, S. V. Sorokin, Ya V. Terent'ev, A. A. Sitnikova, O. V. Rykhova, and S. V. Ivanov. "Giant Zeeman Splitting of Excitons in a III–V Nonmagnetic Quantum Well Electronically Coupled With a II–VI Semimagnetic Quantum Well." Journal of Superconductivity 18, no. 3 (July 9, 2005): 339–44. http://dx.doi.org/10.1007/s10948-005-0003-4.

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12

KASAPOGLU, E., M. GUNES, H. SARI, and I. SÖKMEN. "BARRIER THICKNESS DEPENDENCE OF OPTICAL ABSORPTION OF EXCITONS IN GaAs COUPLED QUANTUM WIRE." Surface Review and Letters 11, no. 01 (February 2004): 49–55. http://dx.doi.org/10.1142/s0218625x04005810.

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We have calculated the binding energy of excitons, and the interband optical absorption in rectangular coupled quantum-well wires of GaAs surrounded by Ga 1-x Al x As in effective-mass approximation, using the variational approach. Results obtained show that the exciton binding energies and optical absorption depend on the sizes of the wire and barrier thickness. To the best of our knowledge the exciton binding energy and interband optical absorption in the rectangular coupled quantum wires have not been clarified yet.
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13

Haas, S., T. Stroucken, M. Hübner, J. Kuhl, B. Grote, A. Knorr, F. Jahnke, S. W. Koch, R. Hey, and K. Ploog. "Intensity dependence of superradiant emission from radiatively coupled excitons in multiple-quantum-well Bragg structures." Physical Review B 57, no. 23 (June 15, 1998): 14860–68. http://dx.doi.org/10.1103/physrevb.57.14860.

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14

THANH, NGO VAN, and NGUYEN AI VIET. "THEORY OF INTERFACE EXCITON WITH A HOLE CONFINED IN A QUANTUM WELL." Modern Physics Letters B 20, no. 23 (October 10, 2006): 1453–60. http://dx.doi.org/10.1142/s0217984906011773.

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We develop a simple model of the interface exciton with an electron strongly confined in the interface plane and a hole confined in the quantum well. The main parameters of the theory are: the distance d between the interface plane and center of the quantum well, and the parameters of quantum well (the half-width a and the height V0). Using the variational method, we obtained the binding energy and effective optical efficiency of this type of interface exciton. This model can be developed to investigate the properties of two-dimensional excitons in coupled quantum well.1
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15

NGO, VAN THANH, and AI VIET NGUYEN. "EFFECTS OF A STRONG MAGNETIC FIELD ON INTERFACE EXCITON WITH A HOLE CONFINED IN A QUANTUM WELL." International Journal of Modern Physics B 20, no. 20 (August 10, 2006): 2921–30. http://dx.doi.org/10.1142/s0217979206034923.

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We study by the variational method the effects of external magnetic field on the interface exciton with a hole confined in the quantum well. The main parameters of our model are: the distance d between the interface plane and center of the quantum well, the parameters of quantum well (the half width a and the height V0) and magnetic length λ. We obtained the binding energy and effective optical efficiency of this type of interface exciton. This model can be developed to investigate the properties of two-dimensional excitons in coupled quantum well.1
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16

CUNNINGHAM, J. E. "RECENT DEVELOPMENTS AND APPLICATIONS IN ELECTROABSORPTION SEMICONDUCTOR MODULATORS." Journal of Nonlinear Optical Physics & Materials 04, no. 02 (April 1995): 363–400. http://dx.doi.org/10.1142/s0218863595000161.

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State-of-the-art developments in electroabsorption modulators that utilize quantum well-semiconductors are reviewed. Optimized Multiple Quantum Well modulators in the GaAs/AlGaAs system have been driven by applications in photonic switching and optical interconnects. Surprisingly, these same structures exhibit a wealth of new behavior that ranges from Bloch oscillations to excitons in Coupled Well, Wannier–Stark and Shallow Well superlattices. Several types of excitonic phases have been identified optically and found to transform as the system dimensionality changes from 2D to 3D. In addition, new material systems have shown that quantum well excitonic absorption quality can be transferred to technologically important wavelengths at 1.06 μm or 1.55 μm.
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17

Кособукин, В. А. "Кулоновские плазмон-экситоны в планарных наноструктурах металл-полупроводник." Физика твердого тела 63, no. 4 (2021): 527. http://dx.doi.org/10.21883/ftt.2021.04.50720.248.

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A theory of Coulomb (non-radiative) plasmons-excitons in a semiconductor with adjacent quantum well and ultrathin metal film is presented. The equations of motion are formulated for the polarization waves of surface plasmons and quasi-two-dimensional excitons with taking account of Coulomb interaction between them. Within a model of coupled harmonic oscillators, solved are the problems of Coulomb plasmon, exciton and plasmon-exciton excitations in the presence of an external dipole force. The coupling contant is calculated for plasmon-excitons, their optical spectra are investigated, and the relative contributions of plasmons and excitons to the normal modes are found. It is concluded that near the resonance between plasmon and exciton the spectrum of plasmon-exciton excitations consists of two peaks whose behavior in passing through the resonance shows the signs of anti-crossing effect (repulsion of frequencies).
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18

Кособукин, В. А. "Кулоновские плазмон-экситоны в планарных наноструктурах металл-полупроводник." Физика твердого тела 63, no. 4 (2021): 527. http://dx.doi.org/10.21883/ftt.2021.04.50720.248.

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A theory of Coulomb (non-radiative) plasmons-excitons in a semiconductor with adjacent quantum well and ultrathin metal film is presented. The equations of motion are formulated for the polarization waves of surface plasmons and quasi-two-dimensional excitons with taking account of Coulomb interaction between them. Within a model of coupled harmonic oscillators, solved are the problems of Coulomb plasmon, exciton and plasmon-exciton excitations in the presence of an external dipole force. The coupling contant is calculated for plasmon-excitons, their optical spectra are investigated, and the relative contributions of plasmons and excitons to the normal modes are found. It is concluded that near the resonance between plasmon and exciton the spectrum of plasmon-exciton excitations consists of two peaks whose behavior in passing through the resonance shows the signs of anti-crossing effect (repulsion of frequencies).
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19

Bitton, Ora, Satyendra Nath Gupta, and Gilad Haran. "Quantum dot plasmonics: from weak to strong coupling." Nanophotonics 8, no. 4 (February 23, 2019): 559–75. http://dx.doi.org/10.1515/nanoph-2018-0218.

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AbstractThe complementary optical properties of surface plasmon excitations of metal nanostructures and long-lived excitations of semiconductor quantum dots (QDs) make them excellent candidates for studies of optical coupling at the nanoscale level. Plasmonic devices confine light to nanometer-sized regions of space, which turns them into effective cavities for quantum emitters. QDs possess large oscillator strengths and high photostability, making them useful for studies down to the single-particle level. Depending on structure and energy scales, QD excitons and surface plasmons (SPs) can couple either weakly or strongly, resulting in different unique optical properties. While in the weak coupling regime plasmonic cavities (PCs) mostly enhance the radiative rate of an emitter, in the strong coupling regime the energy level of the two systems mix together, forming coupled matter-light states. The interaction of QD excitons with PCs has been widely investigated experimentally as well as theoretically, with an eye on potential applications ranging from sensing to quantum information technology. In this review we provide a comprehensive introduction to this exciting field of current research, and an overview of studies of QD-plasmon systems in the weak and strong coupling regimes.
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20

LI, C. M., Y. N. CHEN, C. W. LUO, J. Y. HSIEH, and D. S. CHUU. "W STATE GENERATION AND EFFECT OF CAVITY PHOTONS ON THE PURIFICATION OF DOT-LIKE SINGLE QUANTUM WELL EXCITONS." International Journal of Quantum Information 03, supp01 (November 2005): 111–22. http://dx.doi.org/10.1142/s0219749905001298.

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A scheme of three-particle entanglement purification is presented in this work. The physical system undertaken for investigation is dot-like single quantum well excitons independently coupled through a single microcavity mode. The theoretical framework for the proposed scheme is based on the quantum jump approach for analyzing the progress of the trible-exciton entanglement as a series of conditional measurement has been taken on the cavity field state. We first investigate how cavity photon affects the purity of the double-exciton state and the purification efficiency in two-particle protocol. Then we extend the two-particle case and conclude that the three-exciton state can be purified into W state, which involves the one-photon-trapping phenomenon, with a high yield. Finally, an achievable setup for purification using only modest and presently feasible technologies is also proposed.
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21

Lokot, Lyubov E. "Particle-hole pair and beelectron states in ZnO/(Zn,Mg)O quantum wells and Dirac materials." JOURNAL OF ADVANCES IN PHYSICS 10, no. 1 (August 5, 2015): 2583–604. http://dx.doi.org/10.24297/jap.v10i1.1344.

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In this paper a theoretical studies of the space separation of electron and hole wave functions in the quantum well ZnO/Mg(0.27)Zn(0.73)O are presented. For this aim the self-consistent solution of the Schrödinger equations for electrons and holes and the Poisson equations at the presence of spatially varying quantum well potential due to the piezoelectric effect and local exchange-correlation potential is found. The one-dimensional Poisson equation contains the Hartree potential which includes the one-dimensional charge density for electrons and holes along the polarization field distribution. The three-dimensional Poisson equation contains besides the one-dimensional charge density for electrons and holes the exchange-correlation potential which is built on convolutions of a plane-wave part of wave functions in addition. The shifts of the Hartree valence band spectrums and the conduction band spectrum with respect to the flat band spectrums as well as the Hartree-Fock band spectrums with respect to the Hartree ones are found. An overlap integrals of the wave functions of holes and electron with taking into account besides the piezoelectric effects the exchange-correlation effects in addition is greater than an overlap integral of Hartree ones. The Hartree particles distribute greater on edges of quantum well than Hartree-Fock particles. It is found that an effective mass of heavy hole of Mg(0.27)Zn(0.73)O under biaxial strain is greater than an effective-mass of heavy hole of ZnO. It is calculated that an electron mass is less than a hole mass. It is found that the Bohr radius is grater than the localization range particle-hole pair, and the excitons may be spontaneously created.Schrödinger equation for pair of two massless Dirac particles when magnetic field is applied in Landau gauge is solved exactly. In this case the separation of center of mass and relative motion is obtained. Landau quantization $\epsilon=\pm\,B\sqrt{l}$ for pair of two Majorana fermions coupled via a Coulomb potential from massless chiral Dirac equation in cylindric coordinate is found. The root ambiguity in energy spectrum leads into Landau quantization for beelectron, when the states in which the one simultaneously exists are allowed. The tachyon solution with imaginary energy in Cooper problem ($\epsilon^{2}<0$) is found.
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22

Zhao, Q. X., P. O. Holtz, B. Monemar, B. O. Fimland, and K. Johannessen. "Optical Studies of free and Acceptor-Bound Excitons in GaAs/AlGaAs Symmetric Coupled Double Quantum Well Structures." MRS Proceedings 326 (January 1993). http://dx.doi.org/10.1557/proc-326-383.

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23

Ściesiek, Maciej, Krzysztof Sawicki, Wojciech Pacuski, Kamil Sobczak, Tomasz Kazimierczuk, Andrzej Golnik, and Jan Suffczyński. "Long-distance coupling and energy transfer between exciton states in magnetically controlled microcavities." Communications Materials 1, no. 1 (October 30, 2020). http://dx.doi.org/10.1038/s43246-020-00079-x.

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Abstract Coupling of quantum emitters in a semiconductor relies, generally, on short-range dipole-dipole or electronic exchange type interactions. Consistently, energy transfer between exciton states, that is, electron-hole pairs bound by Coulomb interaction, is limited to distances of the order of 10 nm. Here, we demonstrate polariton-mediated coupling and energy transfer between excitonic states over a distance exceeding 2 μm. We accomplish this by coupling quantum well-confined excitons through the delocalized mode of two coupled optical microcavities. Use of magnetically doped quantum wells enables us to tune the confined exciton energy by the magnetic field and in this way to control the spatial direction of the transfer. Such controlled, long-distance interaction between coherently coupled quantum emitters opens possibilities of a scalable implementation of quantum networks and quantum simulators based on solid-state, multi-cavity systems.
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24

Li, Jianyou, Arup Neogi, and Teruya Ishihara. "Resonant Energy Transfer due to Exciton Coupling in Hybrid Persovskites Conjugated to GaN Semiconductors." MRS Proceedings 955 (2006). http://dx.doi.org/10.1557/proc-0955-i15-07.

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ABSTRACTExciton-Exciton coupling in hybrid persovskites conjugated to GaN Semiconductors system has been studied. Excitons are strongly coupled in (C6H5C2H4NH3)2PbI4[bis(phenethyl-ammonium)tetraiodoplumbatel] (PEPI) is a hybrid inorganic-organic layered, with a perovskite structure quantum well (QW). The inorganic PbI4 monolayer is sandwiched between organic layers. The interaction between electron and hole forming the bound exciton is significantly stronger due to dielectric confinement. The lowest exciton binding energy is 220 meV, which is 20 times in comparison to GaAs. Gallium nitride (GaN) semiconductor has defect bound excitons with absorption band, which overlaps with the emission spectra of the PEPI system. This facilitates resonant energy transfer (RET) from the GaN defect bound exciton states to the excitons confined in the PEPI layer. We investigated the interaction by photoluminescence (PL) and found that 1s exciton in the PEPI layer strongly couples with the GaN defect level exciton, which is pronounced at lower temperature (< ∼ 100 K).
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