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Journal articles on the topic 'Polariton laser'

Author: Grafiati

Published: 4 June 2021

Last updated: 3 February 2022

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1

Wei, Cong, and Yong Sheng Zhao. "Electrically pumped polariton lasers." J. Mater. Chem. C 2, no. 13 (2014): 2295–97. http://dx.doi.org/10.1039/c3tc32427c.

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Exciton–polariton lasers under fermions injection: a condensation of exciton–polaritons was achieved in a microcavity sandwiched by two gradually doped distributed Bragg reflectors with electrical pumping. The polariton laser with an electron–polariton scattering process offers a platform to investigate the interaction between bosons and fermions and an effective way to generate coherent light.

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2

Dietrich, Christof P., Anja Steude, Laura Tropf, Marcel Schubert, Nils M. Kronenberg, Kai Ostermann, Sven Höfling, and Malte C. Gather. "An exciton-polariton laser based on biologically produced fluorescent protein." Science Advances 2, no. 8 (August 2016): e1600666. http://dx.doi.org/10.1126/sciadv.1600666.

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Under adequate conditions, cavity polaritons form a macroscopic coherent quantum state, known as polariton condensate. Compared to Wannier-Mott excitons in inorganic semiconductors, the localized Frenkel excitons in organic emitter materials show weaker interaction with each other but stronger coupling to light, which recently enabled the first realization of a polariton condensate at room temperature. However, this required ultrafast optical pumping, which limits the applications of organic polariton condensates. We demonstrate room temperature polariton condensates of cavity polaritons in simple laminated microcavities filled with biologically produced enhanced green fluorescent protein (eGFP). The unique molecular structure of eGFP prevents exciton annihilation even at high excitation densities, thus facilitating polariton condensation under conventional nanosecond pumping. Condensation is clearly evidenced by a distinct threshold, an interaction-induced blueshift of the condensate, long-range coherence, and the presence of a second threshold at higher excitation density that is associated with the onset of photon lasing.

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3

Ohtani, Keita, Bo Meng, Martin Franckié, Lorenzo Bosco, Camille Ndebeka-Bandou, Mattias Beck, and Jérôme Faist. "An electrically pumped phonon-polariton laser." Science Advances 5, no. 7 (July 2019): eaau1632. http://dx.doi.org/10.1126/sciadv.aau1632.

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We report a device that provides coherent emission of phonon polaritons, a mixed state between photons and optical phonons in an ionic crystal. An electrically pumped GaInAs/AlInAs quantum cascade structure provides intersubband gain into the polariton mode at λ = 26.3 μm, allowing self-oscillations close to the longitudinal optical phonon energy of AlAs. Because of the large computed phonon fraction of the polariton of 65%, the emission appears directly on a Raman spectrum measurement, exhibiting a Stokes and anti-Stokes component with the expected shift of 48 meV.

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4

Котова, Л. В., P. G. Savvidis, L. Besombes, and В. П. Кочерешко. "Поляритонные моды в цилиндрическом микрорезонаторе в режим поляритонного лазера." Физика твердого тела 63, no. 5 (2021): 610. http://dx.doi.org/10.21883/ftt.2021.05.50809.001.

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The spectra of exciton-polariton photoluminescence from cylindrical microcavities under optical excitation below and above the threshold of transition to the polariton laser regime under conditions of strong exciton-photon coupling were studied. At relatively weak optical excitation, lateral quantization modes of polaritons and whispering gallery modes appeared. Both the spectral distribution of these modes and the spatial dependence of their wave functions in the resonator plane were observed. With an increase in the excitation intensity and a transition to the polariton laser regime, only one, the longest-wavelength lasing line remained in the spectrum. It has been suggested that under strong optical excitation, the spectrum contains not only exciton-polariton radiation, but also trion-polariton radiation.

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5

Pile, David. "Organic polariton laser." Nature Photonics 4, no. 6 (June 2010): 402. http://dx.doi.org/10.1038/nphoton.2010.136.

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6

Moskalenko, S. A., and I. M. Tiginyanu. "Exciton-polariton laser." Low Temperature Physics 42, no. 5 (May 2016): 330–39. http://dx.doi.org/10.1063/1.4948615.

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7

Butov, Leonid V. "A polariton laser." Nature 447, no. 7144 (May 2007): 540–41. http://dx.doi.org/10.1038/447540a.

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8

Kavokin, Alexey, Guillaume Malpuech, and Fabrice P. Laussy. "Polariton laser and polariton superfluidity in microcavities." Physics Letters A 306, no. 4 (January 2003): 187–99. http://dx.doi.org/10.1016/s0375-9601(02)01579-7.

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9

Savvidis, Pavlos G. "A practical polariton laser." Nature Photonics 8, no. 8 (July 31, 2014): 588–89. http://dx.doi.org/10.1038/nphoton.2014.176.

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10

Harder, Tristan H., Meng Sun, Oleg A. Egorov, Ihor Vakulchyk, Johannes Beierlein, Philipp Gagel, Monika Emmerling, et al. "Coherent Topological Polariton Laser." ACS Photonics 8, no. 5 (April 14, 2021): 1377–84. http://dx.doi.org/10.1021/acsphotonics.0c01958.

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11

Архипов, Р. М., М. В. Архипов, В. С. Егоров, И. А. Чехонин, М. А. Чехонин, and С. Н. Багаев. "Излучение резонансной среды, возбуждаемое лазерным излучением с периодической фазовой модуляцией в режиме сильной связи поля и вещества." Журнал технической физики 127, no. 12 (2019): 967. http://dx.doi.org/10.21883/os.2019.12.48694.180-19.

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In this paper, the radiation of a two-level resonant medium placed in a cavity and excited by a laser pulse with periodic phase modulation is studied theoretically. The analysis is carried out on the basis of an analytical and numerical solution of the system of Maxwell-Bloch equations under conditions when the regime of strong coupling of the field and matter is realized. Under these conditions, this system is similar to a polariton laser. A high excitation efficiency of a polariton laser by a phase-modulated radiation pulse compared with a pulse without phase modulation of the carrier frequency is shown. It is shown that the main reason for the effective excitation of polariton modes of the medium is the occurrence of a difference combination parametric resonance. The results obtained open up new possibilities in the excitation of radiation from polariton lasers by low-power pumping laser radiation with frequency modulation.

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12

HUNSCHE, S., H. J. BAKKER, and H. KURZ. "TIME-RESOLVED STUDY OF PHONON-POLARITONS IN LiTaO3 AT ROOM TEMPERATURE." Modern Physics Letters B 07, no. 12 (May 20, 1993): 797–811. http://dx.doi.org/10.1142/s0217984993000783.

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We present a time-resolved study of phonon-polaritons in the ferroelectric LiTaO 3 at room temperature. The coherent generation and phase-sensitive detection of polaritons, using femtosecond Laser pulses, allow precise determination of polariton frequencies and dephasing times. The experimental data clearly show a resonance at 0.95 THz that has not been found in previous IR and Raman studies. The simultaneous coherent excitation of polaritons in the upper and the lower dispersion branch associated with this resonance leads to the observation of phonon-polariton beats, A quantum-mechanical model of the lowest A 1 lattice vibration in LiTaO 3 is developed, which provides a quantitative description of the low-frequency dielectric response, including the polariton dispersion and dephasing. Within this model, the transition at 0.95 THz can be identified as a classically forbidden tunneling resonance.

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13

Yamaguchi, Masashi, Minfeng Wang, and Pablo Suarez. "TERAHERTZ PHONON-POLARITON IMAGING FOR THE APPLICATION OF CHEMICAL DETECTION." International Journal of High Speed Electronics and Systems 17, no. 02 (June 2007): 355–65. http://dx.doi.org/10.1142/s0129156407004552.

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A combination of Terahertz (THz) polariton spectroscopy and polariton imaging technique for the application to chemical sensing is presented. We use phonon-polaritons, a coupled oscillation of the lattice vibration and radiation field, as an intense radiation source for THz spectroscopy. The propagation process of the polaritons generated in one of the two LiNbO 3 transducer crystals through the sample sandwiched between the crystals is visualized using a polariton imaging technique. Partially reflected polaritons at the transducer-sample interface and polaritons partially transmitted through the sample are visualized simultaneously in a single frame of an image. The temporal profile of reflected and transmitted phonon-polaritons can be obtained without scanning the delay time between the pump and probe femtosecond laser pulses unlike THz time-domain spectroscopy which requires point-by-point acquisition of the temporal pulse profile using conventional pump-probe scheme. The results suggest possible application of this technique to the chemical sensing with fast acquisition rate. The technique has been successfully applied to the measurement of liquid and solid samples, and simultaneous measurement of multiple samples has also been achieved.

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14

Schneider, Christian, Arash Rahimi-Iman, Na Young Kim, Julian Fischer, Ivan G. Savenko, Matthias Amthor, Matthias Lermer, et al. "An electrically pumped polariton laser." Nature 497, no. 7449 (May 2013): 348–52. http://dx.doi.org/10.1038/nature12036.

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15

Suárez-Forero, D. G., F. Riminucci, V. Ardizzone, M. De Giorgi, L. Dominici, F. Todisco, G. Lerario, et al. "Electrically controlled waveguide polariton laser." Optica 7, no. 11 (November 6, 2020): 1579. http://dx.doi.org/10.1364/optica.403558.

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16

Savage, Neil. "The practical polariton laser [News]." IEEE Spectrum 51, no. 8 (August 2014): 18. http://dx.doi.org/10.1109/mspec.2014.6866426.

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17

Kalozoumis, Panayotis A., and David Petrosyan. "Self-Organized PT-Symmetry of Exciton-Polariton Condensate in a Double-Well Potential." Applied Sciences 11, no. 16 (August 11, 2021): 7372. http://dx.doi.org/10.3390/app11167372.

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We investigate the dynamics and stationary states of a semiconductor exciton–polariton condensate in a double-well potential. We find that upon the population build-up of the polaritons by above-threshold laser pumping, coherence relaxation due to the phase fluctuations in the polaritons drives the system into a stable fixed point corresponding to a self-organized PT-symmetric phase.

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18

Maragkou, M., A. J. D. Grundy, T. Ostatnický, and P. G. Lagoudakis. "Longitudinal optical phonon assisted polariton laser." Applied Physics Letters 97, no. 11 (September 13, 2010): 111110. http://dx.doi.org/10.1063/1.3488012.

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19

Yukalov, V. I. "Inversion-polariton Filamentation in Laser Media." Journal of Modern Optics 35, no. 1 (January 1988): 35–48. http://dx.doi.org/10.1080/09500348814550101.

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20

Kenfack, S. C., C. M. Ekengoue, A. J. Fotué, F. C. Fobasso, G. N. Bawe, and L. C. Fai. "Laser cooling and trapping of polariton." Computational Condensed Matter 11 (June 2017): 47–54. http://dx.doi.org/10.1016/j.cocom.2017.05.001.

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21

Lozovik, Yurii E. "Strong correlations and new phases in an exciton - polariton system; the polariton laser." Uspekhi Fizicheskih Nauk 179, no. 3 (2009): 309. http://dx.doi.org/10.3367/ufnr.0179.200903k.0309.

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22

WEI Lai, 魏来, 李芳 LI Fang, and 周剑心 ZHOU Jian-xin. "Design of Surface Plasmon Polariton Nano-laser." ACTA PHOTONICA SINICA 45, no. 10 (2016): 1014004. http://dx.doi.org/10.3788/gzxb20164510.1014004.

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23

Malpuech, G., Y. G. Rubo, F. P. Laussy, P. Bigenwald, and A. V. Kavokin. "Polariton laser: thermodynamics and quantum kinetic theory." Semiconductor Science and Technology 18, no. 10 (September 3, 2003): S395—S404. http://dx.doi.org/10.1088/0268-1242/18/10/314.

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24

Kim, Seonghoon, Zhaorong Wang, Sebastian Brodbeck, Christian Schneider, Sven Höfling, and Hui Deng. "Monolithic High-Contrast Grating Based Polariton Laser." ACS Photonics 6, no. 1 (November 2, 2018): 18–22. http://dx.doi.org/10.1021/acsphotonics.8b01141.

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25

Laussy, Fabrice P., G. Malpuech, and A. Kavokin. "Spontaneous coherence buildup in a polariton laser." physica status solidi (c) 1, no. 6 (April 2004): 1339–50. http://dx.doi.org/10.1002/pssc.200304064.

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26

Кулаковский, В. Д., and А. А. Деменев. "Динамика когерентности экситон-поляритонной системы в GaAs-микрорезонаторах при импульсном резонансном фотовозбуждении." Физика и техника полупроводников 53, no. 10 (2019): 1343. http://dx.doi.org/10.21883/ftp.2019.10.48287.33.

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AbstractIt is found that exciton-polariton systems resonantly excited in GaAs semiconductor microcavities by coherent picosecond laser pulses inherit the high coherence of the laser beam and retain it for their lifetime (>100 ps), while the coherence-formation time in polariton systems resonantly excited by incoherent pulses without excitation of the exciton reservoir exceeds 200 ps.

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27

Иго, А. В. "Угловые зависимости интенсивности комбинационного рассеяния света на поляритонах в кристалле фосфида галлия." Журнал технической физики 127, no. 8 (2019): 225. http://dx.doi.org/10.21883/os.2019.08.48033.316-18.

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Raman scattering of light by phonons and polaritons in a sample of gallium phosphide was measured. For the excitation, a non-focused beam of a 532 nm single-mode laser was used. The collection of scattered radiation was carried out using a moving mirror of small diameter, which made it possible to measure the spectra of scattered light in the scattering angle range of 0.6o-8o with an angular total divergence of 0.4o. For different crystallographic directions, the intensities of the polarized components of the Raman scattered light were measured on longitudinal, transverse phonons and polaritons in the region of strong dispersion of the polariton branch for three fixed axial scattering angles. The components of scattering on longitudinal optical phonons and polaritons have a strong dependence on the crystallographic direction, as theory predicts, and the component of scattering on transverse optical phonons does not depend on the crystallographic direction. It was found that the intensity of scattering on transverse optical phonons correlates with the width of the spectral line of scattering on a polariton. A mechanism is proposed to explain this correlation.

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28

Деменев, А. А., Н. А. Гиппиус, and В. Д. Кулаковский. "Динамика спинорной экситон-поляритонной системы в латерально сжатых GaAs микрорезонаторах при резонансном фотовозбуждении." Физика твердого тела 60, no. 8 (2018): 1567. http://dx.doi.org/10.21883/ftt.2018.08.46245.06gr.

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AbstractThe evolution of the spatial coherence and the polarization has been studied in a freely decaying polariton condensate that is resonantly excited by linearly polarized picosecond laser pulses at the lower and upper sublevels of the lower polariton branch in a high-Q GaAs-based microcavity with a reduced lateral symmetry without excitation of the exciton reservoir. It is found that the condensate inherits the coherence of the exciting laser pulse at both sublevels in a wide range of excitation densities and retains it for several dozen picoseconds. The linear polarization of the photoexcited condensate is retained only in the condensate at the lower sublevel. The linearly polarized condensate excited at the upper sublevel loses its stability at the excitation densities higher a threshold value: it enters a regime of internal Josephson oscillations with strongly oscillating circular and diagonal linear degrees of polarization. The polariton–polariton interaction leads to the nonlinear Josephson effects at high condensate densities. All the effects are well described in terms of the spinor Gross–Pitaevskii equations. The cause of the polarization instability of the condensate is shown to be the spin anisotropy of the polariton–polariton interaction.

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29

Solnyshkov, Dmitry, Eleonora Petrolati, Aldo Di Carlo, and Guillaume Malpuech. "Theory of an electrically injected bulk polariton laser." Applied Physics Letters 94, no. 1 (January 5, 2009): 011110. http://dx.doi.org/10.1063/1.3067859.

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30

Baten, Md Zunaid, Pallab Bhattacharya, Thomas Frost, Saniya Deshpande, Ayan Das, Dimitri Lubyshev, Joel M. Fastenau, and Amy W. K. Liu. "GaAs-based high temperature electrically pumped polariton laser." Applied Physics Letters 104, no. 23 (June 9, 2014): 231119. http://dx.doi.org/10.1063/1.4883477.

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31

Wang, Zecheng, Xingyu Zhang, Zhenhua Cong, Zhaojun Liu, Xiaohan Chen, Zengguang Qin, Na Ming, and Quanxin Guo. "Tunable Stokes Laser Based on KTiOPO4 Crystal." Crystals 10, no. 11 (October 27, 2020): 974. http://dx.doi.org/10.3390/cryst10110974.

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The characteristics of a tunable Stokes laser based on the cascaded stimulated polariton scattering and stimulated Raman scattering in KTiOPO4 crystal were studied experimentally and theoretically. When the pumping wavelength was 1064 nm, the Stokes laser output wavelength was able to be tuned discontinuously from 1112.08 nm to 1113.64 nm, from 1114.94 nm to 1115.77 nm, and from 1117.37 nm to 1119.92 nm, and the maximum output power appeared at 1118.86 nm. With a pulse repetition frequency of 7 kHz and a pump power of 6.0 W, the maximum output power of the Stokes laser reached 734 mW, and the corresponding diode to laser conversion efficiency was 12.2%. The rate equations describing the temporal evolutions of the fundamental and Stokes waves by noncollinear stimulated polariton scattering and the Stokes wave by collinear stimulated Raman scattering were derived. They were used to simulate the tunable Stokes laser. The calculated results were in agreement with the experimental results on the whole.

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32

Черненко, А. В., А. С. Бричкин, С. И. Новиков, К. Шнайдер, and С. Хёфлинг. "Исследования конденсата поляритонов в микрорезонаторных микростолбиках в сильных магнитных полях -=SUP=-*-=/SUP=-." Физика и техника полупроводников 52, no. 1 (2018): 10. http://dx.doi.org/10.21883/ftp.2018.01.45311.35.

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AbstractThe photoluminescence of a nonequilibrium polariton condensate in cylindrical and rectangular micropillars etched on the surface of a high- Q GaAs microcavity is investigated in magnetic fields of up to 12 T. The measurements are carried out under different levels of nonresonant optical pumping with nanosecond laser pulses for a wide range of cavity detuning. As far as nonresonant excitation produces a high density of excitons in a reservoir, it should be expected that the exciton–polariton interaction, which depends on the pump level, has a considerable effect on the Zeeman splitting and polarization of the condensate. However, measurements of the Zeeman splitting and polarization in high magnetic fields demonstrate that only minor changes take place up to the highest available pump levels. This means that, in the case under study, the effect of exciton–polariton interaction on the polariton system is insignificant. At the same time, the data obtained provide an estimate for the exciton density in the reservoir. In contrast to cylindrical micropillars, the photoluminescence of the condensate in rectangular micropillars consists of two perpendicularly linearly polarized lines which retain a high degree of linear polarization even in a field as high as 12 T. The Zeeman splitting in this case is nearly independent of the pump power. The degrees of both circular and linear polarization change with pump power, but these changes are noticeably smaller than the ones predicted theoretically. This indicates that the system of polaritons in micropillars deviates considerably from thermodynamic equilibrium.

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33

Solnyshkov, D., and G. Malpuech. "A polariton laser based on a bulk GaN microcavity." Superlattices and Microstructures 41, no. 5-6 (May 2007): 279–83. http://dx.doi.org/10.1016/j.spmi.2007.03.013.

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34

Oh, Geum-Yoon, Hyungchan Kim, Jeong Beom Ko, Choon Keun Park, and Young-Wan Choi. "Design of a nanogap resonator surface plasmon polariton laser." Optics Letters 45, no. 11 (May 20, 2020): 2961. http://dx.doi.org/10.1364/ol.390868.

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35

Lee, Andrew J., and Helen M. Pask. "Cascaded stimulated polariton scattering in a Mg:LiNbO_3 terahertz laser." Optics Express 23, no. 7 (March 27, 2015): 8687. http://dx.doi.org/10.1364/oe.23.008687.

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36

Solnyshkov, D. D., T. Weiss, G. Malpuech, and N. A. Gippius. "Polariton laser based on a ZnO photonic crystal slab." Applied Physics Letters 99, no. 11 (September 12, 2011): 111110. http://dx.doi.org/10.1063/1.3639272.

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37

Estrecho, Eliezer. "Laser trapping and manipulation of exciton–polariton quantum fluids." Nature Reviews Physics 3, no. 8 (May 20, 2021): 536. http://dx.doi.org/10.1038/s42254-021-00333-2.

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38

Dusel, Marco, Simon Betzold, Tristan H. Harder, Monika Emmerling, Johannes Beierlein, Jürgen Ohmer, Utz Fischer, et al. "Room-Temperature Topological Polariton Laser in an Organic Lattice." Nano Letters 21, no. 15 (July 30, 2021): 6398–405. http://dx.doi.org/10.1021/acs.nanolett.1c00661.

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39

SHIRASAKA, Y., H. MINO, T. KAWAI, I. AKAI, and T. KARASAWA. "SPATIAL BEHAVIOR OF EXCITON-POLARITON MASSES IN A LAYERED CRYSTAL BiI3." International Journal of Modern Physics B 15, no. 28n30 (December 10, 2001): 3960–64. http://dx.doi.org/10.1142/s0217979201009104.

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Spatial behavior of the stacking fault excitons (SFE's) excited heavily in a two-dimensional space at a stacking fault interface in BiI 3 has been studied. The SFE's whose center-of-mass motion is confined at the interface show more efficient spatial expansion for higher excitation densities. In order to get phase information of the high-density SFE masses, the degnerate four-wave-mixing (DFWM) measurements with two laser beams including space-resolved regime were performed. It was found that the increase in the dephasing due to exciton-exciton collision is suppressed above a certain density. In a space-resolved regime, it turned out that the high-density exciton mass excited at one laser spot propagates coherently to the other laser-spot propagates coherently to the other laser-spot site and induces nonlinear polarization resulting in momentum-selective emission of the DFWM lights. These result suggest the possibility of a coherent collective motion of the SFE masses in a new condensate of the high-density exciton-polaritons.

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40

Walla, Frederik, Matthias M. Wiecha, Nicolas Mecklenbeck, Sabri Beldi, Fritz Keilmann, Mark D. Thomson, and Hartmut G. Roskos. "Anisotropic excitation of surface plasmon polaritons on a metal film by a scattering-type scanning near-field microscope with a non-rotationally-symmetric probe tip." Nanophotonics 7, no. 1 (January 1, 2018): 269–76. http://dx.doi.org/10.1515/nanoph-2017-0042.

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AbstractWe investigated the excitation of surface plasmon polaritons on gold films with the metallized probe tip of a scattering-type scanning near-field optical microscope (s-SNOM). The emission of the polaritons from the tip, illuminated by near-infrared laser radiation, was found to be anisotropic and not circularly symmetric as expected on the basis of literature data. We furthermore identified an additional excitation channel via light that was reflected off the tip and excited the plasmon polaritons at the edge of the metal film. Our results, while obtained for a non-rotationally-symmetric type of probe tip and thus specific for this situation, indicate that when an s-SNOM is employed for the investigation of plasmonic structures, the unintentional excitation of surface waves and anisotropic surface wave propagation must be considered in order to correctly interpret the signatures of plasmon polariton generation and propagation.

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41

Fedorenko, Leonid, and Arthur Medvid. "Laser-Induced Nano-Structuring of Semiconductors and Metals in near Surface Layers by Nanosecond Pulses." Advanced Materials Research 1117 (July 2015): 9–14. http://dx.doi.org/10.4028/www.scientific.net/amr.1117.9.

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It was established that irradiation of a semiconductor by nanosecond laser leads to drift of the impurity atoms. The direction of the drift depends on relation between covalent radius of the impurity and of the basic substance atoms. This effect was shown for a wide class of semiconductors, such as: Si, Ge, InSb, GaAs, CdTe, CdxZn1-xTe. This is due to a laser thermal shock effect connected with action of high temperature and pressure gradients formed by strong absorbed nanosecond laser pulse. A new concept was proposed, and the technology has been developed of laser-induced (YAG: Nd +3, wavelength l= 0.532 mm, pulse duration τp = 10 ns) nano-fragmentation of metal film, for example, Au with an average size of fragments <δ> = 80 nm, and the concentration on the surface <n> = 2.5×109 cm-2. The fragmentation is realized by the self organization of surface plasmon-polariton subsystem excited by high power laser pulses at a surface plasmon-polariton resonance. It was shown that the proposed method provides by laser-assisted fragmentation of the metal film (Au) in conditions of the resonance, decomposition of the nanofragments from the substrate, their transfer through an air gap, and implantation in a polymer layer on a separate surface at the same laser pulse.

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42

Jayaprakash, Rahul, Charles E. Whittaker, Kyriacos Georgiou, Onkar S. Game, Kirsty E. McGhee, David M. Coles, and David G. Lidzey. "Two-Dimensional Organic-Exciton Polariton Lattice Fabricated Using Laser Patterning." ACS Photonics 7, no. 8 (July 23, 2020): 2273–81. http://dx.doi.org/10.1021/acsphotonics.0c00867.

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43

Cotta, E. A., and F. M. Matinaga. "Self-oscillations in GaAs microcavity: Polariton and photon laser superposition." Solid State Communications 194 (September 2014): 10–15. http://dx.doi.org/10.1016/j.ssc.2014.06.004.

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Startsev, Aleksandr V., and Yurii Yu Stoilov. "On the nature of laser polariton tracks in soap films." Quantum Electronics 34, no. 6 (June 30, 2004): 569–71. http://dx.doi.org/10.1070/qe2004v034n06abeh002775.

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Qu, Yue, Shaocong Hou, and Stephen R. Forrest. "Temperature-Dependence of an Amorphous Organic Thin Film Polariton Laser." ACS Photonics 7, no. 4 (March 20, 2020): 867–72. http://dx.doi.org/10.1021/acsphotonics.9b01656.

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Kaliteevskii, M. A., and K. A. Ivanov. "Double-boson stimulated terahertz emission in a polariton cascade laser." Technical Physics Letters 39, no. 1 (January 2013): 91–94. http://dx.doi.org/10.1134/s1063785013010148.

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CHEN Yong-yi, 陈泳屹, 佟存柱 TONG Cun-zhu, 秦莉 QIN Li, 王立军 WANG Li-jun, and 张金龙 ZHANG Jin-long. "Progress in surface plasmon polariton nano-laser technologies and applications." Chinese Journal of Optics and Applied Optics 5, no. 5 (2012): 453–63. http://dx.doi.org/10.3788/co.20120505.0453.

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Glauser, M., G. Rossbach, G. Cosendey, J. Levrat, M. Cobet, J. F. Carlin, J. Besbas, et al. "Investigation of InGaN/GaN quantum wells for polariton laser diodes." physica status solidi (c) 9, no. 5 (April 12, 2012): 1325–29. http://dx.doi.org/10.1002/pssc.201100180.

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Schmutzler, J., F. Veit, M. Aßmann, J. S. Tempel, S. Höfling, M. Kamp, A. Forchel, and M. Bayer. "Determination of operating parameters for a GaAs-based polariton laser." Applied Physics Letters 102, no. 8 (February 25, 2013): 081115. http://dx.doi.org/10.1063/1.4794144.

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Cao, H., S. Pau, J. M. Jacobson, G. Björk, Y. Yamamoto, and A. Imamŏglu. "Transition from a microcavity exciton polariton to a photon laser." Physical Review A 55, no. 6 (June 1, 1997): 4632–35. http://dx.doi.org/10.1103/physreva.55.4632.

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