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Journal articles on the topic 'Photon drag effect'

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1

Shalygin, V. A., M. D. Moldavskaya, S. N. Danilov, I. I. Farbshtein, and L. E. Golub. "Circular photon drag effect in bulk semiconductors." Journal of Physics: Conference Series 864 (June 2017): 012072. http://dx.doi.org/10.1088/1742-6596/864/1/012072.

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2

Obraztsov, Alexander N., Dmitry A. Lyashenko, Shaoli Fang, et al. "Photon drag effect in carbon nanotube yarns." Applied Physics Letters 94, no. 23 (2009): 231112. http://dx.doi.org/10.1063/1.3151834.

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3

Rasulov, R. Ya, V. R. Rasulov, I. Eshboltaev, and N. Z. Mamadalieva. "Photon-Drag Effect in p-Type Tellurium." Russian Physics Journal 62, no. 6 (2019): 1082–89. http://dx.doi.org/10.1007/s11182-019-01818-5.

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4

Mikheev, Gennady M., Aleksandr S. Saushin, Viatcheslav V. Vanyukov, Konstantin G. Mikheev, and Yuri P. Svirko. "Femtosecond Circular Photon Drag Effect in the Ag/Pd Nanocomposite." Nanoscale Research Letters 12, no. 1 (2017): 39. https://doi.org/10.1186/s11671-016-1771-4.

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We report on the observation of the helicity-dependent photoresponse of the 20-μm-thick silver–palladium (Ag/Pd) nanocomposite films. In the experiment, 120 fs pulses of Ti:S laser induced in the film an electric current perpendicular to the incidence plane. The photoinduced current is a linear function of the incident beam power, and its sign depends on the beam polarization and angle of incidence. In particular, the current is zero for the <i>p</i>- and <i>s</i>-polarized beams, while its sign is opposite for the right- and left-circularly polarized beams. By comparing experimental results w
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5

Vasko, F. T. "Photon drag effect in tunnel-coupled quantum wells." Physical Review B 53, no. 15 (1996): 9576–78. http://dx.doi.org/10.1103/physrevb.53.9576.

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6

Nunes, O. A. C., D. A. Agrello, and A. L. A. Fonseca. "Low-temperature photon-drag effect in magnetic semiconductors." Physics Letters A 266, no. 4-6 (2000): 421–24. http://dx.doi.org/10.1016/s0375-9601(00)00055-4.

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7

Goff, John Eric, and W. L. Schaich. "Theory of the photon-drag effect in simple metals." Physical Review B 61, no. 15 (2000): 10471–77. http://dx.doi.org/10.1103/physrevb.61.10471.

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8

Rodrigues-Costa, C., and O. A. C. Nunes. "Theory of photon-drag effect in bulk magnetic semiconductors." Physical Review B 46, no. 23 (1992): 15046–52. http://dx.doi.org/10.1103/physrevb.46.15046.

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9

Mikheev, Gennady M., Albert G. Nasibulin, Ruslan G. Zonov, Antti Kaskela, and Esko I. Kauppinen. "Photon-Drag Effect in Single-Walled Carbon Nanotube Films." Nano Letters 12, no. 1 (2011): 77–83. http://dx.doi.org/10.1021/nl203003p.

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10

Luo, Qinghuan. "The Effect of Radiation Drag on Relativistic Bulk Flows in Active Galactic Nuclei." Publications of the Astronomical Society of Australia 19, no. 1 (2002): 122–24. http://dx.doi.org/10.1071/as01112.

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AbstractThe effect of radiation drag on relativistic bulk flows is re-examined. Highly relativistic bulk flows in the nuclear region are subject to Compton drag, i.e. radiation deceleration as a result of inverse Compton scattering of ambient soft photon fields from emission from the accretion disk, broad line region, or dusty torus. Possible observational consequences of X-/γ-ray emission produced from Compton drag are specifically discussed.
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11

Rodrigues, C., A. L. A. Fonseca, D. A. Agrello, and O. A. C. Nunes. "The phonon-assisted photon-drag effect in a two-dimensional semiconductor quantum-well structure." Superlattices and Microstructures 29, no. 1 (2001): 33–42. http://dx.doi.org/10.1006/spmi.2000.0909.

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12

Malyutenko, Volodymyr, Vitalii Borblik, and Victor Vainberg. "UP-conversion of terahertz radiation induced by photon drag effect." Physica E: Low-dimensional Systems and Nanostructures 20, no. 3-4 (2004): 563–66. http://dx.doi.org/10.1016/j.physe.2003.09.010.

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13

Luo, Qinghuan. "The Effect of Nonaxisymmetric Radiative Drag on Relativistic Jets in Active Galactic Nuclei." Publications of the Astronomical Society of Australia 18, no. 3 (2001): 215–20. http://dx.doi.org/10.1071/as01033.

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AbstractThe effect of nonaxisymmetric radiation drag on relativistic jets in active galactic nuclei (AGN) is discussed. The radiation force due to inverse Compton scattering of photon fields from a noncircular accretion disk is calculated. It is shown that such nonaxisymmetric drag can cause jet path distortion within the subparsec region of the black hole. This subparsec scale distortion is potentially observable with the current VLBI, VLBA techniques. Any modulation of the axially asymmetric distribution of disk emission can result in variability in electromagnetic radiation from the jet.
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14

Luryi, Serge. "Photon-Drag Effect in Intersubband Absorption by a Two-Dimensional Electron Gas." Physical Review Letters 58, no. 21 (1987): 2263–66. http://dx.doi.org/10.1103/physrevlett.58.2263.

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15

Załużny, M. "Resonant screening effect on the photon-drag current spectra in quantum wells." Solid State Communications 103, no. 8 (1997): 435–39. http://dx.doi.org/10.1016/s0038-1098(97)00225-1.

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16

A. Grinberg, Anatoly, and Serge Luryi. "Theory of the photon-drag effect in a two-dimensional electron gas." Physical Review B 38, no. 1 (1988): 87–96. http://dx.doi.org/10.1103/physrevb.38.87.

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17

Kastalsky, A. "Resonant photon-drag effect for interband absorption in a single quantum well." Solid State Communications 68, no. 10 (1988): 947–51. http://dx.doi.org/10.1016/0038-1098(88)90139-1.

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18

Torres, Jean-Manuel. "Nanosecond Optical Rectification and Photon Drag Effect in Nanocarbon Thin Films and Wires." Journal of Nanoelectronics and Optoelectronics 4, no. 2 (2009): 247–51. http://dx.doi.org/10.1166/jno.2009.1034.

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19

Lee, Hyun C. "On the photon-drag effect of photocurrent of surface states of topological insulators." Physica E: Low-dimensional Systems and Nanostructures 79 (May 2016): 44–51. http://dx.doi.org/10.1016/j.physe.2015.12.005.

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20

Mikheev, K. G., R. G. Zonov, D. L. Bulatov, A. E. Fateev, and G. M. Mikheev. "Laser-Induced Graphene on a Polyimide Film: Observation of the Photon Drag Effect." Technical Physics Letters 46, no. 5 (2020): 458–61. http://dx.doi.org/10.1134/s1063785020050119.

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21

Kimmitt, M. F., C. R. Pidgeon, D. A. Jaroszynski, R. J. Bakker, A. F. G. van der Meer, and D. Oepts. "Infrared free electron laser measurement of the photon drag effect in P-silicon." International Journal of Infrared and Millimeter Waves 13, no. 8 (1992): 1065–73. http://dx.doi.org/10.1007/bf01009051.

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22

Koch, J., and A. D. Wieck. "Photon-drag effect in a two-dimensional electron gas in high magnetic fields." Superlattices and Microstructures 25, no. 1-2 (1999): 143–48. http://dx.doi.org/10.1006/spmi.1998.0627.

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23

Chen, Jianbin, Hacer Koc, Shengkai Zhao, Kaiyu Wang, Lingfeng Chao, and Mustafa Eginligil. "Emerging Nonlinear Photocurrents in Lead Halide Perovskites for Spintronics." Materials 17, no. 8 (2024): 1820. http://dx.doi.org/10.3390/ma17081820.

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Lead halide perovskites (LHPs) containing organic parts are emerging optoelectronic materials with a wide range of applications thanks to their high optical absorption, carrier mobility, and easy preparation methods. They possess spin-dependent properties, such as strong spin–orbit coupling (SOC), and are promising for spintronics. The Rashba effect in LHPs can be manipulated by a magnetic field and a polarized light field. Considering the surfaces and interfaces of LHPs, light polarization-dependent optoelectronics of LHPs has attracted attention, especially in terms of spin-dependent photocu
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24

Zav’yalov, D. V., S. V. Kryuchkov, and E. I. Kukhar’. "Electron-photon drag effect in a semiconductor superlattice subjected to a high electric field." Semiconductors 41, no. 6 (2007): 704–7. http://dx.doi.org/10.1134/s1063782607060176.

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25

Woerdman, J. P. "Comment on ‘‘Photon-drag effect in intersubband absorption in a two-dimensional electron gas’’." Physical Review Letters 59, no. 14 (1987): 1624. http://dx.doi.org/10.1103/physrevlett.59.1624.

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26

Maysonnave, J., S. Huppert, F. Wang, et al. "Terahertz Generation by Dynamical Photon Drag Effect in Graphene Excited by Femtosecond Optical Pulses." Nano Letters 14, no. 10 (2014): 5797–802. http://dx.doi.org/10.1021/nl502684j.

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27

Shalygin, V. A., H. Diehl, Ch Hoffmann, et al. "Spin photocurrents and the circular photon drag effect in (110)-grown quantum well structures." JETP Letters 84, no. 10 (2007): 570–76. http://dx.doi.org/10.1134/s0021364006220097.

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28

Feitosa, M. I. M., and O. N. Mesquita. "Wall-drag effect on diffusion of colloidal particles near surfaces: A photon correlation study." Physical Review A 44, no. 10 (1991): 6677–85. http://dx.doi.org/10.1103/physreva.44.6677.

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29

Khichar, Vivek, Suresh C. Sharma, and Nader Hozhabri. "New features in the surface plasmon induced photon drag effect in noble metal thin films." Journal of Physics Communications 5, no. 5 (2021): 055005. http://dx.doi.org/10.1088/2399-6528/abfd42.

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30

Zhu, L., Y. Huang, Z. Yao, et al. "Enhanced polarization-sensitive terahertz emission from vertically grown graphene by a dynamical photon drag effect." Nanoscale 9, no. 29 (2017): 10301–11. http://dx.doi.org/10.1039/c7nr02227a.

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31

Mikheev, Konstantin G., Aleksandr S. Saushin, Ruslan G. Zonov, Albert G. Nasibulin, and Gennady M. Mikheev. "Photon-drag in single-walled carbon nanotube and silver-palladium films: the effect of polarization." Journal of Nanophotonics 10, no. 1 (2015): 012505. http://dx.doi.org/10.1117/1.jnp.10.012505.

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32

Van Oss, R. F., G. H. J. Van Den Oord, and M. Kuperus. "Accretion Disk Flares in Energetic Radiation Fields." Symposium - International Astronomical Union 157 (1993): 217–18. http://dx.doi.org/10.1017/s0074180900174157.

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We consider the physics of magnetic flares in the energetic radiation field of an accretion disk corona (ADC). The X-ray emission from these flares is thought to be responsable for the observed hard powerlaw component in the X-ray spectra of galactic black hole candidates in their ‘high’ spectral state. During the flare event (inverse Compton) scattering of soft photons from the underlying disk into hard photons occurs on accelerated electrons in current sheets. The electrons are decelerated by the radiation drag force that results from the up-scattering. This friction-like effect of the inten
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33

Krevchik, V. D., and A. V. Razumov. "Features of the electron-photon drag effect in a spiral ribbon in the external magnetic field." Physics of the Solid State 53, no. 12 (2011): 2500–2503. http://dx.doi.org/10.1134/s1063783411120110.

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34

Михеев, К. Г., Р. Г. Зонов, Д. Л. Булатов, А. Е. Фатеев та Г. М. Михеев. "Лазерно-индуцированный графен на полиимидной пленке: наблюдение эффекта увлечения". Письма в журнал технической физики 46, № 9 (2020): 51. http://dx.doi.org/10.21883/pjtf.2020.09.49375.18152.

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Porous graphene film structures were produced by irradiation of polyimide film with focused continuous wave CO2 laser. Generation of nanosecond pulses of photocurrent was observed in the obtained structures upon excitation by nanosecond laser pulses in a wide range of wavelengths. It is shown that the photocurrent linearly increases with pulsed laser power and its dependence on the angle of light incidence on the film structure is symmetric about the origin. Wavelength dependence of light-to-photocurrent conversion coefficient was measured. The obtained results are explained by photon-drag eff
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35

Kropotov, Grigory, Vladimir Rogalin, and Ivan Kaplunov. "Germanium Single Crystals for Photonics." Crystals 14, no. 9 (2024): 796. http://dx.doi.org/10.3390/cryst14090796.

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Germanium (Ge) is a system-forming material of IR photonics for the atmospheric transparency window of 8–14 µm. For optics of the 3–5 µm range, more widespread silicon (Si), which has phonon absorption bands in the long-wave region, is predominantly used. A technology for growing Ge single crystals has been developed, allowing the production of precision optical parts up to 500 mm in diameter. Ge is used primarily for the production of transparent optical parts for thermal imaging devices in the 8–14 µm range. In addition, germanium components are widely used in a large number of optical devic
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36

Ochiai, Tetsuyuki. "Enhanced second-harmonic generation and photon drag effect in a doped graphene placed on a two-dimensional diffraction grating." Journal of the Optical Society of America B 34, no. 4 (2017): 740. http://dx.doi.org/10.1364/josab.34.000740.

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37

Solanki, Reena, and Seema Agrawal. "Thermoelectric Properties of Zn Nanowires: Phonon Scattering Effect." Research Journal of Chemistry and Environment 26, no. 5 (2022): 114–18. http://dx.doi.org/10.25303/2605rjce114118.

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The temperature-dependent thermoelectric power (S) of Zn nanostructures is numerically estimated using a theoretical model. The electron diffusive and phonon drag contributions to thermoelectric power are calculated within the relaxation time approximation. The phonon drag thermopower is an artifact of various operating scattering mechanisms. The anomalous behavior of (S) is successfully estimated in accordance with interaction of heat carrying phonons with impurity, grain boundaries, electrons and phonons. The scattering and transport cross sections are function of phonon frequency  in the p
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38

Zhou, Jiawei, Bolin Liao, Bo Qiu, et al. "Ab initio optimization of phonon drag effect for lower-temperature thermoelectric energy conversion." Proceedings of the National Academy of Sciences 112, no. 48 (2015): 14777–82. http://dx.doi.org/10.1073/pnas.1512328112.

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Although the thermoelectric figure of merit zT above 300 K has seen significant improvement recently, the progress at lower temperatures has been slow, mainly limited by the relatively low Seebeck coefficient and high thermal conductivity. Here we report, for the first time to our knowledge, success in first-principles computation of the phonon drag effect—a coupling phenomenon between electrons and nonequilibrium phonons—in heavily doped region and its optimization to enhance the Seebeck coefficient while reducing the phonon thermal conductivity by nanostructuring. Our simulation quantitative
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39

Kuleyev I. G. and Kuleyev I. I. "The Effect of phonon focusing on the mutual drag of electrons and phonons and the electrical resistance of potassium." Physics of the Solid State 64, no. 8 (2022): 901. http://dx.doi.org/10.21883/pss.2022.08.54601.324.

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The effect influence of elastic energy anisotropy on the mutual drag of electrons and phonons and the electrical resistance of potassium crystals at low temperatures have investigated. We have analyzed the momentum exchange between the electron and three phonon flows corresponding to three branches of the vibrational spectrum in the hydrodynamic approximation. The actual mechanisms of phonon momentum relaxation have taken into account: scattering at sample boundaries, dislocations, and in the processes of phonon-phonon transfer. It have shown that in the limiting case of strong mutual drag of
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40

Suresha, Kasala. "Phonon Drag Thermopower in Silicene in Equipartition Regime at Room Temperature." International Journal for Research in Applied Science and Engineering Technology 9, no. 11 (2021): 399–403. http://dx.doi.org/10.22214/ijraset.2021.38818.

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Abstract: Similar to graphene, zero band gap limits the application of Silicene in nanoelectronics despite of its high carrier mobility. In this article we calculate the contribution of electron-phonon interaction to thermoelectric effects in silicene. One considers the case of free standing silicene taking into account interaction with intrinsic acoustic phonons. The temperature considered here is at room temperature. We noticed that the contribution to thermoelectromotive force due to electron drag by phonons is determined by the Fermi energy. The explicit temperature dependence of the contr
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41

Кулеев, И. Г., та И. И. Кулеев. "Влияние фокусировки на взаимное увлечение электронов и фононов и электросопротивление кристаллов калия". Физика твердого тела 64, № 8 (2022): 899. http://dx.doi.org/10.21883/ftt.2022.08.52680.324.

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The effect influence of elastic energy anisotropy on the mutual drag of electrons and phonons and the electrical resistance of potassium crystals at low temperatures have investigated. We have analyzed the momentum exchange between the electron and three phonon flows corresponding to three branches of the vibrational spectrum in the hydrodynamic approximation. The actual mechanisms of phonon momentum relaxation have taken into account: scattering at sample boundaries, dislocations, and in the processes of phonon-phonon transfer. It have shown that in the limiting case of strong mutual drag of
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42

Seminozhenko, V. P., and S. E. Shafranyuk. "Effect of an external electromagnetic field on electron drag of dislocations." Soviet Journal of Low Temperature Physics 13, no. 7 (1987): 430–31. https://doi.org/10.1063/10.0031741.

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The effect of an external electromagnetic field on the electron drag of dislocations under conditions of multiphoton absorption at low temperatures is studied. It is shown that a randomly polarized field with frequency Ω ≫ ωq (ωq is the frequency of the dislocation phonon), changing the character of the interaction of the dislocation phonons with current carriers, also changes the friction between the dislocations and the electron gas.
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43

Shkorbatov, A. G., and T. Z. Sarkisyants. "Phonon–phonon relaxation and thermoelectric effects in point contacts." Soviet Journal of Low Temperature Physics 16, no. 6 (1990): 427–34. https://doi.org/10.1063/10.0032634.

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The contribution of phonon-phonon scattering to point-contact thermoelectric effects (quenching of phonon drag thermo-emf and asymmetry in heat release in a symmetric point contact) is considered. The effective lengths of phonon relaxation due to normal processes lNc and umklapp processes lUc in the point contact are calculated for d≪lNc,lUc (d is the contact diameter). If the main relaxation mechanism is the nonelectron scattering of phonons of length lph, the quantities describing point-contact thermoelectric effects contain the parameter lph/lph-e (lph-e is the phonon-electron scattering le
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44

Pokharel, Mani, Huaizhou Zhao, Kevin Lukas, Zhifeng Ren, Cyril Opeil, and Bogdan Mihaila. "Phonon drag effect in nanocomposite FeSb2." MRS Communications 3, no. 1 (2013): 31–36. http://dx.doi.org/10.1557/mrc.2013.7.

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45

Lopez-Castillo, J. M., A. Amara, S. Jandl, J. P. Jay-Gerin, C. Ayache, and M. J. Aubin. "Phonon-drag effect inTiSe2−xSxmixed compounds." Physical Review B 36, no. 8 (1987): 4249–53. http://dx.doi.org/10.1103/physrevb.36.4249.

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46

Arkhipov, Alexander, Karina Trofimovich, Nikolay Arkhipov, and Pavel Gabdullin. "Phonon Drag Contribution to Thermopower for a Heated Metal Nanoisland on a Semiconductor Substrate." Nanomaterials 14, no. 20 (2024): 1684. http://dx.doi.org/10.3390/nano14201684.

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The possible contribution of phonon drag effect to the thermoelectrically sustained potential of a heated nanoisland on a semiconductor surface was estimated in a first principal consideration. We regarded electrons and phonons as interacting particles, and the interaction cross-section was derived from the basic theory of semiconductors. The solution of the equation of motion for average electrons under the simultaneous action of phonon drag and electric field gave the distributions of phonon flux, density of charge carriers and electric potential. Dimensional suppression of thermal conductan
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47

Condrea, Elena. "Strain influence on the diffusion thermopower in Bi wires." Moldavian Journal of the Physical Sciences 3-4(17) (December 15, 2018): 154–60. https://doi.org/10.5281/zenodo.4019250.

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We present the results of studies of the thermopower in glass-coated Bi wires under the action of uniaxial deformation. At the liquid helium temperature, thin Bi wires exhibit large positive thermopower values, which are dominated by the diffusive transport mechanism of holes. The observed increase in the negative contribution to total thermopower under uniaxial strain testifies that the hole-dominated transport can be transformed into the electron-dominated transport. The observed trend to negative thermopower values under strain can be attributed partially to a slight increase in the electro
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48

Wu, M. W., N. J. M. Horing, and H. L. Cui. "Phonon-drag effects on thermoelectric power." Physical Review B 54, no. 8 (1996): 5438–43. http://dx.doi.org/10.1103/physrevb.54.5438.

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49

Lehmann, D., Cz Jasiukiewicz, R. E. Strickland, K. R. Strickland, A. J. Kent, and T. Paszkiewicz. "Phonon-drag effect in 2D hole gases." Physica B: Condensed Matter 219-220 (April 1996): 25–27. http://dx.doi.org/10.1016/0921-4526(95)00638-9.

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50

Lyapilin, Igor, and Mikhail Okorokov. "THE INFLUENCE OF “INJECTED” AND “THERMAL” MAGNONS ON A SPIN WAVE CURRENT AND DRAG EFFECT IN HYBRID STRUCTURES." EPJ Web of Conferences 185 (2018): 01022. http://dx.doi.org/10.1051/epjconf/201818501022.

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The formation of the two: injected and thermally excited, different in energies magnon subsystems and the influence of its interaction with phonons and between on drag effect under spin Seebeck effect conditions in the magnetic insulator part of the metal/ferromagnetic insulator/metal structure is studied. The analysis of the macroscopic momentum balance equations of the systems of interest conducted for different ratios of the drift velocities of the magnon and phonon currents show that the injected magnons relaxation on the thermal ones is possible to be dominant over its relaxation on phono
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