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Books on the topic 'Interaction electron-phonon'

Author: Grafiati

Published: 4 June 2021

Last updated: 8 March 2025

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1

1933-, Challis L. J., ed. Electron-phonon interaction in low-dimensional structures. Oxford: Oxford University Press, 2003.

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2

Aynajian, Pegor. Electron-Phonon Interaction in Conventional and Unconventional Superconductors. Berlin, Heidelberg: Springer Berlin Heidelberg, 2011. http://dx.doi.org/10.1007/978-3-642-14968-9.

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3

service), SpringerLink (Online, ed. Electron-Phonon Interaction in Conventional and Unconventional Superconductors. Berlin, Heidelberg: Springer-Verlag Berlin Heidelberg, 2011.

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4

R, Baquero, ed. Manifestations of the electron-phonon interaction: Proceedings of the 2nd CINVESTAV Superconductivity Symposium, Tequisquiapan, Mexico, 2-6 November 1992. Singapore: World Scientific, 1994.

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5

Capelleti, Rosanna. Rare earths as a probe of environment and electron-phonon interaction in optical materials. New York: Nova Science Publishers, 2009.

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6

R, Baquero, ed. Electron-phonon interaction in oxide superconductors: Proceedings of the First CINVESTAV Superconductivity Symposium, Oaxtepec, Mexico, 11-14 December, 1990. Singapore: World Scientific, 1991.

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7

Kato, Takashi. Electron-phonon interactions in novel nanoelectronics. New York: Nova Science, 2009.

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8

Kasii͡an, A. I. Kineticheskie ėffekty v poluprovodnikakh razlichnoĭ razmernosti. Kishinev: "Shtiint͡sa", 1989.

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9

Nicholas, R. J. The magnetophonon effect. Oxford, England: Pergamon Press, 1985.

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10

Graja, Andrzej. Les interactions électron-électron et électron-phonon dans les systèmes unidimensionnels des sels de TCNQ: Nature et conséquences spectrales. Varsovie: Editions scientifiques de Pologne, 1985.

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11

I͡Anson, I. K. Atlas mikrokontaknykh spektrov ėlektron-fononnogo vzaimodeĭstvii͡a v metallakh: Spravochnik. Kiev: Nauk. dumka, 1986.

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12

Khotkevich, A. V., and I. K. Yanson. Atlas of Point Contact Spectra of Electron-Phonon Interactions in Metals. Boston, MA: Springer US, 1995. http://dx.doi.org/10.1007/978-1-4615-2265-2.

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13

Trallero-Giner, C. Long wave polar modes in semiconductor heterostructures. Oxford: Pergamon, 1998.

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14

Svistunov, V. M. Tunnelʹnai͡a︡ spektroskopii͡a︡ kvazichastichnykh vozbuzhdeniĭ v metallakh. Kiev: Nauk. dumka, 1986.

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15

Torres, C. M. Sotomayor, J. P. Leburton, and Jordi Pascual. Phonons in semiconductor nanostructures. Dordrecht: Springer, 1993.

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16

1949-, Leburton J. P., Pascual Jordi 1949-, Sotomayor Torres C. M, North Atlantic Treaty Organization. Scientific Affairs Division., and NATO Advanced Research Workshop on Phonons in Semiconductor Nanostructures (1992 : San Felíu de Guixols, Spain), eds. Phonons in semiconductor nanostructures. Dordrecht: Kluwer Academic, 1993.

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17

Tarasenko, A. A. Fluktuat͡s︡ii v obʺeme i na poverkhnosti tverdykh tel. Kiev: Nauk. dumka, 1992.

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18

A, Khon I͡U︡, and Institut fiziki prochnosti i materialovedenii͡a︡ (Akademii͡a︡ nauk SSSR), eds. Ėlektrony i fonony v neupori͡a︡dochennykh splavakh. Novosibirsk: "Nauka," Sibirskoe otd-nie, 1989.

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19

Howard, Colin. Measuring, Interpreting and Translating Electron Quasiparticle - Phonon Interactions on the Surfaces of the Topological Insulators Bismuth Selenide and Bismuth Telluride. Cham: Springer International Publishing, 2016. http://dx.doi.org/10.1007/978-3-319-44723-0.

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20

NATO Advanced Study Institute on the Physics of the Two-Dimensional Electron Gas (1986 Oostduinkerke, Belgium). The physics of the two-dimensional electron gas. New York: Plenum Press, 1987.

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21

Horing, Norman J. Morgenstern. Interacting Electron–Hole–Phonon System. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198791942.003.0011.

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Chapter 11 employs variational differential techniques and the Schwinger Action Principle to derive coupled-field Green’s function equations for a multi-component system, modeled as an interacting electron-hole-phonon system. The coupled Fermion Green’s function equations involve five interactions (electron-electron, hole-hole, electron-hole, electron-phonon, and hole-phonon). Starting with quantum Hamilton equations of motion for the various electron/hole creation/annihilation operators and their nonequilibrium average/expectation values, variational differentiation with respect to particle sources leads to a chain of coupled Green’s function equations involving differing species of Green’s functions. For example, the 1-electron Green’s function equation is coupled to the 2-electron Green’s function (as earlier), also to the 1-electron/1-hole Green’s function, and to the Green’s function for 1-electron propagation influenced by a nontrivial phonon field. Similar remarks apply to the 1-hole Green’s function equation, and all others. Higher order Green’s function equations are derived by further variational differentiation with respect to sources, yielding additional couplings. Chapter 11 also introduces the 1-phonon Green’s function, emphasizing the role of electron coupling in phonon propagation, leading to dynamic, nonlocal electron screening of the phonon spectrum and hybridization of the ion and electron plasmons, a Bohm-Staver phonon mode, and the Kohn anomaly. Furthermore, the single-electron Green’s function with only phonon coupling can be rewritten, as usual, coupled to the 2-electron Green’s function with an effective time-dependent electron-electron interaction potential mediated by the 1-phonon Green’s function, leading to the polaron as an electron propagating jointly with its induced lattice polarization. An alternative formulation of the coupled Green’s function equations for the electron-hole-phonon model is applied in the development of a generalized shielded potential approximation, analysing its inverse dielectric screening response function and associated hybridized collective modes. A brief discussion of the (theoretical) origin of the exciton-plasmon interaction follows.

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22

Aynajian, Pegor. Electron-Phonon Interaction in Conventional and Unconventional Superconductors. Springer Berlin / Heidelberg, 2013.

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23

Aynajian, Pegor. Electron-Phonon Interaction in Conventional and Unconventional Superconductors. Springer, 2011.

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24

Zhang, Han. Electron–Phonon Interaction and Lattice Dynamics in High Tc Superconductors. WORLD SCIENTIFIC, 2020. http://dx.doi.org/10.1142/11010.

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25

Han, Zhang. Electron-Phonon Interaction and Lattice Dynamics in High Tc Superconductors. World Scientific Publishing Co Pte Ltd, 2019.

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26

Janz, Siegfried Oskar. Regularization, electrical resistivity and the electron-phonon interaction in PdH r. 1985.

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27

Baquero, R. Electron-Phonon Interaction in Oxide Superconductors: Proceedings of the First Cinvestav Superconductivity Symposium. World Scientific Publishing Co Pte Ltd, 1991.

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28

Baquero, R. Electron-Phonon Interaction in Oxide Superconductors: Proceedings of the First CINVESTAV Superconductivity Symposium. World Scientific Publishing Co Pte Ltd, 1991.

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29

Challis, Lawrence. Electron-Phonon Interaction in Low-Dimensional Structures (Series on Semiconductor Science and Technology, 10). Oxford University Press, USA, 2003.

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30

Launay, Jean-Pierre, and Michel Verdaguer. The moving electron: electrical properties. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198814597.003.0003.

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The three basic parameters controlling electron transfer are presented: electronic interaction, structural change and interelectronic repulsion. Then electron transfer in discrete molecular systems is considered, with cases of inter- and intramolecular transfers. The semi-classical (Marcus—Hush) and quantum models are developed, and the properties of mixed valence systems are described. Double exchange in magnetic mixed valence entities is introduced. Biological electron transfer in proteins is briefly presented. The conductivity in extended molecular solids (in particular organic conductors) is tackled starting from band theory, with examples such as KCP, polyacetylene and TTF-TCNQ. It is shown that electron–phonon interaction can change the geometrical structure and alter conductivity through Peierls distortion. Another important effect occurs in narrow-band systems where the interelectronic repulsion plays a leading role, for instance in Mott insulators.

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31

Mexico) Cinvestav Superconductivity Symposium 1990 (Oaxtepec. Electron-Phonon Interaction in Oxide Superconductors: Proceedings of the First Cinvestav-Superconductivity Symposium : Oaxtepec, Mexico, 11-14 Decem. World Scientific Publishing Company, 1992.

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32

Baquero, Rafael. Manifestations of the Electron-Phonon Interaction: Proceedings of the 2nd Cinvestav Superconductivity Symposium : Tequisquiapan, Mexico 2-6 November. World Scientific Pub Co Inc, 1995.

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33

Riste, T. Electron-Phonon Interactions and Phase Transitions. Springer, 2013.

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34

Riste, T. Electron-Phonon Interactions and Phase Transitions. Springer, 2013.

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35

Kato, Takashi. Electron-Phonon Interactions in Novel Nanoelectronics. Nova Science Publishers, Incorporated, 2009.

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36

Riste, T. Electron-Phonon Interactions and Phase Transitions. Springer, 2013.

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37

Electron-phonon interactions in novel nanoelectronics. New York: Nova Science, 2009.

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38

Challis, Lawrence, ed. Electron-Phonon Interactions in Low-Dimensional Structures. Oxford University Press, 2003. http://dx.doi.org/10.1093/acprof:oso/9780198507321.001.0001.

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39

Electron Phonon Interactions: A Novel Semiclassical Approach. World Scientific Pub Co Inc, 1989.

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40

Electron Phonon Interactions: A Novel Semiclassified Approach. World Scientific Publishing Co Pte Ltd, 1989.

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41

Electron and Phonon Interactions: A Novel Semiclassical Approach. World Scientific Publishing Co Pte Ltd, 1989.

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42

Zhang, H. Mesoscopic Structures and Their Effects on High-Tc Superconductivity. Edited by A. V. Narlikar. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780198738169.013.12.

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This article presents the results of model calculations carried out to determine the mesoscopic structural features of high-temperature superconducting (HTS) crystal structures, and especially their characteristic high critical temperature (Tc) and anisotropy. The crystal structure of high-temperature superconductors (HTSc) is unique in having some mesoscopic features. For example, the structures of a majority of cuprite superconductors are comprised of two structural blocks, perovskite and rock salt, stacked along the c-direction. This article calculates the interaction between the perovskite and rock salt blocks in the form of combinative energy in order to elucidate the effects of mesoscopic structures on high-Tc superconductivity. Both X-ray diffraction and Raman spectroscopy show that a ‘fixed triangle’ exists in the samples under investigation. The article also examines the importance of electron–phonon coupling in high-Tc superconductors.

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43

Barrett, T. W. Energy Transfer Dynamics: Studies and Essays in Honor of Herbert Frohlich. Springer-Verlag, 1987.

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44

Alloy Dependence of Electron-Phonon Interactions in Double Barrier Structures. Storming Media, 1996.

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45

Khotkevich, A. V., Igor K. Yanson, and Randal C. Reinertson. Atlas of Point Contact Spectra of Electron-Phonon Interactions in Metals. Springer, 2011.

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46

Khotkevich, A. V., and Igor K. Yanson. Atlas of Point Contact Spectra of Electron-Phonon Interactions in Metals. Springer, 1994.

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47

Khotkevich, A. V., Igor K. Yanson, and Randal C. Reinertson. Atlas of Point Contact Spectra of Electron-Phonon Interactions in Metals. Springer, 2014.

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48

Yanson, Igor K., Randal C. Reinertson, and A. V. Khotkevich. Atlas of Point Contact Spectra of Electron-Phonon Interactions in Metals. Springer London, Limited, 2013.

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49

Atlas of point contact spectra of electron-phonon interactions in metals. Boston: Kluwer Academic, 1995.

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50

Trallero-Giner, C., R. Pérez-Alvarez, and F. García-Moliner. Long Wave Polar Modes in Semiconductor Heterostructures. Elsevier Science & Technology Books, 1998.

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