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1

Dobrovolʹskiĭ, V. N. Perenos ėlektronov i dyrok u poverkhnosti poluprovodnikov. Nauk. dumka, 1985.

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2

Gupta, Atam D. The electron-positron theory of the nucleus and the constructive role of black holes and of the neutrino and the antineutrino. A.D. Gupta, 1994.

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3

Norbury, John W. Symmetry considerations in the scattering of identical composite bodies. National Aeronautics and Space Administration, Scientific and Technical Information Branch, 1986.

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4

Isihara, Akira. Electron liquids. Springer-Verlag, 1993.

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5

Isihara, A. Electron liquids. 2nd ed. Springer, 1998.

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6

Isihara, Akira. Electron liquids. 2nd ed. Springer, 1998.

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7

Isihara, A. Electron liquids. Springer-Verlag, 1993.

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8

Sevortʹi︠a︡n, Anna. Shattering hopes: Post-election crackdown in Belarus. Human Rights Watch, 2011.

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9

Casati, Roberto. Holes and other superficialities. MIT Press, 1994.

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10

Administration, Bonneville Power. Lighting options for homes. Bonneville Power Administration, 1991.

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11

Dymond, Christopher. Oregon solar electric guide: Independent and utility-connected homes. 2nd ed. Oregon Office of Energy (625 Marion St. NE, Ste. 1, Salem, 97301-3742), 2003.

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12

Oregon. Dept. of Energy., ed. Oregon solar electric guide: Independent and utility-connected homes. Oregon Dept. of Energy, 2006.

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13

Leslie, Russell P. The lighting pattern book for homes. Lighting Research Center, 1993.

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14

J, Kenney Patrick, ed. No holds barred: Negativity in U.S. Senate campaigns. Pearson/Prentice Hall, 2004.

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15

Tsounakos, Othōn. Mauro ston Maurogialouro!: Mnēmes kai analōsima ap' holes tis vouleutikes ekloges tēs metapolemikēs periodou. Ekdoseis Hēliotropio, 2004.

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16

B, Fradkov A., ed. Opticheski vozbuzhdennye poluprovodniki pri nizkikh i sverkhnizkikh temperaturakh. "Nauka", 1988.

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17

Miller, Jan. Better homes and gardens better than mom's slow cooker recipes. Meredith Books, 2007.

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18

Matt, Sly, and Patrikios Jay, eds. Dear future me: Hopes, fears, secrets, resolutions. HOW Books, 2007.

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19

Jaworowski, Susan. Elected Hawaiian Homes commissioners?: Weighing the options after Rice. Legislative Reference Bureau, 2000.

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20

Agency, International Energy, ed. Cool appliances: Policy strategies for energy-efficient homes. OECD, 2003.

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21

Agency, International Energy, ed. Cool appliances: Policy strategies for energy-efficient homes. OECD, 2003.

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22

McKinley, Alan D. Home automation: A useful tool for improving the operation of homes. Canadian Automated Buildings Association, 1993.

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23

Administration, Bonneville Power. Field measurements of the heating efficiency of electric forced-air furnaces in six manufactured homes. Ecotope, 1994.

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24

Glazov, M. M. Hyperfine Interaction of Electron and Nuclear Spins. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0004.

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This chapter discusses the key interaction–hyperfine coupling–which underlies most of phenomena in the field of electron and nuclear spin dynamics. This interaction originates from magnetic interaction between the nuclear and electron spins. For conduction band electrons in III–V or II–VI semiconductors, it is reduced to a Fermi contact interaction whose strength is proportional to the probability of finding an electron at the nucleus. A more complex situation is realized for valence band holes where hole Bloch functions vanish at the nuclei. Here the hyperfine interaction is of the dipole–dip
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25

Glazov, M. M. Electron & Nuclear Spin Dynamics in Semiconductor Nanostructures. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.001.0001.

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In recent years, the physics community has experienced a revival of interest in spin effects in solid state systems. On one hand, solid state systems, particularly semicon- ductors and semiconductor nanosystems, allow one to perform benchtop studies of quantum and relativistic phenomena. On the other hand, interest is supported by the prospects of realizing spin-based electronics where the electron or nuclear spins can play a role of quantum or classical information carriers. This book aims at rather detailed presentation of multifaceted physics of interacting electron and nuclear spins in sem
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26

Opticheskie i kineticheskie ėffekty v neravnovesnykh ėlektronnykh i ėlektron-kolebatelʹnykh sistemakh. "Shtiint͡s︡a", 1986.

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27

Magnus, Wim, and Wim Schoenmaker. Quantum Transport in Sub-Micron Devices. Springer, 2002.

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28

Magnus, Wim, and Wim Schoenmaker. Quantum Transport in Submicron Devices: A Theoretical Introduction. Springer London, Limited, 2012.

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29

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 s
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30

Hirohata, A., and J. Y. Kim. Optically Induced and Detected Spin Current. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198787075.003.0006.

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This chapter presents an alternative method of injecting spin-polarized electrons into a nonmagnetic semiconductor through photoexcitation. This method uses circularly-polarized light, whose energy needs to be the same as, or slightly larger than, the semiconductor band-gap, to excite spin-polarized electrons. This process will introduce a spin-polarized electron-hole pair, which can be detected as electrical signals. Such an optically induced spin-polarized current can only be generated in a direct band-gap semiconductor due to the selection rule described in the following sections. This intr
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31

), Robert Hammond (Electrician. Electric Light in Our Homes. Creative Media Partners, LLC, 2015.

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32

Solymar, L., D. Walsh, and R. R. A. Syms. Semiconductors. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198829942.003.0008.

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Both intrinsic and extrinsic semiconductors are discussed in terms of their band structure. The acceptor and donor energy levels are introduced. Scattering is discussed, from which the conductivity of semiconductors is derived. Some mathematical relations between electron and hole densities are derived. The mobilities of III–V and II–VI compounds and their dependence on impurity concentrations are discussed. Band structures of real and idealized semiconductors are contrasted. Measurements of semiconductor properties are reviewed. Various possibilities for optical excitation of electrons are di
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33

Vishveshwara, Smitha, and C. V. Vishveshwara. Two Revolutions: Einstein’s Relativity and Quantum Physics. Oxford University PressOxford, 2024. https://doi.org/10.1093/9780191818080.001.0001.

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Abstract “Can you kick apart a black hole?” “What about electrons?” As a child, quantum-physicist Smitha Vishveshwara pondered such questions with her astrophysicist father, C. V. Vishveshwara (Vishu); decades later, their musings grew into a series of letter exchanges in Two Revolutions: Einstein’s Relativity and Quantum Physics. The letters between father and daughter lead the scientifically curious reader through these two remarkable branches of physics that dramatically changed our perception of Nature. From the subatomic to the astronomical realms, they weave a rich tapestry of scientific
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34

Thygesen, K. S., and A. Rubio. Correlated electron transport in molecular junctions. Edited by A. V. Narlikar and Y. Y. Fu. Oxford University Press, 2017. http://dx.doi.org/10.1093/oxfordhb/9780199533046.013.23.

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This article focuses on correlated electron transport in molecular junctions. More specifically, it considers how electronic correlation effects can be included in transport calculations using many-body perturbation theory within the Keldysh non-equilibrium Green’s function formalism. The article uses the GW self-energy method (G denotes the Green’s function and W is the screened interaction) which has been successfully applied to describe quasi-particle excitations in periodic solids. It begins by formulating the quantum-transport problem and introducing the non-equilibrium Green’s function f
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35

Holes and Other Superficialities. MIT Press, 1995.

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36

Corder, J. Kevin, and Christina Wolbrecht. Disappointed Hopes? Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780190265144.003.0002.

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How did the first female voters use their ballots? Focusing on the presidential election of 1924—in which Progressive Robert M. La Follette secured 17% of the vote—this chapter examines the expectation that women would be particularly likely to support candidates associated with the Progressive movement. Employing new strategies to estimate women’s vote choice using aggregate data, the findings show that female voters were not uniquely likely to support the Progressive candidate. Rather, in a small number of Republican-dominated midwestern states, female voters were more Republican than men, a
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37

Who Holds the Power: The Future's Electric... Independently Published, 2021.

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38

Stephen, Taylor. Who Holds the Power: The Future's Electric... Independently Published, 2021.

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39

Amrine, Thomas Hamer. Lighting Country Homes by Private Electric Plants. Creative Media Partners, LLC, 2018.

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40

Wonderful Fifty Years: By Edwin T. Holmes, President Holmes Electric Protective Co. , New York. Creative Media Partners, LLC, 2022.

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41

Glazov, M. M. Electron Spin Relaxation Beyond the Hyperfine Interaction. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0008.

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Here, some prospects for future studies in the field of electron and nuclear spin dynamics are outlined. In contrast to previous chapters where the electron interaction with multitude of nuclei was discussed, in Chapter 8 particular emphasis is put on a situation where hyperfine interaction is so strong that it leads to a qualitative rear rangement of the energy spectrum resulting in coherent excitation transfer between electron and nucleus. The strong coupling between the spin of the charge carrier and of the nucleus is realized; e.g., in the case of deep impurity centers in semiconductors or
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42

Johnson, Dennis W. Campaigns and Elections. Oxford University Press, 2019. http://dx.doi.org/10.1093/wentk/9780190935580.001.0001.

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Frequent and fair elections, open to all, are fundamental elements of a democracy. The United States, through its local, state, and national contests, holds more elections, more often, than any other democracy in the world. But in recent years, there have been troubling signs that our system of campaigns and elections has become much more fragile than we had previously thought. More specifically, in the past twenty years, campaigns have changed profoundly: social media and viral messaging compete with traditional media, races once considered local in nature have become nationalized, Supreme Co
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43

Marvin, Carolyn. When Old Technologies Were New. Oxford University Press, 1990. http://dx.doi.org/10.1093/oso/9780195063417.001.0001.

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In the history of electronic communication, the last quarter of the nineteenth century holds a special place, for it was during this period that the telephone, phonograph, electric light, wireless, and cinema were all invented. In When old Technologies Were New, Carolyn Marvin explores how two of these new inventions--the telephone and the electric light--were publicly envisioned at the end of the nineteenth century, as seen in specialized engineering journals and popular media. Marvin pays particular attention to the telephone, describing how it disrupted established social relations, unsettl
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44

Katz, Mark. Music and Technology: A Very Short Introduction. Oxford University PressNew York, 2022. http://dx.doi.org/10.1093/actrade/9780199946983.001.0001.

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Abstract This Very Short Introduction takes an expansive and inclusive approach meant to broaden and challenge traditional views of music and technology. In its most common use, “music technology” tends to evoke images of twentieth and twenty-first century electronic devices: synthesizers, recording equipment, music notation software, and the like. This volume, however, treats all tools used to create, store, reproduce, and transmit music—new or old, electronic or not—as technologies worthy of investigation. All musical instruments can be considered technologies. The modern piano, for example,
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45

Better Homes and Gardens so-easy slow cooker. Meredith, 2008.

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46

Holmes, Edwin Thomas. A Wonderful Fifty Years: By Edwin T. Holmes, President Holmes Electric Protective Co., New York. Franklin Classics Trade Press, 2018.

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47

Holmes, Edwin Thomas. A Wonderful Fifty Years: By Edwin T. Holmes, President Holmes Electric Protective Co., New York. Franklin Classics, 2018.

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48

Glazov, M. M. Strong Coupling of Electron and Nuclear Spins: Outlook and Prospects. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198807308.003.0011.

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In this chapter, some prospects in the field of electron and nuclear spin dynamics are outlined. Particular emphasis is put ona situation where the hyperfine interaction is so strong that it leads to a qualitative rearrangement of the energy spectrum resulting in the coherent excitation transfer between the electron and nucleus. The strong coupling between the spin of the charge carrier and of the nucleus is realized, for example in the case of deep impurity centers in semiconductors or in isotopically purified systems. We also discuss the effect of the nuclear spin polaron, that is ordered st
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49

How Electricity Gets from Power Plants to Homes. Raintree Publishers, 2017.

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50

Horing, Norman J. Morgenstern. Equations of Motion with Particle–Particle Interactions and Approximations. Oxford University Press, 2018. http://dx.doi.org/10.1093/oso/9780198791942.003.0008.

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Starting with the equation of motion for the field operator ψ(x,t) of an interacting many-particle system, the n-particle Green’s function (Gn) equation of motion is developed, with interparticle interactions generating an infinite chain of equations coupling it to (n+1)- and (n−1)-particle Green’s functions (Gn+1 and Gn−1, respectively). Particularly important are the one-particle Green’s function equation with its coupling to the two-particle Green’s function and the two-particle Green’s function equation with its coupling to the three-particle Green’s function. To develop solutions, it is n
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