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Books on the topic 'Temperature coupling'

Author: Grafiati
Published: 10 December 2022
Last updated: 28 January 2023

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1

Hightower, Tess. 10 ways to take your relationship temperature: An empirically based interactive workbook to help couples create conscious coupling. Mustard Seed Press, 2002.

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2

Hart, David P. Earth-coupled heat transfer: Offers engineers and other practitioners of applied physics the information to solve heat transfer problems as they apply to earth-coupling. National Water Well Association, 1986.

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3

Vallée, Charlotte. Long-term evolution and coupling of the boundary layers in the STRATUS deck regions of the eastern Pacific (STRATUS): Data report. Upper Ocean Processes Group, WHOI, 2002.

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4

Vallée, Charlotte. Long-term evolution and coupling of the boundary layers in the STRATUS deck regions of the eastern Pacific (STRATUS): Data report. Upper Ocean Processes Group, WHOI, 2002.

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5

Alexandrov, Alexandre S. Strong-Coupling Theory of High-Temperature Superconductivity. Cambridge University Press, 2013.

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6

Alexandrov, Alexandre S. Strong-Coupling Theory of High-Temperature Superconductivity. Cambridge University Press, 2013.

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7

Alexandrov, Alexandre S. Strong-Coupling Theory of High-Temperature Superconductivity. Cambridge University Press, 2013.

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8

Alexandrov, Alexandre S. Strong-Coupling Theory of High-Temperature Superconductivity. Cambridge University Press, 2013.

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9

Kavokin, Alexey V., Jeremy J. Baumberg, Guillaume Malpuech, and Fabrice P. Laussy. Strong Coupling: Polariton Bose Condensation. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198782995.003.0008.

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In this Chapter we address the physics of Bose-Einstein condensation and its implications to a driven-dissipative system such as the polariton laser. We discuss the dynamics of exciton-polaritons non-resonantly pumped within a microcavity in the strong coupling regime. It is shown how the stimulated scattering of exciton-polaritons leads to formation of bosonic condensates that may be stable at elevated temperatures, including room temperature.
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10

United States. National Aeronautics and Space Administration., ed. Test program, helium II, orbital resupply coupling: Final report. Ball Aerospace Systems Group, Ball Corp., 1991.

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11

Test program, helium II, orbital resupply coupling: Final report. Ball Aerospace Systems Group, Ball Corp., 1991.

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12

Scott, Williamson Gary, and United States. National Aeronautics and Space Administration., eds. Experimental results of Hooper's gravity-electromagnetic coupling concept. National Aeronautics and Space Administration, 1995.

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13

Eriksson, Olle, Anders Bergman, Lars Bergqvist, and Johan Hellsvik. Spin Dynamics at Finite Temperature. Oxford University Press, 2017. http://dx.doi.org/10.1093/oso/9780198788669.003.0005.

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In Chapter 4 we presented a microscopic mechanism behind the LL equation and its connection to ab-initio results, such as that provided by density functional theory. All the analysis of Chapter 4 was done by considering a temperature T=0 K. Since most magnetic phenomena of interest are observed at finite temperature, it is important to generalize the analysis presented above to incorporate effects of finite temperature. In the discussion of Eqn. 4.1 it was mentioned briefly that finite temperature effects are incorporated in the stochastic field. Details of the coupling between temperature and
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14

Calculated coupling efficiency between an elliptical-core optical fiber and an optical waveguide over temperature [microform]. National Aeronautics and Space Administration, 1995.

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15

United States. National Aeronautics and Space Administration., ed. Feasibility of coupling between a single-mode elliptical-core fiber and a single mode rib waveguide over temperature. National Aeronautics and Space Administration, 1995.

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16

United States. National Aeronautics and Space Administration., ed. Comparison of methods for the calculation of thermal contact resistance of the first Brazilian satellite. National Aeronautics and Space Administration, 1988.

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17

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
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18

Zhang, Wei. Synthetic Spin-Orbit Coupling in Cold Atoms. World Scientific Publishing Co Pte Ltd, 2018.

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19

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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20

L, Horwitz James, University of Alabama in Huntsville. Center for Space Plasma and Aeronomic Research., University of Alabama in Huntsville. College of Science., and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations: Final report, grant NAG8-239, July 10, 1992-November 9, 1996. National Aeronautics and Space Administration, 1996.

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21

L, Horwitz James, and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations: February-July, 1994 : semiannual progress report. National Aeronautics and Space Administration, 1994.

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22

L, Horwitz James, University of Alabama in Huntsville. Center for Space Plasma and Aeronomic Research., University of Alabama in Huntsville. College of Science., and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations: Final report, grant NAG8-239, July 10, 1992-November 9, 1996. National Aeronautics and Space Administration, 1996.

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23

L, Horwitz James, and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations. National Aeronautics and Space Administration, 1995.

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24

L, Horwitz James, and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations: February-July, 1994 : semiannual progress report. National Aeronautics and Space Administration, 1994.

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25

L, Horwitz James, and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations: Semiannual progress report, grant NAG8-239, July, 1992 - January, 1993. National Aeronautics and Space Administration, 1993.

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26

L, Horwitz James, and United States. National Aeronautics and Space Administration., eds. Magnetospheric space plasma investigations: Semiannual progress report, grant NAG8-239, July, 1992 - January, 1993. National Aeronautics and Space Administration, 1993.

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27

Magnetospheric space plasma investigations. National Aeronautics and Space Administration, 1995.

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28

Cao, Gang, and Lance DeLong. Physics of Spin-Orbit-Coupled Oxides. Oxford University Press, 2021. http://dx.doi.org/10.1093/oso/9780199602025.001.0001.

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Prior to 2010, most research on the physics and chemistry of transition metal oxides was dominated by compounds of the 3d-transition elements such as Cr, Mn, Fe, Co, Ni, and Cu. These materials exhibited novel, important phenomena that include giant magnetoresistance in manganites, as well as high-temperature superconductivity in doped La<sub>2</sub>CuO<sub>4</sub> and related cuprates. The discovery in 1994 of an exotic superconducting state in Sr<sub>2</sub>RuO<sub>4</sub> shifted some interest toward ruthenates. Moreover, the realization in 2008 that a novel variant of the classic Mott meta
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29

Zinn-Justin, Jean. Quantum Field Theory and Critical Phenomena. 5th ed. Oxford University Press, 2021. http://dx.doi.org/10.1093/oso/9780198834625.001.0001.

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Introduced as a quantum extension of Maxwell's classical theory, quantum electrodynamic (QED) has been the first example of a quantum field theory (QFT). Eventually, QFT has become the framework for the discussion of all fundamental interactions at the microscopic scale except, possibly, gravity. More surprisingly, it has also provided a framework for the understanding of second order phase transitions in statistical mechanics. In fact, as hopefully this work illustrates, QFT is the natural framework for the discussion of most systems involving an infinite number of degrees of freedom with loc
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