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排序方式: 共有91条查询结果,搜索用时 15 毫秒
11.
W. Sokoloff 《Fresenius' Journal of Analytical Chemistry》1875,14(1):423
Ohne Zusammenfassung 相似文献
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Polarized Raman and infrared spectra of the one dimensional (1-D) superionic conductor (K2xMgxTi(8?x)O16; x = 0.77) have been measured over the phonon frequency region 10–1000 cm?1 as a function of temperature and pressure. The majority of the IR and Raman active modes predicted by group theory for the (Ti, Mg)O6 framework were observed. The frequencies and their IR and Raman scattering cross-sections for the incommensurate lattice of K+ ions were calculated using a one dimensional linear chain model. This model assumes Coulomb interaction between nearest neighbors that are located in a sinusoidal potential due to the framework lattice. Several broad Raman bands were attributed to amplitudon type modes from the one dimensional incommensurate K+ ion sublattice. The IR active phason modes could not be identified unambiguously due to the underlying TiO framework vibrations which are known to possess large anharmonicity and oscillator strenghts. 相似文献
14.
J. B. Sokoloff 《Molecular Crystals and Liquid Crystals》2013,570(1-4):91-94
It is argued that the existence of a dynamical threshold field [i.e. the value of the electric field such that when the applied field is reduced to this value the charge density wave (CDW) stops sliding] requires that the sliding of the CDW at low center of mass velocity occurs as local sudden jumping motion reminiscent of “stick-slip” friction. Using this model, it is argued in the weak impurity limit that the static threshold field is greater than the dynamic threshold field. 相似文献
15.
Yushkov E. V. Lukin A. S. Sokoloff D. D. 《Journal of Experimental and Theoretical Physics》2020,130(6):935-944
Journal of Experimental and Theoretical Physics - We compare the classical mean-field dynamo model proposed by Steenbeck, Krause, and Rädler to describe the generation of large-scale magnetic... 相似文献
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Anjos JC Appel JA Bean A Bracker SB Browder TE Cremaldi LM Duboscq JE Elliot JR Escobar CO Gibney MC Hartner GF Karchin PE Kumar BR Losty MJ Luste GJ Mantsch PM Martin JF McHugh S Menary SR Morrison RJ Nash T Ong P Pinfold J Punkar G Purohit MV Ross WR Santoro AF Shoup AL Sliwa K Sokoloff MD Souza MH Spalding WJ Streetman ME Stundzia AB Witherell MS 《Physical review D: Particles and fields》1992,46(1):R1-R5
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Anjos JC Appel JA Bean A Bracker SB Browder TE Cremaldi LM Duboscq JE Elliott JR Escobar CO Gibney MC Hartner GF Huber J Karchin PE Kumar BR Losty MJ Luste GJ Mantsch PM Martin JF McHugh S Menary SR Morrison RJ Nash T Pinfold J Punkar G Purohit MV Ross WR Santoro AF Schmidt DM Shoup AL Sliwa K Sokoloff MD Souza MH Sperka D Spalding WJ Streetman ME Stundzia AB Witherell MS 《Physical review D: Particles and fields》1992,46(5):1941-1950
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Anjos JC Appel JA Bean A Bracker SB Browder TE Cremaldi LM Duboscq JE Elliott JR Escobar CO Gibney MC Hartner GF Karchin PE Kumar BR Losty MJ Luste GJ Mantsch PM Martin JF McHugh S Menary SR Morrison RJ Nash T Nauenberg U Ong P Pinfold J Punkar G Purohit MV Santoro AF Sidhu JS Shoup AL Sliwa K Sokoloff MD Souza MH Spalding WJ Streetman ME Stundzia AB Witherell MS 《Physical review D: Particles and fields》1990,41(9):2705-2708
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Anjos JC Appel JA Bean A Bracker SB Browder TE Cremaldi LM Elliott JR Escobar CO Estabrooks P Gibney MC Hartner GF Karchin PE Kumar BR Losty MJ Luste GJ Mantsch PM Martin JF McHugh S Menary SR Morrison RJ Nash T Nauenberg U Ong P Pinfold J Punkar G Purohit MV Raab JR Santoro AF Sidhu JS Sliwa K Sokoloff MD Souza MH Spalding WJ Streetman ME Stundia AB Witherell MS 《Physical review letters》1989,62(15):1721-1723