Titlebook: Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries; Kenneth E. Gray Book 1981 Plenum Press, New York 1981 Josephson junctio

預(yù)兆前

書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries影響因子(影響力)




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries影響因子(影響力)學(xué)科排名




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries網(wǎng)絡(luò)公開(kāi)度




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries網(wǎng)絡(luò)公開(kāi)度學(xué)科排名




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries被引頻次




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries被引頻次學(xué)科排名




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries年度引用




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries年度引用學(xué)科排名




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries讀者反饋




書目名稱Nonequilibrium Superconductivity, Phonons, and Kapitza Boundaries讀者反饋學(xué)科排名

AIL

The Effect of Microwaves on Tunnel Junctions,oretical predictions and experimental observations relating to redistribution of quasiparticles and their relationship to the “gap enhancement” phenomenon. In the present paper we will describe the effect of microwaves on tunnel junctions excluding specifically “gap enhancement,” which will be described in Chapter 7 by J. E. Mooij.

AMPLE

卡死偷電

Kapitza Conductance of Solid-Liquid He Interfaces,es ?0.05K. Although many of the characteristics of this non-classical channel have been measured the microscopic process still remains a mystery. The subject has been reviewed by Pollack (1969) Snyder (1970) Challis (1974, 1975) Anderson (1976) Kinder et al. (1979) and Wyatt (1979).

Collected

Nonequilibrium Phonons,eration and detection in Section 2, experimental probing of nonequilibrium phonon emission in Section 3, applications to phonon absorption spectrocopy in Section 4, quantitative phonon intensity measurements in Section 5, applications to phonon emission spectroscopy in Section 6, and aspects of future work in Section 7.

VEN

maudtin

Normal-Superconducting Boundaries,. the thermal boundary resistance becomes less marked and at the same time a boundary contribution to the electrical resistance becomes apparent, as illustrated in Fig. 2 (Landau, 1970; Pippard et al., 1971).

MOAT

MOCK

Heating and Dynamic Enhancement in Metallic Weak Links,hich slows down the gap response time from τ. to τ., which may be orders of magnitude longer, and also provides a type of dynamic enhancement of superconductivity in current-driven metallic weak links.

放逐某人

Nonequilibrium Effects in 1-D Superconductors,s that is not quite cleared up obtains ordinary resistance.” Such a transition is inherently a nonequilibrium phenomenon, and given what we have learned from the preceding chapters it should be possible to see what aspects of this process have and have not yet been cleared up.