Phenomenological theory of superfluidity and superconductivity
Identifieur interne : 000628 ( Istex/Corpus ); précédent : 000627; suivant : 000629Phenomenological theory of superfluidity and superconductivity
Auteurs : Mario RabinowitzSource :
- International Journal of Theoretical Physics [ 0020-7748 ] ; 1994-02-01.
English descriptors
- Teeft :
- Angular momentum, Boson, Broglie wavelength, Coherence, Coherence length, Coherence lengths, Condensation temperature, Cooper pair, Cooper pairs, Different ways, Effective mass, Electron pairs, Energy level, Excellent agreement, Experimental range, Experimental value, Fermi, Fermi energy, Fermion, Ground state, Heavy fermion, International journal, Large number, Modern physics, Multiple occupancy, Number density, Pairing, Pairing mechanism, Phase space, Phenomenological theory, Physical review, Physical review letters, Rabinowitz, Simple terms, Simplest materials, Small number, Superconducting electrons, Superconductivity, Superconductors, Superfluid, Superfluid transition, Superfluid transition temperature, Superfluidity, Theoretical physics, Transition temperatures, Triplet state, Unorthodox superconductors, Wave function.
Abstract
Abstract: Quantum condensation is used here as the basis for a phenomenological theory of superfluidity and superconductivity. It leads to remarkably good calculations of the transition temperaturesT c of superfluid3He and4He, as well as a large number of cuprate, heavy fermion, organic, dichalcogenide, and bismuth oxide superconductors. Although this approach may apply least to the long-coherence-length metallics, reasonably good estimates are made for them and chevral superconductors.T c for atomic H is estimated.T c can be calculated as a function of number density or density of states and effective mass of normal carriers; or alternatively with the Fermi energy as the only input parameter. Predictions are made for a total of 26 superconductors and four superfluids. An estimate is also made for coherence lengths.
Url:
DOI: 10.1007/BF00844979
Links to Exploration step
ISTEX:3ED27D0D32322473E51C133F8BB99AD81939B261Le document en format XML
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It leads to remarkably good calculations of the transition temperatures<Emphasis Type="Italic">T</Emphasis><Subscript><Emphasis Type="Italic">c</Emphasis></Subscript> of superfluid<Superscript>3</Superscript>He and<Superscript>4</Superscript>He, as well as a large number of cuprate, heavy fermion, organic, dichalcogenide, and bismuth oxide superconductors. Although this approach may apply least to the long-coherence-length metallics, reasonably good estimates are made for them and chevral superconductors.<Emphasis Type="Italic">T</Emphasis><Subscript><Emphasis Type="Italic">c</Emphasis></Subscript> for atomic H is estimated.<Emphasis Type="Italic">T</Emphasis><Subscript><Emphasis Type="Italic">c</Emphasis></Subscript> can be calculated as a function of number density or density of states and effective mass of normal carriers; or alternatively with the Fermi energy as the only input parameter. Predictions are made for a total of 26 superconductors and four superfluids. 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It leads to remarkably good calculations of the transition temperaturesT c of superfluid3He and4He, as well as a large number of cuprate, heavy fermion, organic, dichalcogenide, and bismuth oxide superconductors. Although this approach may apply least to the long-coherence-length metallics, reasonably good estimates are made for them and chevral superconductors.T c for atomic H is estimated.T c can be calculated as a function of number density or density of states and effective mass of normal carriers; or alternatively with the Fermi energy as the only input parameter. Predictions are made for a total of 26 superconductors and four superfluids. 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