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Volumn 79, Issue 21, 2009, Pages

Topological properties of spin-triplet superconductors and Fermi surface topology in the normal state

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EID: 68949137230     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.79.214526     Document Type: Article
Times cited : (192)

References (25)
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    • Note that in order to determine which N0 in Table 1 is realized in a time-reversal-invariant spin-triplet superconductor, we need the knowledge of the gap function in addition to that of the Fermi surface structure. Nevertheless, for the cases in the first row in Table 1 (a) and the first and third rows in Table 1 (b), we can conclude that N0 becomes nonzero only from the knowledge of the Fermi surface topology.
    • Note that in order to determine which N0 in Table 1 is realized in a time-reversal-invariant spin-triplet superconductor, we need the knowledge of the gap function in addition to that of the Fermi surface structure. Nevertheless, for the cases in the first row in Table 1 (a) and the first and third rows in Table 1 (b), we can conclude that N0 becomes nonzero only from the knowledge of the Fermi surface topology.
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    • This assumption is met for most cases, however, for a system with a sublattice structure, the parity operator may also exchange the sublattice structure (for example, see Ref.).
    • This assumption is met for most cases, however, for a system with a sublattice structure, the parity operator may also exchange the sublattice structure (for example, see Ref.).
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* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.