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Volumn 86, Issue 4, 2001, Pages 676-679

Two-dimensional anisotropic non-Fermi-liquid phase of coupled Luttinger liquids

Author keywords

[No Author keywords available]

Indexed keywords

ANISOTROPY; CARRIER CONCENTRATION; ELECTRON SCATTERING; FERMIONS; FOURIER TRANSFORMS; MAGNETIC FIELD EFFECTS; MOLECULAR DYNAMICS; MOLECULAR STRUCTURE; NUMERICAL ANALYSIS; QUANTUM THEORY;

EID: 0035130967     PISSN: 00319007     EISSN: None     Source Type: Journal    
DOI: 10.1103/PhysRevLett.86.676     Document Type: Article
Times cited : (186)

References (19)
  • 1
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    • S. Tomonaga. Prog. Theor. Phys. 5, 544 (1950); J.M. Luttinger, J. Math. Phys. (N.Y.) 4, 1154 (1963); F. D.M. Haldane, J. Phys. C 14, 2585 (1981).
    • (1950) Prog. Theor. Phys. , vol.5 , pp. 544
    • Tomonaga, S.1
  • 2
    • 33744514746 scopus 로고
    • S. Tomonaga. Prog. Theor. Phys. 5, 544 (1950); J.M. Luttinger, J. Math. Phys. (N.Y.) 4, 1154 (1963); F. D.M. Haldane, J. Phys. C 14, 2585 (1981).
    • (1963) J. Math. Phys. (N.Y.) , vol.4 , pp. 1154
    • Luttinger, J.M.1
  • 3
    • 4344648736 scopus 로고
    • S. Tomonaga. Prog. Theor. Phys. 5, 544 (1950); J.M. Luttinger, J. Math. Phys. (N.Y.) 4, 1154 (1963); F. D.M. Haldane, J. Phys. C 14, 2585 (1981).
    • (1981) J. Phys. C , vol.14 , pp. 2585
    • Haldane, F.D.M.1
  • 6
    • 0342334664 scopus 로고    scopus 로고
    • condmat/0002087
    • See the recent review by F. von Oppen et al., condmat/0002087.
    • Von Oppen, F.1
  • 7
    • 0029322096 scopus 로고
    • J. Tranquada et al., Nature (London) 375, 561 (1995); S. A. Kivelson et al., Nature (London) 393, 550 (1998).
    • (1995) Nature (London) , vol.375 , pp. 561
    • Tranquada, J.1
  • 8
    • 0032508034 scopus 로고    scopus 로고
    • J. Tranquada et al., Nature (London) 375, 561 (1995); S. A. Kivelson et al., Nature (London) 393, 550 (1998).
    • (1998) Nature (London) , vol.393 , pp. 550
    • Kivelson, S.A.1
  • 11
    • 0343639808 scopus 로고    scopus 로고
    • note
    • Although the electrons in quantum Hall effect stripes are spin polarized, the physics in that case differs in many details from what we consider here, due to the presence of the soft translational mode and the magnetic field.
  • 14
    • 0343204235 scopus 로고    scopus 로고
    • note
    • ij(0) + ⋯, which leads to terms containing additional spatial derivatives, which are irrelevant at the SLL fixed points.
  • 15
    • 0342769579 scopus 로고    scopus 로고
    • note
    • i can slide relative to each other at no cost.
  • 16
    • 0343639806 scopus 로고    scopus 로고
    • note
    • The case of double roots is considered in [6].
  • 17
    • 0343204233 scopus 로고    scopus 로고
    • note
    • Choosing the set of perturbing operators for a physical situation is an involved issue, which will depend on details of the system and the small but, nevertheless, finite temperature at which it is considered. Then, operators that have small bare values and are not further generated in the RG could be unimportant, even if relevant.
  • 18
    • 0343639804 scopus 로고    scopus 로고
    • note
    • δl where α = ±1 for (L/R) and α + β = γ + δ by momentum conservation. We have taken the maximum separation between any two fermion operators to be ≤10. The ones that destabilize the SLL points usually involve simultaneous hops on pairs of nearest neighbor chains. These could well be present or generated in physical systems.


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.