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Volumn 59, Issue 9, 1999, Pages 6266-6277

Excitation spectrum of the (formula presented) quantum spin ladder with frustration: Elementary quasiparticles and many-particle bound states

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EID: 0000014452     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.59.6266     Document Type: Article
Times cited : (72)

References (29)
  • 18
    • 85038952091 scopus 로고    scopus 로고
    • X. Wang, cond-mat/9803290 (unpublished).
    • Wang, X.1
  • 19
    • 85038902499 scopus 로고    scopus 로고
    • (private communication)
    • H.Q. Lin, cond-mat/9805269 (unpublished);and (private communication).
    • Lin, H.Q.1
  • 24
    • 85038938249 scopus 로고    scopus 로고
    • Equation (30) can also be derived as a two-particle Schrödinger equation in momentum space (Formula presented) For the singlet bound state one has (Formula presented) where (Formula presented) are defined in the text before Eq. (28). For a triplet bound state with polarization (Formula presented) While this way of deriving the Bethe-Salpeter equation is quite simple and physically transparent, the approach presented in the text is more general and we give it preference since it is better suited for treating more complicated interaction terms [e.g., three-body interactions which appear in certain models with dimerization (Ref. 17
    • Equation (30) can also be derived as a two-particle Schrödinger equation in momentum space (Formula presented) For the singlet bound state one has (Formula presented) where (Formula presented) are defined in the text before Eq. (28). For a triplet bound state with polarization (Formula presented) While this way of deriving the Bethe-Salpeter equation is quite simple and physically transparent, the approach presented in the text is more general and we give it preference since it is better suited for treating more complicated interaction terms [e.g., three-body interactions which appear in certain models with dimerization (Ref. 17)].
  • 25
    • 85038908520 scopus 로고    scopus 로고
    • Strictly speaking Eq. (40) is valid for (Formula presented) However it works quite well even for (Formula presented) For example at the point (Formula presented) according to Eq. (40) (Formula presented) while the numerical result (Refs. 6 and 13) is (Formula presented)
    • Strictly speaking Eq. (40) is valid for (Formula presented) However it works quite well even for (Formula presented) For example at the point (Formula presented) according to Eq. (40) (Formula presented) while the numerical result (Refs. 6 and 13) is (Formula presented)
  • 26
    • 85038934954 scopus 로고    scopus 로고
    • This effect is similar to the shift of energy levels due to radiative corrections in relativistic atomic physics (Lamb shift)
    • This effect is similar to the shift of energy levels due to radiative corrections in relativistic atomic physics (Lamb shift).
  • 29
    • 85038908381 scopus 로고
    • Phys. Rev. BY. Xian, 52, 12 485 (1995).
    • (1995) , vol.52 , pp. 12
    • Xian, Y.1


* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.