SCOPUS 정보 검색 플랫폼

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- 84913080906
- Monte Carlo Simulations of Vortex Lines in a Lattice London Model
- (1992) Europhysics Letters (EPL) , vol.17 , pp. 449
- Cavalcanti, R.¹ Carneiro, G.² Gartner, A.³

15
- 33646663852
- A recent work that similarly studies vortex lines with finite λ, although with a different objective, is
- (1994) Phys. Rev. B , vol.50 , pp. 6982
- Carneiro, G.¹

17
- 0008874475
- (1994) Phys. Rev. Lett. , vol.72 , pp. 2085
- Chen, T.¹ Teitel, S.²

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- 0003635562
- R. C. Clark, D. H. Derrick, Oliver and Boyd, Edinburgh
- (1969) Mathematical Methods in Solid State and Superfluid Theory , pp. 121
- Baym, G.¹

22
- 0000379688
- For free boundary conditions along z^, as opposed to the periodic boundary conditions of the analog 2D bosons, a sharp KT transition does not exist; nevertheless, a strong crossover should remain. See
- (1989) Phys. Rev. B , vol.39 , pp. 2756
- Fisher, M.P.A.¹ Lee, D.H.²

23
- 18344383012
- (1987) Phys. Rev. B , vol.36 , pp. 8343
- Pollock, E.L.¹ Ceperley, D.M.²

24
- 84927479239
- Since we work in the Helmholtz ensemble at fixed Bz^, our configurations are constrained to satisfy nx,y(q=0)=0. Hence a direct computation of W must always rigorously vanish in each individual configuration. Nevertheless, we can compute the correct value of 〈W2〉 that one would find in the Gibbs ensemble [with no constraint on nx,y(q=0)] by taking an appropriate q→0 limit. This is done by considering only one component, say Wy2, and taking q in the x-y plane transverse to this direction, i.e., qz=qy=0 as qx→0. This procedure leads to a factor of 2 correction to the KT transition temperature reported in Ref. [c11]. We thank A. P. Young for clarification on this point.

25
- 0542408167
- Flux lattice melting and collective creep in high-Tc superconductors
- (1990) Physica A: Statistical Mechanics and its Applications , vol.168 , pp. 319
- Feigelman, M.V.¹

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- 84927501076
- (unpublished) also suggest Λ as an important length in the vortex liquid. However, their arguments seem unrelated to the KT transition discussed here, and they suggest that the intermediate superconducting line liquid persists even for Lz→∞.
- Feigelman, M.V.¹ Ioffe, L.B.²

* 이 정보는 Elsevier사의 SCOPUS DB에서 KISTI가 분석하여 추출한 것입니다.