Phase shift, the Marshall sign, and the Luttinger-liquid behavior in one dimension

1994 ◽  
Vol 50 (18) ◽  
pp. 13837-13840 ◽  
Author(s):  
Z. Y. Weng
1997 ◽  
Vol 11 (01n02) ◽  
pp. 141-146
Author(s):  
A. Klümper

The supersymmetric tJ model in one dimension is investigated by means of the quantum transfer matrix (QTM). The free energy of the quantum system is given by just the largest eigenvalue of the QTM whereas the next-largest ones determine the correlation lengths at finite temperature. The first step of the analysis consists of an embedding of the QTM into a family of commuting matrices. In the second step the eigenvalues equations are derived by an algebraic Bethe ansatz. Finally, the eigenvalue equations are transformed into a set of nonlinear integral equations. Some numerical results are presented. The specific heat for instance shows the typical Luttinger liquid behavior at low temperatures.


1999 ◽  
Vol 83 (7) ◽  
pp. 1383-1386 ◽  
Author(s):  
A. F. Ho ◽  
P. Coleman

2012 ◽  
Vol 26 (22) ◽  
pp. 1244003
Author(s):  
C. DI CASTRO ◽  
S. CAPRARA

With particular reference to the role of the renormalization group (RG) approach and Ward identities (WI's), we start by recalling some old features of the one-dimensional Luttinger liquid as the prototype of non-Fermi-liquid behavior. Its dimensional crossover to the Landau normal Fermi liquid implies that a non-Fermi liquid, as, e.g., the normal phase of the cuprate high temperature superconductors, can be maintained in d>1 only in the presence of a sufficiently singular effective interaction among the charge carriers. This is the case when, nearby an instability, the interaction is mediated by critical fluctuations. We are then led to introduce the specific case of superconductivity in cuprates as an example of avoided quantum criticality. We will disentangle the fluctuations which act as mediators of singular electron–electron interaction, enlightening the possible order competing with superconductivity and a mechanism for the non-Fermi-liquid behavior of the metallic phase. This paper is not meant to be a comprehensive review. Many important contributions will not be considered. We will also avoid using extensive technicalities and making full calculations for which we refer to the original papers and to the many good available reviews. We will here only follow one line of reasoning which guided our research activity in this field.


1999 ◽  
Vol 12 (3) ◽  
pp. 351-365 ◽  
Author(s):  
H. Nélisse ◽  
C. Bourbonnais ◽  
H. Touchette ◽  
Y.M. Vilk ◽  
A.-M.S. Tremblay

2013 ◽  
pp. 319-327
Author(s):  
E. Levy ◽  
I. Sternfeld ◽  
M. Eshkol ◽  
M. Karpovski ◽  
A. Palevski ◽  
...  

2003 ◽  
Vol 67 (20) ◽  
Author(s):  
Y. C. Chung ◽  
M. Heiblum ◽  
Y. Oreg ◽  
V. Umansky ◽  
D. Mahalu

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