scholarly journals Field-induced double dome and Bose-Einstein condensation in the crossing quantum spin chain system AgVOAsO4

2019 ◽  
Vol 100 (10) ◽  
Author(s):  
Franziska Weickert ◽  
Adam A. Aczel ◽  
Matthew B. Stone ◽  
V. Ovidiu Garlea ◽  
Chao Dong ◽  
...  
2013 ◽  
Vol 113 (17) ◽  
pp. 17D910 ◽  
Author(s):  
Yukio Yasui ◽  
Yudai Yanagisawa ◽  
Ryuji Okazaki ◽  
Ichiro Terasaki ◽  
Yasuhiro Yamaguchi ◽  
...  

2006 ◽  
Vol 51 ◽  
pp. 87-90 ◽  
Author(s):  
Y Furukawa ◽  
Y Nishisaka ◽  
K Kumagai ◽  
T Asano ◽  
Y Inagaki

Author(s):  
Klaus Morawetz

The Bose–Einstein condensation and appearance of superfluidity and superconductivity are introduced from basic phenomena. A systematic theory based on the asymmetric expansion of chapter 11 is shown to correct the T-matrix from unphysical multiple-scattering events. The resulting generalised Soven scheme provides the Beliaev equations for Boson’s and the Nambu–Gorkov equations for fermions without the usage of anomalous and non-conserving propagators. This systematic theory allows calculating the fluctuations above and below the critical parameters. Gap equations and Bogoliubov–DeGennes equations are derived from this theory. Interacting Bose systems with finite temperatures are discussed with successively better approximations ranging from Bogoliubov and Popov up to corrected T-matrices. For superconductivity, the asymmetric theory leading to the corrected T-matrix allows for establishing the stability of the condensate and decides correctly about the pair-breaking mechanisms in contrast to conventional approaches. The relation between the correlated density from nonlocal kinetic theory and the density of Cooper pairs is shown.


2021 ◽  
Vol 2021 (7) ◽  
Author(s):  
Pengcheng Lu ◽  
Yi Qiao ◽  
Junpeng Cao ◽  
Wen-Li Yang ◽  
Kang jie Shi ◽  
...  

Abstract A new nonlinear integral equation (NLIE) describing the thermodynamics of the Heisenberg spin chain is derived based on the t − W relation of the quantum transfer matrices. The free energy of the system in a magnetic field is thus obtained by solving the NLIE. This method can be generalized to other lattice quantum integrable models. Taking the SU(3)-invariant quantum spin chain as an example, we construct the corre- sponding NLIEs and compute the free energy. The present results coincide exactly with those obtained via other methods previously.


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