scholarly journals Bose-Einstein condensation of triplons close to the quantum critical point in the quasi-one-dimensional spin- 12 antiferromagnet NaVOPO4

2019 ◽  
Vol 100 (14) ◽  
Author(s):  
Prashanta K. Mukharjee ◽  
K. M. Ranjith ◽  
B. Koo ◽  
J. Sichelschmidt ◽  
M. Baenitz ◽  
...  
2005 ◽  
Vol 72 (10) ◽  
Author(s):  
S. E. Sebastian ◽  
P. A. Sharma ◽  
M. Jaime ◽  
N. Harrison ◽  
V. Correa ◽  
...  

2019 ◽  
Vol 100 (12) ◽  
Author(s):  
Rui-Zhen Huang ◽  
Da-Chuan Lu ◽  
Yi-Zhuang You ◽  
Zi Yang Meng ◽  
Tao Xiang

2017 ◽  
Vol 96 (4) ◽  
Author(s):  
Benedikt Lechtenberg ◽  
Fabian Eickhoff ◽  
Frithjof B. Anders

2020 ◽  
Vol 35 (03) ◽  
pp. 2040005 ◽  
Author(s):  
M. Bordag

We investigate Bose-Einstein condensation of a gas of non-interacting Bose particles moving in the background of a periodic lattice of delta functions. In the one-dimensional case, where one has no condensation in the free case, we showed that this property persist also in the presence of the lattice. In addition we formulated some conditions on the spectral functions which would allow for condensation.


2018 ◽  
Vol 182 ◽  
pp. 02066
Author(s):  
Evgeni E. Kolomeitsev ◽  
Maxim E. Borisov ◽  
Dmitry N. Voskresensky

We consider a non-ideal hot pion gas with the dynamically fixed number of particles in the model with the λφ4 interaction. The effective Lagrangian for the description of such a system is obtained by dropping the terms responsible for the change of the total particle number. Within the self-consistent Hartree approximation, we compute the effective pion mass, thermodynamic characteristics of the system and identify a critical point of the induced Bose-Einstein condensation when the pion chemical potential reaches the value of the effective pion mass. The normalized variance, skewness, and kurtosis of the particle number distributions are calculated. We demonstrate that all these characteristics remain finite at the critical point of the Bose-Einstein condensation. This is due to the non-perturbative account of the interaction and is in contrast to the ideal-gas case.


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