scholarly journals Exact high temperature expansion of the one-loop thermodynamic potential with complex chemical potential

2014 ◽  
Vol 89 (3) ◽  
Author(s):  
Bruno Klajn
2003 ◽  
Vol 67 (11) ◽  
Author(s):  
Onofre Rojas ◽  
E. V. Corrêa Silva ◽  
Winder A. Moura-Melo ◽  
S. M. de Souza ◽  
M. T. Thomaz

2015 ◽  
Vol 16 (1) ◽  
pp. 136-139
Author(s):  
N. Yu. Filonenko

The thermodynamic quantities for iron monoboride FeB, such as entropy, enthalpy, heat capacity and their temperature dependence, are considered. It is shown, that accounting for contribution to the zeroth-order high-temperature expansion of thermodynamic potential for Fe-B binary alloy enables to describe forming monoboride FeB in more complete way from the viewpoint of thermodynamics.


1995 ◽  
Vol 10 (22) ◽  
pp. 1619-1626 ◽  
Author(s):  
A.A. BYTSENKO ◽  
S.D. ODINTSOV ◽  
S. ZERBINI

The high temperature behavior of the open bosonic string free energy in the space S1 ⊗ HN with vanishingly small curvature is investigated. The leading term of the high temperature expansion of the one-loop free energy, near the Hagedorn instability, is obtained. The problem of ir regularization of thermodynamical quantities is pointed out. For minimally coupling quantum fields related to the normal modes of strings, the results are similar to the ones valid for Rindler space. In the lower mass string states regime a connection with the quantum corrections to the black hole entropy is outlined.


1991 ◽  
Vol 05 (13) ◽  
pp. 907-914 ◽  
Author(s):  
RICHARD J. CRESWICK ◽  
CYNTHIA J. SISSON

The properties of the spin-1/2 Heisenberg model on 1, 2, and 3-dimensional lattices are calculated using the Decoupled Cell Method of Homma et al., and these results are compared with high temperature and spin-wave expansions, and with other numerical approaches. The DCM has advantages over other Monte Carlo methods currently in wide use in that the transition probability is positive definite, there is no need to introduce an additional imaginary time, or Trotter, dimension, and the acceptance rate for transitions is comparable to that of classical lattice models. We find very good agreement between the DCM and the high temperature expansion in the temperature region where the high temperature expansion is valid, and reasonably good agreement at low temperatures with spin wave theory. The DCM fails for temperatures T < Tc which decreases with the size of the cell.


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