Temperature definition for a finite number of classical spin-half particles: A canonical ensemble approach

2008 ◽  
Vol 372 (5) ◽  
pp. 574-578
Author(s):  
Q.H. Liu ◽  
X. Wang
2007 ◽  
Vol 21 (23n24) ◽  
pp. 4007-4012
Author(s):  
X. WANG ◽  
Q. H. LIU

For the classical spin 1/2 system, a canonical ensemble theory for finite number of particles is developed to show that when the temperature approaches to 0K and in thermodynamic limit, the temperature fluctuation [Formula: see text] itself does not diverge, but the product of the particle number N and [Formula: see text] as [Formula: see text] does.


2002 ◽  
Vol 16 (14n15) ◽  
pp. 2017-2032 ◽  
Author(s):  
KEH-FEI LIU

I will review the finite density algorithm for lattice QCD based on finite chemical potential and summarize the associated difficulties. I will propose a canonical ensemble approach which projects out the finite baryon number sector from the fermion determinant. For this algorithm to work, it requires an efficient method for calculating the fermion determinant and a Monte Carlo algorithm which accommodates unbiased estimate of the probability. I shall report on the progress made along this direction with the Padé–Z2 estimator of the determinant and its implementation in the newly developed Noisy Monte Carlo algorithm.


1999 ◽  
Vol 59 (3) ◽  
pp. 3386-3401 ◽  
Author(s):  
D. Bollé ◽  
R. Erichsen

2017 ◽  
Vol 138 ◽  
pp. 02002
Author(s):  
V. G. Bornyakov ◽  
D. L. Boyda ◽  
V. A. Goy ◽  
A. V. Molochkov ◽  
Atsushi Nakamura ◽  
...  

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