Parallel-tempering Monte Carlo simulations of the finite temperature behavior of (H2O)6−

2003 ◽  
Vol 119 (22) ◽  
pp. 11645-11653 ◽  
Author(s):  
F. Wang ◽  
K. D. Jordan
2019 ◽  
Vol 34 (09) ◽  
pp. 1950052
Author(s):  
Natalia V. Kolomoyets ◽  
Vladimir V. Skalozub

The color structure of the gluon field magnetic mass is investigated in the lattice SU(2) gluodynamics. To realize that the interaction between a monopole–antimonopole string and external neutral Abelian chromomagnetic field flux is considered. The string is introduced in the way proposed by Srednicki and Susskind. The neutral Abelian field flux is introduced through the twisted boundary conditions. Monte Carlo simulations are performed on 4D lattices at finite temperature. It is shown that the presence of the Abelian field flux weakens the screening of the string field. That means decreasing the gluon magnetic mass for this environment. The contribution of the neutral Abelian field has the form of “enhancing” factor in the fitting functions. This behavior independently confirms the long-range nature of the neutral Abelian field reported already in the literature. The comparison with analytic calculations is given.


2020 ◽  
Vol 124 (20) ◽  
pp. 4036-4047
Author(s):  
Aleš Vítek ◽  
Daniel J. Arismendi-Arrieta ◽  
Martina Šarmanová ◽  
René Kalus ◽  
Rita Prosmiti

2007 ◽  
Vol 19 (40) ◽  
pp. 406208 ◽  
Author(s):  
Artur P Terzyk ◽  
Sylwester Furmaniak ◽  
Piotr A Gauden ◽  
Peter J F Harris ◽  
Jerzy Włoch ◽  
...  

2014 ◽  
Vol 2014.20 (0) ◽  
pp. _20206-1_-_20206-2_
Author(s):  
Satoshi USUI ◽  
Tatsunari HANAZONO ◽  
Hiroshi KOIBUCHI

2008 ◽  
Vol 455 (4-6) ◽  
pp. 135-138 ◽  
Author(s):  
Albert DeFusco ◽  
Thomas Sommerfeld ◽  
Kenneth D. Jordan

2015 ◽  
Vol 17 (16) ◽  
pp. 10532-10537 ◽  
Author(s):  
Aleš Vítek ◽  
René Kalus

Classical parallel-tempering Monte Carlo simulations of [H2O]48 and [H2O]118 have been performed in the isothermal–isobaric ensemble and a two-dimensional multiple-histogram method has been used to calculate the heat capacity of the two clusters.


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