Geometrical aspects and quantum brachistochrone problem for a collection of N spin-s system with long-range Ising-type interaction

2020 ◽  
Vol 384 (27) ◽  
pp. 126682
Author(s):  
B. Amghar ◽  
M. Daoud
2010 ◽  
Vol 24 (32) ◽  
pp. 6323-6333
Author(s):  
BAKHROM YAVIDOV

In this work, renormalization of effective mass of an electron due to small polaron formation is studied within the framework of Extended Holstein model. It is assumed that electron moves along one-dimensional chain of ions and interacts with ions vibrations of neighboring chain via long-range density–displacement type force. By means of exact calculations, renormalized mass of nonadiabatic small polaron is obtained at strong coupling limit. Obtained results compared with those of small polaron mass of ordinary Holstein model. An effect of ions vibrations polarization on small polaron mass is addressed.


2013 ◽  
Vol 2013 ◽  
pp. 1-10 ◽  
Author(s):  
A. Ranjkesh ◽  
M. Ambrožič ◽  
G. Cordoyiannis ◽  
Z. Kutnjak ◽  
S. Kralj

We study the characteristics of nematic structures in a randomly perturbed nematic liquid crystal (LC) phase. We focus on the impact of the samples history on the universal behavior. The obtained results are of interest for every randomly perturbed system exhibiting a continuous symmetry-breaking phase transition. A semimicroscopic lattice simulation is used where the LC molecules are treated as cylindrically symmetric, rod-like objects interacting via a Lebwohl-Lasher (LL) interaction. Pure LC systems exhibit a first order phase transition into the orientationally ordered nematic phase atT=Tcon lowering the temperatureT. The orientational ordering of LC molecules is perturbed by the quenched, randomly distributed rod-likeimpuritiesof concentrationp. Their orientation is randomly distributed, and they are coupled with the LC molecules via an LL-type interaction. Only concentrations below the percolation threshold are considered. The key macroscopic characteristics of perturbed LC structures in the symmetry-broken nematic phase are analyzed for two qualitatively different histories atT≪Tc. We demonstrate that, for a weak enough interaction among the LC molecules andimpurities, qualitatively different history-dependent states could be obtained. These states could exhibit either short-range, quasi-long-range, or even long-range order.


Physica ◽  
1952 ◽  
Vol 18 (2) ◽  
pp. 1020-1022 ◽  
Author(s):  
E CAIANIELLO
Keyword(s):  

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