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    Thermal Quench at Finite t'Hooft Coupling

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    Using holography we have studied thermal electric field quench for infinite and finite t'Hooft coupling constant. The set-up we consider here is D7-brane embedded in (α′\alpha' corrected) AdS-black hole background. It is well-known that due to a time-dependent electric field on the probe brane, a time-dependent current will be produced and it will finally relax to its equilibrium value. We have studied the effect of different parameters of the system on equilibration time. As the most important results, we have observed a universal behaviour in the rescaled equilibration time in the very fast quench regime for different values of the temperature and α′\alpha' correction parameter. It seems that in the slow quench regime the system behaves adiabatically. We have also observed that the equilibration time decreases in finite t'Hooft coupling limit.Comment: 6 pages, 9 figure

    On the Unit Graph of a Noncommutative Ring

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    Let RR be a ring (not necessary commutative) with non-zero identity. The unit graph of RR, denoted by G(R)G(R), is a graph with elements of RR as its vertices and two distinct vertices aa and bb are adjacent if and only if a+ba+b is a unit element of RR. It was proved that if RR is a commutative ring and \fm is a maximal ideal of RR such that |R/\fm|=2, then G(R)G(R) is a complete bipartite graph if and only if (R, \fm) is a local ring. In this paper we generalize this result by showing that if RR is a ring (not necessary commutative), then G(R)G(R) is a complete rr-partite graph if and only if (R, \fm) is a local ring and r=∣R/m∣=2nr=|R/m|=2^n, for some n∈Nn \in \N or RR is a finite field. Among other results we show that if RR is a left Artinian ring, 2∈U(R)2 \in U(R) and the clique number of G(R)G(R) is finite, then RR is a finite ring.Comment: 6 pages. To appear in Algebra Colloquiu
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