scholarly journals Simulating the scalar field on the fuzzy sphere

Author(s):  
Fernando Garcia Flores ◽  
Denjoe O'Connor ◽  
X. Martin
Keyword(s):  
1998 ◽  
Vol 13 (19) ◽  
pp. 3235-3243 ◽  
Author(s):  
URSULA CAROW-WATAMURA ◽  
SATOSHI WATAMURA

We find that there is an alternative possibility to define the chirality operator on the fuzzy sphere, due to the ambiguity of the operator ordering. Adopting this new chirality operator and the corresponding Dirac operator, we define Connes' spectral triple on the fuzzy sphere and the differential calculus. The differential calculus based on this new spectral triple is simplified considerably. Using this formulation the action of the scalar field is derived.


2003 ◽  
Vol 18 (33n35) ◽  
pp. 2389-2396 ◽  
Author(s):  
XAVIER MARTIN

Fuzzy spaces provide a new approximation scheme using (non–commutative) matrix algebras to approximate the algebra of function of the continuous space. This paper describes how to implement a numerical scheme based on a fuzzy space approximation. In this first attempt, the simplest fuzzy space and field theory, respectively the fuzzy two–sphere and the real scalar field, are used to simulate the real scalar field on the plane. Along the way, this method is compared to its traditional lattice discretisation equivalent.


2012 ◽  
Vol 27 (14) ◽  
pp. 1250082 ◽  
Author(s):  
S. DIGAL ◽  
T. R. GOVINDARAJAN

We study the spontaneous symmetry breaking of O(3) scalar field on a fuzzy sphere [Formula: see text]. We find that the fluctuations in the background of topological configurations are finite. This is in contrast to the fluctuations around a uniform configuration which diverge, due to Mermin–Wagner–Hohenberg–Coleman theorem, leading to the decay of the condensate. Interesting implications of enhanced topological stability of the configurations are pointed out.


2008 ◽  
Vol 23 (21) ◽  
pp. 1781-1791 ◽  
Author(s):  
C. R. DAS ◽  
S. DIGAL ◽  
T. R. GOVINDARAJAN

We study finite temperature phase transition of neutral scalar field on a fuzzy sphere using Monte Carlo simulations. We work with the zero mode in the temporal directions, while the effects of the higher modes are taken care by the temperature dependence of r. In the numerical calculations we use "pseudo-heatbath" method which reduces the auto-correlation considerably. Our results agree with the conventional calculations. We report some new results which show the presence of meta-stable states, first order symmetry breaking transition and existence of multiple triple points in the phase diagram..


2018 ◽  
Vol 2018 (10) ◽  
Author(s):  
Samuel Kováčik ◽  
Denjoe O’Connor

2009 ◽  
Vol 24 (33) ◽  
pp. 2693-2701 ◽  
Author(s):  
C. R. DAS ◽  
S. DIGAL ◽  
T. R. GOVINDARAJAN

We study and analyse the questions regarding breakdown of global symmetry on noncommutative sphere. We demonstrate this by considering a complex scalar field on a fuzzy sphere and isolating Goldstone modes. We discuss the role of nonlocal interactions present in these through geometrical considerations.


2016 ◽  
Vol 2016 (2) ◽  
pp. 023B03 ◽  
Author(s):  
Shizuka Okuno ◽  
Mariko Suzuki ◽  
Asato Tsuchiya

2012 ◽  
Vol 27 (24) ◽  
pp. 1250137 ◽  
Author(s):  
FEDELE LIZZI ◽  
BERNARDINO SPISSO

The fuzzy disk is a discretization of the algebra of functions on the two-dimensional disk using finite matrices which preserves the action of the rotation group. We define a φ4 scalar field theory on it and analyze numerically three different limits for the rank of the matrix going to infinity. The numerical simulations reveal three different phases: uniform and disordered phases already present in the commutative scalar field theory and a nonuniform ordered phase as noncommutative effects. We have computed the transition curves between phases and their scaling. This is in agreement with studies on the fuzzy sphere, although the speed of convergence for the disk seems to be better. We have also performed the limits for the theory in the cases of the theory going to the commutative plane or commutative disk. In this case the theory behaves differently, showing the intimate relationship between the nonuniform phase and noncommutative geometry.


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