scholarly journals Fast algorithms for chiral fermions in 2 dimensions

2018 ◽  
Vol 175 ◽  
pp. 14005
Author(s):  
Dafina Hyka (Xhako) ◽  
Rudina Osmanaj (Zeqirllari)

In lattice QCD simulations the formulation of the theory in lattice should be chiral in order that symmetry breaking happens dynamically from interactions. In order to guarantee this symmetry on the lattice one uses overlap and domain wall fermions. On the other hand high computational cost of lattice QCD simulations with overlap or domain wall fermions remains a major obstacle of research in the field of elementary particles. We have developed the preconditioned GMRESR algorithm as fast inverting algorithm for chiral fermions in U(1) lattice gauge theory. In this algorithm we used the geometric multigrid idea along the extra dimension.The main result of this work is that the preconditioned GMRESR is capable to accelerate the convergence 2 to 12 times faster than the other optimal algorithms (SHUMR) for different coupling constant and lattice 32x32. Also, in this paper we tested it for larger lattice size 64x64. From the results of simulations we can see that our algorithm is faster than SHUMR. This is a very promising result that this algorithm can be adapted also in 4 dimension.

2011 ◽  
Author(s):  
Yao-Yuan Mao ◽  
Ting-Wai Chiu ◽  
Tung-Han Hsieh ◽  
Kenji Ogawa

2012 ◽  
Vol 86 (9) ◽  
Author(s):  
A. Bazavov ◽  
Tanmoy Bhattacharya ◽  
Michael I. Buchoff ◽  
Michael Cheng ◽  
N. H. Christ ◽  
...  

2018 ◽  
Vol 175 ◽  
pp. 10006 ◽  
Author(s):  
Renwick Hudspith ◽  
Randy Lewis ◽  
Kim Maltman ◽  
Eigo Shintani

We present our result for the strong coupling constant computed from the u-d vector Hadronic Vacuum Polarisation function. We use nf = 2 + 1 flavours of Domain Wall fermions at 3 lattice spacings, generated by the RBC-UKQCD collaboration. We identify several possible pitfalls in this method for determining the coupling and illustrate how to resolve them.


1994 ◽  
Vol 422 (1-2) ◽  
pp. 382-396 ◽  
Author(s):  
G.M. de Divitiis ◽  
R. Frezzotti ◽  
M. Guagnelli ◽  
R. Petronzio

2003 ◽  
Vol 68 (5) ◽  
Author(s):  
S. Sasaki ◽  
K. Orginos ◽  
S. Ohta ◽  
T. Blum

2020 ◽  
Vol 2020 (4) ◽  
Author(s):  
Hidenori Fukaya ◽  
Naoki Kawai ◽  
Yoshiyuki Matsuki ◽  
Makito Mori ◽  
Katsumasa Nakayama ◽  
...  

Abstract We propose a nonperturbative formulation of the Atiyah–Patodi–Singer (APS) index in lattice gauge theory in four dimensions, in which the index is given by the $\eta$ invariant of the domain-wall Dirac operator. Our definition of the index is always an integer with a finite lattice spacing. To verify this proposal, using the eigenmode set of the free domain-wall fermion we perturbatively show in the continuum limit that the curvature term in the APS theorem appears as the contribution from the massive bulk extended modes, while the boundary $\eta$ invariant comes entirely from the massless edge-localized modes.


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