Minimizing storage in implementations of the overlap lattice-Dirac operator

被引:24
作者
Neuberger, H [1 ]
机构
[1] Rutgers State Univ, Dept Phys & Astron, Piscataway, NJ 08855 USA
来源
INTERNATIONAL JOURNAL OF MODERN PHYSICS C | 1999年 / 10卷 / 06期
关键词
lattice gauge theory; overlap lattice-Dirac operator; storage;
D O I
10.1142/S012918319900084X
中图分类号
TP39 [计算机的应用];
学科分类号
081203 ; 0835 ;
摘要
The overlap lattice-Dirac operator contains the sign function epsilon(H). Recent practical implementations replace epsilon(H) by a ratio of polynomials, HPn(H-2)/Q(n)(H-2), and require storage of 2n + 2 large vectors. Here I show that one can use only four large vectors at the cost of executing the core conjugate algorithm twice. The slow-down might be less than by a factor of 2, depending on the architecture of the computer one uses.
引用
收藏
页码:1051 / 1057
页数:7
相关论文
共 13 条
[1]  
[Anonymous], MATRIX COMPUTATIONS
[2]  
BORICI A, HEPLAT9810064
[3]   Topological charge and the spectrum of exactly massless fermions on the lattice [J].
Chiu, TW .
PHYSICAL REVIEW D, 1998, 58 (07)
[4]  
Cullum J. K., 1985, LANCZOS ALGORITHMS L, V1
[5]   QCDF90: A set of Fortran 90 modules for a high-level, efficient implementation of QCD simulations [J].
Dasgupta, I ;
Levi, AR ;
Lubicz, V ;
Rebbi, C .
COMPUTER PHYSICS COMMUNICATIONS, 1996, 98 (03) :365-397
[6]  
EDWARDS RG, HEPLAT9807017
[7]  
HIGHAM NJ, 1993, P PUR APPL LIN ALG N
[8]  
Jegerlehner B., HEPLAT9612014
[9]   A SIMULATION OF THE SCHWINGER MODEL IN THE OVERLAP FORMALISM [J].
NARAYANAN, R ;
NEUBERGER, H ;
VRANAS, P .
PHYSICS LETTERS B, 1995, 353 (04) :507-512
[10]   INFINITELY MANY REGULATOR FIELDS FOR CHIRAL FERMIONS [J].
NARAYANAN, R ;
NEUBERGER, H .
PHYSICS LETTERS B, 1993, 302 (01) :62-69