| Home > External Publications > Vita Publications > Numerical methods for the QCDd overlap operator. I. Sign-function and error bounds > print |
| 001 | 860300 | ||
| 005 | 20200914102037.0 | ||
| 024 | 7 | _ | |a 10.1016/S0010-4655(02)00455-1 |2 doi |
| 024 | 7 | _ | |a 0010-4655 |2 ISSN |
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| 024 | 7 | _ | |a 1879-2944 |2 ISSN |
| 037 | _ | _ | |a FZJ-2019-01075 |
| 082 | _ | _ | |a 530 |
| 100 | 1 | _ | |a van den Eshof, J. |0 P:(DE-HGF)0 |b 0 |
| 245 | _ | _ | |a Numerical methods for the QCDd overlap operator. I. Sign-function and error bounds |
| 260 | _ | _ | |a Amsterdam |c 2002 |b North Holland Publ. Co. |
| 336 | 7 | _ | |a article |2 DRIVER |
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| 336 | 7 | _ | |a Journal Article |0 0 |2 EndNote |
| 520 | _ | _ | |a The numerical and computational aspects of the overlap formalism in lattice quantum chromodynamics are extremely demanding due to a matrix–vector product that involves the sign function of the Hermitian Wilson matrix. In this paper we investigate several methods to compute the product of the matrix sign-function with a vector, in particular Lanczos based methods and partial fraction expansion methods. Our goal is two-fold: we give realistic comparisons between known methods together with novel approaches and we present error bounds which allow to guarantee a given accuracy when terminating the Lanczos method and the multishift-CG solver, applied within the partial fraction expansion methods. |
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| 700 | 1 | _ | |a Frommer, A. |0 P:(DE-HGF)0 |b 1 |
| 700 | 1 | _ | |a Lippert, Th. |0 P:(DE-Juel1)132179 |b 2 |u fzj |
| 700 | 1 | _ | |a Schilling, K. |0 P:(DE-HGF)0 |b 3 |
| 700 | 1 | _ | |a van der Vorst, H. A. |0 P:(DE-HGF)0 |b 4 |
| 773 | _ | _ | |a 10.1016/S0010-4655(02)00455-1 |g Vol. 146, no. 2, p. 203 - 224 |0 PERI:(DE-600)1466511-6 |n 2 |p 203 - 224 |t Computer physics communications |v 146 |y 2002 |x 0010-4655 |
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