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Preliminary results in unquenched numerical stochastic perturbation theory

✍ Scribed by F. Di Renzo; A. Mantovi; V. Miccio; L. Scorzato


Publisher
Elsevier Science
Year
2004
Tongue
English
Weight
272 KB
Volume
129-130
Category
Article
ISSN
0920-5632

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✦ Synopsis


Introducing fermionic loops contributions in Numerical Stochastic Perturbation

Theory was mainly motivated by the proposal to compute 2-3 loops for renormalization constants (and improvement coefficients). This is feasible because the computational overhead of unquenching NSPT is by far lower than for non perturbative simulations. We report on first, preliminary results for the quark propagator (basically the third loop for the critical mass) and discuss the status of the computation of other quantities.


πŸ“œ SIMILAR VOLUMES


Unquenched numerical stochastic perturba
✍ F. Di Renzo; V. Miccio; L. Scorzato πŸ“‚ Article πŸ“… 2003 πŸ› Elsevier Science 🌐 English βš– 242 KB

The inclusion of fermionic loops contribution in Numerical Stochastic Perturbation Theory (NSPT) h;t~ a nice feature: it does not cost so much (provided only that an FFT can be implemented in a fairly efficient, way). Focusing on Lattice SU(3), we report on the performance of the current implementat

Quenched and unquenched chiral perturbat
✍ P.H. Damgaard πŸ“‚ Article πŸ“… 2004 πŸ› Elsevier Science 🌐 English βš– 627 KB

The chiral limit of finite-volume &CD is the e-regime of the theory. We discuss how this regime can be used for determining low-energy observables of QCD by means of comparisons between lattice simulations and quenched and unquenched chiral perturbation theory. The quenched theory suffers in the e-r

Four loop stochastic perturbation theory
✍ F. Di Renzo; A. Mantovi; V. Miccio; Y. SchrΓΆder πŸ“‚ Article πŸ“… 2004 πŸ› Elsevier Science 🌐 English βš– 277 KB

## Dimensional reduction is a key issue in finite temperature field theory. For example, when following the QCD Free Energy from low to high scales across the critical temperature, ultrasoft degrees of freedom can be captured by a 3d SU(3) pure gauge theory. For such a theory a complete perturbati