non-perturbative improvement of nhyp smeared fermions r. hoffmann in collaboration with a....
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Non-perturbative improvement of Non-perturbative improvement of nHYP smeared fermionsnHYP smeared fermions
R. HoffmannR. Hoffmann
In collaboration withIn collaboration with
A. Hasenfratz A. Hasenfratz andand S. Schaefer S. Schaefer
University of ColoradoUniversity of Colorado
PeakPeak
Mt. WilsonMt. WilsonWilson MesaWilson Mesa
WilsonWilson
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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Our action/setupOur action/setup
Plaquette gauge actionPlaquette gauge action
Wilson clover fermions coupled toWilson clover fermions coupled tonHYPnHYP smeared gauge field smeared gauge field [[→→ talk by S. Schaefer] talk by S. Schaefer]
SchrSchröödinger Functionaldinger Functional setup: setup:QCD with Dirichlet boundary conditions in time directionQCD with Dirichlet boundary conditions in time direction
[[ALPHA collaboration ALPHA collaboration 1992-…1992-…]] Provides Provides IRIR cutoff → in principle cutoff → in principle mmq q = 0= 0 is possible is possible
Useful for formulating non-perturbative Useful for formulating non-perturbative improvementimprovement and andrenormalizationrenormalization conditions conditions
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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““Smearing helps”… Want to quantify thisSmearing helps”… Want to quantify this
Use plaquette gauge action Use plaquette gauge action →→direct comparison to thin-link resultsdirect comparison to thin-link results
Preparation for SchrPreparation for Schrödinger Functionalödinger Functionalruns with runs with nHYPnHYP smearing smearing
We determine the clover coefficient nonWe determine the clover coefficient non -- perturbatively perturbatively using SF techniques in the quenched approximation…using SF techniques in the quenched approximation…
• Value of the clover coefficient
• Fluctuations of low Dirac modes (due to dislocations) → → appearance of exceptionals
• cutoff effects
[L[Lüscherüscher et al. 1996] et al. 1996]All thin link data we quote in the following is from All thin link data we quote in the following is from
Why?Why?
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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nHYP smearing in the SFnHYP smearing in the SF
Need prescription to combine the HYP constructionNeed prescription to combine the HYP constructionwith SF boundary conditionswith SF boundary conditions
Preserve boundary conditions through all levels in the Preserve boundary conditions through all levels in the construction:construction:
thin linkthin linknHYPnHYP link link IntermediateIntermediatelinkslinks
thin link boundary fieldSF boundary
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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Remark: smearing the tree-level BG fieldRemark: smearing the tree-level BG field
Any Any Abelian homogeneousAbelian homogeneous boundary field induces a boundary field induces atree level background fieldtree level background field
Thus Thus alwaysalways link+staples = link+staples =
Projection/Normalization reduces this to Projection/Normalization reduces this to
Any projected/normalized smearing leaves theAny projected/normalized smearing leaves thetree-level SF background field invarianttree-level SF background field invariant
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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Determining the clover coefficientDetermining the clover coefficient Follow the Follow the strategy strategy [L[Lüscherüscher et al. 1996] et al. 1996]
Use 2 PCAC quark masses in the SF w/ non-trivial BG fieldUse 2 PCAC quark masses in the SF w/ non-trivial BG fieldthat are improved w/o knowing that are improved w/o knowing ccAA
Simulate at several values of Simulate at several values of ccSWSW, find point where masses “agree”, find point where masses “agree”
All simulations at zero quark mass andAll simulations at zero quark mass and
Example: Example:
tree-level cutoff effect
SensitivitySensitivitysimilar to similar to thin linkthin link case case
thin @ thin @
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Results for Results for ccSWSW
N.P. N.P. ccswsw remains smallremains small
(even for coarse lattices)(even for coarse lattices)
1-loop 1-loop nHYPnHYP seems to be tiny seems to be tiny
(0.266 for (0.266 for thin linksthin links))
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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What about What about ccAA??
Several methods available, Several methods available, see e.g. see e.g. [D[Dürr & Della Morteürr & Della Morte 2003] 2003]
quenched strategy (2 quenched strategy (2 values) values)
slope methodslope method
gap method (wave functions)gap method (wave functions)
Already with Already with thin linksthin links: : cutoff effects small after cutoff effects small after ccSWSW is fixed is fixed
e.g. e.g. method with method with nHYPnHYP: : with increasing lattice spacing, cutoff effect actually with increasing lattice spacing, cutoff effect actually
decreasesdecreases from its tree level value… from its tree level value…
Typical Typical nHYPnHYP results at : results at : No good signal with No good signal with nHYPnHYP smearing after fixing smearing after fixing ccSWSW
Might require larger volume/wave functions…Might require larger volume/wave functions…
But: How good are we already with But: How good are we already with ccA A = 0 ?= 0 ?
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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Test Test II: :
Non-perturbative improvement of nHYP smeared Wilson fermions R. Hoffmann, lat07
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Test Test IIII: :
3 MeV band3 MeV band5 MeV band5 MeV band
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Test Test IIIIII: and : and
thin
nHYPIsovector vector current renormalization:Isovector vector current renormalization:
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Exceptional configurations?Exceptional configurations?
Quenched SF w/ Quenched SF w/ thin linkthin link clover requires clover requires
to safely simulate to safely simulate ……
,,
no BG field:no BG field:
Same at requires 25 MeV quark mass, Same at requires 25 MeV quark mass, but…but…
::
nHYPnHYP
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Conclusions / OutlookConclusions / Outlook Successfully used Successfully used nHYPnHYP smeared clover fermions in the smeared clover fermions in the
SchrSchröödinger functional framework (quenched for now)dinger functional framework (quenched for now)
As expected, the As expected, the non-perturbative non-perturbative ccSWSW remains close remains close
to 1 with to 1 with nHYPnHYP smeared clover fermions smeared clover fermions
Finite renormalization constantsFinite renormalization constants seem to be ~1 seem to be ~1
The problem with The problem with exceptional configurationsexceptional configurationsoccurs only at occurs only at muchmuch coarser lattice spacing coarser lattice spacing
Will be useful for non-perturbative Will be useful for non-perturbative improvementimprovement and and renormalizationrenormalization with dynamical fermions with dynamical fermions
NNf f > 0 is on the way…> 0 is on the way…