High Precision. Charm Physics. HISQ quarks
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1 f % f K High Precision m Charm Physics $ with m N m Ds m D m D * HISQ quarks - m s D s m " - m #c "(1P-1S) 2m Bs,av -m! Christine m Davies Bc E. Follana, G. P. Lepage, R. Horgan, K. Hornbostel, C. McNeile, J.Shigemitsu, H. Trottier HPQCD collaboration!(3s-1s)!(2p-1s)!(1p-1s)!(1d-1s) Quenched with sea quarks
2 Charm quarks in lattice QCD - heavy or light? Relativistic light quark advantages: E sim = m PCAC relation (if enough chiral symmetry) gives Z = 1 for decay constants same action as for u, d, s. Can take ratios to light physics. Key issue is discretisation errors: m c a 0.4, (m c a) 2 0.2, α s (m c a) , (m c a) Need to remove all of these errors for precision results
3 Improved staggered formalism = c1 c3 c5 c7 c5 (Fat link) Naik term removes treelevel a 2 errors. Smeared link reduces tasteexchange errors α s a 2 c3 = (Naik) Highly Improved staggered formalism Second level of smearing (with polar projection) reduces taste-exchange errors further. Change Naik coefficient to remove leading (am c ) 4 errors (check speed of light)
4 Used HISQ valence light and charm quarks on MILC very coarse, coarse and fine configs with imp.stagg sea quarks Excellent statistical accuracy from random wall sources (as used by MILC for light mesons) D s t a i e M it + ( 1) t a ip e M ipt correlator/(fit ground state) signal noise = e 0.133GeV T Allows systematic errors to be studied in detail
5 Calculate D/Ds masses and decay constants very precisely NO free parameters since fixed from m c η c 2 Mass (GeV) 1.9 M Ds M D Exp t m u/d /m s E.Follana et al, [hep-lat]
6 2008 Improved accuracy from CLEO-c Determine decay constant from leptonic rate and taking Vcs=Vud, Vcd=Vus agree disagree Belle EPS2007 BaBar hep-ex/ CLEO-c FPCP08 HPQCD HISQ on MILC cfgs, [hep-lat] FNAL/MILC on MILC cfgs, LAT07 prelim different expts using different channels two different lattice QCD methods New physics? see Kronfeld talk Friday 2:50pm
7 Further checks of lattice calculations important Spectrum hyperfine splitting / GeV link vec - goldstone Charmonium Hyperfine Fine Coarse Very coarse Hyperfine splitting between vector and pseudoscalar No dependence on sea quark mass m u/d /m s
8 Dependence on a clearly visible - some of this is a tasteexchange effect hyperfine splitting / GeV Comparison to expt complicated few MeV e.m and annihiln corrns. Lattice error dominated by square of absolute scale error - 3% see Kendall talk, Thursday 8:50am Hyperfine splittings 1-link! local! 1-link D s * local D s * expt D s corrected expt! (a/r 1 ) 2 Prelim. result on MILC superfine a=0.06fm
9 Further taste effects Taste-split / MeV Taste-splittings vs a 2! c HISQ locng - gold! c DHISQ locng - gold! c THISQ locng - gold (a/r 1 ) 2 Double HISQ reduces tasteexchange discretisation errors further - Treble HISQ worse again Too much smearing makes disc. errors worse again
10 Improved scaling of hyperfine splitting also seen in Double HISQ hyperfine splitting / GeV All taste versions converging with a 2 to same answer charmonium hyperfine splitting HISQ 1-link! - goldstone HISQ local! - goldstone HISQ local! - local ng corrected expt! DHISQ local! - goldstone DHISQ local! - local ng (a/r 1 ) 2
11 2. Decay constants Decay constant / GeV Pseudoscalar decay constants Superfine Fine Coarse Very coarse η c η s Again, no sea quark mass dependence. Lattice spacing dependence evident for charm m u/d /m s
12 Vector decay constants f V m V =< 0 J V > Decay constant / GeV Γ e + e = 4π 3 α2 QEDe 2 Q f 2 V m V f! loc f! 1-link expt f " 1-link f " loc (a/r 1 ) 2 nonpert renormln using t-moments of JJ correlator (Lepage talk) error = 4% at a=0. renormalise using 1-loop pert. th. Different tastes heading towards agreement with expt - need to complete calc. with conserved vector current
13 Conclusions HISQ allows us to do charm physics accurately f Ds = 241(3)MeV 3σ from expt All other charmonium and charm-light results agree with expt at few % level. Future: Similarly accurate 3pt calculations See also: for 1% accurate mc Lepage talk, Thursday 9:10am Allison talk, Thursday 9:30am Bazavov talk, Tuesday 5:00pm, dynamical HISQ
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