Size of the pion from full lattice QCD with physical u, d, s and c quarks
نویسندگان
چکیده
We present the first calculation of the electromagnetic form factor of the π meson at physical light quark masses. We use configurations generated by the MILC Collaboration including the effect of u, d, s and c sea quarks with the highly improved staggered quark formalism. We work at three values of the lattice spacing on large volumes and with u=d quark masses going down to the physical value. We study scalar and vector form factors for a range in spacelike q from 0.0 to −0.13 GeV and from their shape we extract mean square radii. Our vector form factor agrees well with experiment and we find hriV 1⁄4 0.403ð18Þð6Þ fm. For the scalar form factor we include quark-line disconnected contributions which have a significant impact on the radius. We give the first results for SU(3) flavor-singlet and flavor-octet scalar mean square radii, obtaining hr2i S 1⁄4 0.506ð38Þð53Þ fm and hr2ioctet S 1⁄4 0.431ð38Þð46Þ fm. We discuss the comparison with expectations from chiral perturbation theory.
منابع مشابه
The spectrum of static-light baryons in twisted mass lattice QCD
We compute the static-light baryon spectrum with N f = 2 flavors of sea quarks using Wilson twisted mass lattice QCD. As light valence quarks we consider quarks, which have the same mass as the sea quarks with corresponding pion masses in the range 340MeV∼mPS ∼525MeV, as well as partially quenched quarks, which have the mass of the physical s quark. We extract masses of states with isospin I = ...
متن کاملB → πlν at zero recoil from lattice QCD with physical u=d quarks
The exclusive semileptonic decay B → πlν is a key process for the determination of the CabibboKobayashi-Maskawa matrix element Vub from the comparison of experimental rates as a function of q with theoretically determined form factors. The sensitivity of the form factors to the u=d quark mass has meant significant systematic uncertainties in lattice QCD calculations at unphysically heavy pion m...
متن کاملStrong-Isospin Breaking in the Neutron-Proton Mass Difference
We determine the strong-isospin violating component of the neutron-proton mass difference from fully-dynamical lattice QCD and partially-quenched QCD calculations of the nucleon mass, constrained by partially-quenched chiral perturbation theory at one-loop level. The lattice calculations were performed with domain-wall valence quarks on MILC lattices with rooted staggered sea-quarks at a lattic...
متن کاملLattice QCD ensembles with four flavors of highly improved staggered quarks
We present results from our simulations of quantum chromodynamics (QCD) with four flavors of quarks: u, d, s, and c. These simulations are performed with a one-loop Symanzik improved gauge action, and the highly improved staggered quark (HISQ) action. We are generating gauge configurations with four values of the lattice spacing ranging from 0.06 fm to 0.15 fm, and three values of the light qua...
متن کاملFinite - Volume Partially - Quenched Two - Pion Amplitudes in the I = 0 Channel
We present a study of the finite-volume two-pion matrix elements and correlation functions of the I = 0 scalar operator, in full and partially quenched QCD, at one-loop order in chiral perturbation theory. In partially quenched QCD, when the sea and valence light quark masses are not equal, the lack of unitarity leads to the same inconsistencies as in quenched QCD and the matrix elements cannot...
متن کامل