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The large mass of the ninth pseudoscalar meson, the $\eta^\prime$, is believed to arise from the combined effects of the axial anomaly and the gauge field topology present in QCD. We report a realistic, 2+1 flavor, lattice QCD calculation…

高能物理 - 格点 · 物理学 2010-12-28 N. H. Christ , C. Dawson , T. Izubuchi , C. Jung , Q. Liu , R. D. Mawhinney , C. T. Sachrajda , A. Soni , R. Zhou

We use the 1/N_c method to estimate electromagnetic contributions to vector meson masses and mixings. We identify several new sources of rho-omega mixing coming from short-distance effects. We comment on the extraction of quark masses from…

高能物理 - 唯象学 · 物理学 2009-10-28 J. Bijnens , P. Gosdzinsky

We determine the masses, the singlet and octet decay constants as well as the anomalous matrix elements of the $\eta$ and $\eta^\prime$ mesons in $N_f=2+1$ QCD\@. The results are obtained using twenty-one CLS ensembles of non-perturbatively…

高能物理 - 格点 · 物理学 2021-08-27 Gunnar S. Bali , Vladimir Braun , Sara Collins , Andreas Schäfer , Jakob Simeth

We present a lattice calculation of the $\eta$ and $\eta^{\prime}$ meson masses at the physical point and in the continuum limit, based on $N_f = 2+1+1$ flavors of rooted staggered quarks. Our analysis includes gauge ensembles at the…

We discuss in detail the extraction of hadronic mixing strengths from lattice studies. We apply this to the mixing of a scalar glueball and a scalar meson in the quenched approximation. We also measure correlations appropriate for…

高能物理 - 格点 · 物理学 2008-11-26 UKQCD Collaboration , Craig McNeile , Chris Michael

In a full QCD lattice study with $N_f = 2$ Wilson fermions, we seek to optimize the signals for the disconnected contributions to the matrix element of flavour-singlet operators between nucleon states, which are indicative for sea quark…

An extension of the Standard Model (SM) based on the non-Abelian discrete group $\Delta(27)$ is considered. The $\Delta(27)$ flavour symmetry is spontaneously broken only by gauge singlet scalar fields, therefore our model is free from any…

高能物理 - 唯象学 · 物理学 2015-03-18 Mohammed Abbas , Shaaban Khalil

The $\eta^{(\prime)}$-mesons in the quark-flavor basis are mixtures of two mesonic states $|\eta_{q}\rangle=|\bar u u+\bar d d\rangle/\sqrt 2$ and $|\eta_{s}\rangle=|\bar s s\rangle$. In the previous work, we have made a detailed study on…

高能物理 - 唯象学 · 物理学 2024-01-10 Dan-Dan Hu , Xing-Gang Wu , Hai-Bing Fu , Tao Zhong , Zai-Hui Wu , Long Zeng

I review to which extent the properties of pseudoscalar mesons can be understood in terms of the underlying quark (and eventually gluon) structure. Special emphasis is put on the progress in our understanding of eta-eta' mixing.…

高能物理 - 唯象学 · 物理学 2014-11-17 Thorsten Feldmann

We analyze power-suppressed contributions to singlet pseudoscalar $\eta$ and $\eta^{\prime}$ meson transition form factors. These corrections stem from endpoint singularities and help improve the agreement between QCD theory and the…

高能物理 - 唯象学 · 物理学 2007-05-23 N. G. Stefanis , S. S. Agaev

Flavor singlet combinations of quark operators ${\cal{O}}_S^{\Gamma} = \bar{u}\Gamma u + \bar{d}\Gamma d + \bar{s}\Gamma s$ contribute to many important physical observables in the low energy region of QCD. Experimentally one finds the…

高能物理 - 格点 · 物理学 2007-05-23 S. Güsken

We discuss a new mass matrix with specific texture zeros for the quarks. The three flavor mixing angles for the quarks are functions of the quark masses and can be calculated. The following ratios among CKM matrix elements are given by…

高能物理 - 唯象学 · 物理学 2021-05-12 Harald Fritzsch

We calculate for the first time the form factors of the semi-leptonic decays of the $D_s$ meson to $\eta$ and $\eta^\prime$ using lattice techniques. As a by-product of the calculation we obtain the masses and leading distribution…

高能物理 - 格点 · 物理学 2015-06-22 Gunnar S. Bali , Sara Collins , Stephan Durr , Issaku Kanamori

We study the finite supersymmetric loop corrections to fermion masses and mixing matrices in the generic MSSM. In this context the effects of non-decoupling chirally-enhanced self-energies are studied beyond leading order in perturbation…

高能物理 - 唯象学 · 物理学 2015-03-13 Andreas Crivellin , Jennifer Girrbach

Accurately calculating the mass of flavor-singlet meson states from numerical lattice simulations is an important milestone for lattice QCD. Careful measurement of the full pseudoscalar flavor-singlet propagator is also a crucial step in…

高能物理 - 格点 · 物理学 2008-11-26 Eric B. Gregory , Alan Irving , Chris M. Richards , Craig McNeile , Alistair Hart

It has been realized for a long time that knowing the eta and eta^prime wave functions in terms of quark and gluon components probes our understanding of non-perturbative QCD dynamics. Great effort has been given to this challenge -- yet no…

高能物理 - 唯象学 · 物理学 2012-02-03 Camilla Di Donato , Giulia Ricciardi , Ikaros Bigi

The pseudo-scalar flavor-singlet meson mixes with two gluons. A dimensional argument by Kogut and Susskind shows that this can screen the Goldstone pole of the chiral limit in this channel, if the gluon correlations are infrared enhanced.…

高能物理 - 唯象学 · 物理学 2009-10-30 Lorenz von Smekal , Almut Mecke , Reinhard Alkofer

The large mass of the $\eta'$ meson indicates that a sizeable gluon component is present in the meson wave function. However, the $\chi_{c0}$ and $\chi_{c2}$ decays to $\eta'$ mesons, which proceed via a purely gluonic intermediate state…

高能物理 - 唯象学 · 物理学 2017-05-24 L. A. Harland-Lang , V. A. Khoze , M. G. Ryskin , A. G. Shuvaev

U_A(1) symmetry breaking is studied by introducing the flavor mixing interaction proposed by Kobayashi, Maskawa and 't Hooft. Combining the one gluon exchange interaction, the rainbow like Schwinger-Dyson equation and the ladder like…

高能物理 - 唯象学 · 物理学 2016-09-06 K. Naito , Y. Nemoto , M. Takizawa , K. Yoshida , M. Oka

Numerical correlations between fermion masses and mixings could indicate the presence of a flavor symmetry at high energies. In general, the search for these correlations using low-energy data requires an estimate of leading-log radiative…

高能物理 - 唯象学 · 物理学 2009-10-28 J. A. Aguilar-Saavedra , M. Masip