AbstractWe compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-leading logarithmic approximation using the nonrelativistic renormalization group. We predict the mass difference of the vector and pseudoscalar charm-bottom mesons to be M(B∗c)−M(Bc)=65±24 (th)+19−16(δαs) MeV
The hyperfine splittings in heavy quarkonia are studied using new experimental data on the di-electr...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
AbstractWe compute the hyperfine splitting in a heavy quarkonium composed of different flavors in ne...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperne splitting usin...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting, u...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
AbstractThe hyperfine splittings in heavy quarkonia are studied using new experimental data on the d...
We present a calculation of the hyperfine splittings in bottomonium using lattice nonrelativistic QC...
We present a calculation of the hyperfine splittings in bottomonium using lattice nonrelativistic QC...
The hyperfine splittings in heavy quarkonia are studied using new experimental data on the di-electr...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
AbstractWe compute the hyperfine splitting in a heavy quarkonium composed of different flavors in ne...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperne splitting usin...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting, u...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
AbstractThe hyperfine splittings in heavy quarkonia are studied using new experimental data on the d...
We present a calculation of the hyperfine splittings in bottomonium using lattice nonrelativistic QC...
We present a calculation of the hyperfine splittings in bottomonium using lattice nonrelativistic QC...
The hyperfine splittings in heavy quarkonia are studied using new experimental data on the di-electr...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
Abstract We determine the charm and bottom quark masses using the N3LO perturbative expression of th...
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