We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting, using the nonrelativistic renormalization group. On the basis of this result, we predict the mass of the η b meson to be M ( η b ) = 9421 ± 11 ( th ) + 9 − 8 ( δ α s ) MeV . The experimental measurement of M ( η b ) with a few MeV error would be sufficient to determine α s ( M Z ) with an accuracy of ± 0.003 . For the hyperfine splitting in charmonium, the use of the nonrelativistic renormalization group brings the perturbative prediction significantly closer to the experimental figure
We compute the energy levels of some of the lower-lying heavy quarkonium states perturbatively up to...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
AbstractWe compute the energy levels of some of the lower-lying heavy quarkonium states perturbative...
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...
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 hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
A recently proposed strictly phenomenological static quark-antiquark potential belonging to the gene...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We complete the leading-log renormalization group scaling of the nonrelativistic (NRQCD) Lagrangian ...
We compute the energy levels of some of the lower-lying heavy quarkonium states perturbatively up to...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
AbstractWe compute the energy levels of some of the lower-lying heavy quarkonium states perturbative...
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...
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 hyperfine splitting us...
We sum up the next-to-leading logarithmic corrections to the heavy-quarkonium hyperfine splitting us...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
A recently proposed strictly phenomenological static quark-antiquark potential belonging to the gene...
We compute the hyperfine splitting in a heavy quarkonium composed of different flavors in next-to-le...
We complete the leading-log renormalization group scaling of the nonrelativistic (NRQCD) Lagrangian ...
We compute the energy levels of some of the lower-lying heavy quarkonium states perturbatively up to...
We include two loop, relativistic one loop and second order relativistic tree level corrections, plu...
AbstractWe compute the energy levels of some of the lower-lying heavy quarkonium states perturbative...