We show that the nonperturbative solution of the SU(2) linear sigma model field theory requires color number Nc=3. Also, we show that the three-point and four-point functions bootstrap (or nonperturbatively ``shrink'') in the chiral limit to the tree amplitudes. Independently, we show that a chiral phase transition for Nf=2 requires Tc=180 MeV, consistent with the computer lattice value (173 +/- 8 MeV)
AbstractRecent data on B→pp̄K, K0ππ and KKK hint at a ∼2.3 GeV object recoiling against a kaon. This...
It is shown that a 25(20)% difference between the decay constants $f_{D_s}(f_{B_s})$ and $f_D(f_B)$ ...
AbstractWe use the AdS/QCD distribution amplitudes for light mesons to calculate the transition form...
AbstractIn this Letter, we investigate the radiative leptonic decays D−(s)→γℓν̄ (ℓ=e,μ) at tree leve...
AbstractThe quark–gluon mixed condensate g〈q̄σμνFμνq〉 is calculated in the Gaussian approximation of...
AbstractThe couplings of the η and η′ mesons to the nucleon are obtained from the UA(1) Goldberger–T...
AbstractRecent experimental results for the ratio of the branching fractions of B¯→D(⁎)τν¯τ and B¯→D...
The hierarchy among the radiative γ(π0,η,η′) decay channels for the ψ′ looks quite different from th...
AbstractThe rare decay B¯d0→J/ψϕ can proceed via four distinct mechanisms: (i) production of the ϕ v...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
AbstractThe hierarchy among the radiative γ(π0,η,η′) decay channels for the ψ′ looks quite different...
AbstractIn previous work it has been shown that, either from a sum rule for the subleading Isgur–Wis...
Using proton-proton collision data corresponding to an integrated luminosity of 3.0 fb−1, recorded b...
We correct our treatment of decays of the lightest chargino to final states containing the lightest ...
We estimate the quantity |f_eta'^(c)| which is associated with the charm content of eta' meson from ...
AbstractRecent data on B→pp̄K, K0ππ and KKK hint at a ∼2.3 GeV object recoiling against a kaon. This...
It is shown that a 25(20)% difference between the decay constants $f_{D_s}(f_{B_s})$ and $f_D(f_B)$ ...
AbstractWe use the AdS/QCD distribution amplitudes for light mesons to calculate the transition form...
AbstractIn this Letter, we investigate the radiative leptonic decays D−(s)→γℓν̄ (ℓ=e,μ) at tree leve...
AbstractThe quark–gluon mixed condensate g〈q̄σμνFμνq〉 is calculated in the Gaussian approximation of...
AbstractThe couplings of the η and η′ mesons to the nucleon are obtained from the UA(1) Goldberger–T...
AbstractRecent experimental results for the ratio of the branching fractions of B¯→D(⁎)τν¯τ and B¯→D...
The hierarchy among the radiative γ(π0,η,η′) decay channels for the ψ′ looks quite different from th...
AbstractThe rare decay B¯d0→J/ψϕ can proceed via four distinct mechanisms: (i) production of the ϕ v...
Final state quark-antiquark interactions give origin to non zero values of the off-diagonal element ...
AbstractThe hierarchy among the radiative γ(π0,η,η′) decay channels for the ψ′ looks quite different...
AbstractIn previous work it has been shown that, either from a sum rule for the subleading Isgur–Wis...
Using proton-proton collision data corresponding to an integrated luminosity of 3.0 fb−1, recorded b...
We correct our treatment of decays of the lightest chargino to final states containing the lightest ...
We estimate the quantity |f_eta'^(c)| which is associated with the charm content of eta' meson from ...
AbstractRecent data on B→pp̄K, K0ππ and KKK hint at a ∼2.3 GeV object recoiling against a kaon. This...
It is shown that a 25(20)% difference between the decay constants $f_{D_s}(f_{B_s})$ and $f_D(f_B)$ ...
AbstractWe use the AdS/QCD distribution amplitudes for light mesons to calculate the transition form...