AbstractWe perform a finite energy sum rule analysis of the flavor ud two-point V–A current correlator, ΔΠ(Q2). The analysis, which is performed using both the ALEPH and OPAL databases for the V–A spectral function, Δρ, allows us to extract the dimension six V–A OPE coefficient, a6, which is related to the matrix element of the electroweak penguin operator, Q8, by chiral symmetry. The result for a6 leads directly to the improved (chiral limit) determination ϵ′/ϵ=(−15.0±2.7)×10−4. Determination of higher dimension OPE contributions also allows us to perform an independent test using a low-scale constrained dispersive analysis, which provides a highly nontrivial consistency check of the results
A search is performed for the as yet unobserved baryonic Λ0 b → Λη 0 and Λ 0 b → Λη decays with...
Motivated by the LHCb measurement, we analyze the Bs→π+π−ℓ+ℓ− decay in the kinematics region where t...
We show how the isospin vector and axialvector current spectral functions V,3 and A,3 can be used to...
AbstractThe couplings of the η and η′ mesons to the nucleon are obtained from the UA(1) Goldberger–T...
AbstractNature might be kinder than previously thought as far as ε′/ε is concerned. We show that the...
We show how the isospin vector and axialvector current spectral functions rho_V and rho_A can be use...
AbstractA theoretical description of the differential decay spectrum for the decay τ−→ντKSπ−, which ...
Three years after the completion of the next-to-leading order calculation, the status of the theoret...
AbstractThe anomaly in the vacuum expectation value of the product of axial and two vector currents ...
AbstractThe pion scalar radius is given by 〈rS2〉=(6/π)∫4Mπ2∞dsδS(s)/s2, with δS the phase of the sca...
We propose to use rich informations on pi p total cross sections below N=10 GeV in order to investig...
We show that the nonperturbative solution of the SU(2) linear sigma model field theory requires colo...
AbstractThe quark–gluon mixed condensate g〈q̄σμνFμνq〉 is calculated in the Gaussian approximation of...
We use general relations between the Transition Distribution Amplitudes (TDAs), entering the descrip...
The η′ meson is associated with the U(1) anomaly. In this paper, a successful effective chiral theor...
A search is performed for the as yet unobserved baryonic Λ0 b → Λη 0 and Λ 0 b → Λη decays with...
Motivated by the LHCb measurement, we analyze the Bs→π+π−ℓ+ℓ− decay in the kinematics region where t...
We show how the isospin vector and axialvector current spectral functions V,3 and A,3 can be used to...
AbstractThe couplings of the η and η′ mesons to the nucleon are obtained from the UA(1) Goldberger–T...
AbstractNature might be kinder than previously thought as far as ε′/ε is concerned. We show that the...
We show how the isospin vector and axialvector current spectral functions rho_V and rho_A can be use...
AbstractA theoretical description of the differential decay spectrum for the decay τ−→ντKSπ−, which ...
Three years after the completion of the next-to-leading order calculation, the status of the theoret...
AbstractThe anomaly in the vacuum expectation value of the product of axial and two vector currents ...
AbstractThe pion scalar radius is given by 〈rS2〉=(6/π)∫4Mπ2∞dsδS(s)/s2, with δS the phase of the sca...
We propose to use rich informations on pi p total cross sections below N=10 GeV in order to investig...
We show that the nonperturbative solution of the SU(2) linear sigma model field theory requires colo...
AbstractThe quark–gluon mixed condensate g〈q̄σμνFμνq〉 is calculated in the Gaussian approximation of...
We use general relations between the Transition Distribution Amplitudes (TDAs), entering the descrip...
The η′ meson is associated with the U(1) anomaly. In this paper, a successful effective chiral theor...
A search is performed for the as yet unobserved baryonic Λ0 b → Λη 0 and Λ 0 b → Λη decays with...
Motivated by the LHCb measurement, we analyze the Bs→π+π−ℓ+ℓ− decay in the kinematics region where t...
We show how the isospin vector and axialvector current spectral functions V,3 and A,3 can be used to...