We derive new convergent series representations for the two-loop sunset diagram with three different propagator masses $$m_1,\, m_2$$ and $$m_3$$ and external momentum p by techniques of analytic continuation on a well-known triple series that corresponds to the Lauricella $$F_C^{(3)}$$ function. The convergence regions of the new series contain regions of interest to physical problems. These include some ranges of masses and squared external momentum values which make them useful from Chiral Perturbation Theory to some regions of the parameter space of the Minimal Supersymmetric Standard Model. The analytic continuation results presented for the Lauricella series could be used in other settings as well
For certain dimensionally-regulated one-, two- and three-loop diagrams, problems of constructing the...
Fleischer J, Kotikov AV, Veretin OL. Analytic two-loop results for self-energy- and vertex-type diag...
We integrate three-loop sunrise-type vacuum diagrams in D0=4 dimensions with four different masses u...
International audienceWe derive new convergent series representations for the two-loop sunset diagra...
We present an analytic representation of FK/Fπ as calculated in three-flavor two-loop chiral perturb...
International audienceWe present an analytic representation of FK/Fπ as calculated in three-flavor t...
We present an analytic representation of F-K / F(pi )as calculated in three-flavor two-loop chiral p...
We demonstrate the use of several code implementations of the Mellin-Barnes method available in the ...
We demonstrate the use of several code implementations of the Mellin-Barnes method available in the ...
In this paper, we consider the two-loop sunset diagram with two different masses, m and M , at space...
International audienceIn this work, we consider expressions for the masses and decay constants of th...
In this work, we consider expressions for the masses and decay constants of the pseudoscalar mesons ...
From the computation of three-point singlet correlators in the two-matrix model, we obtain an explic...
We show how to compute the two-loop sunset integrals at finite volume, for non-degenerate masses and...
For certain dimensionally-regulated one-, two- and three-loop diagrams, problems of constructing the...
For certain dimensionally-regulated one-, two- and three-loop diagrams, problems of constructing the...
Fleischer J, Kotikov AV, Veretin OL. Analytic two-loop results for self-energy- and vertex-type diag...
We integrate three-loop sunrise-type vacuum diagrams in D0=4 dimensions with four different masses u...
International audienceWe derive new convergent series representations for the two-loop sunset diagra...
We present an analytic representation of FK/Fπ as calculated in three-flavor two-loop chiral perturb...
International audienceWe present an analytic representation of FK/Fπ as calculated in three-flavor t...
We present an analytic representation of F-K / F(pi )as calculated in three-flavor two-loop chiral p...
We demonstrate the use of several code implementations of the Mellin-Barnes method available in the ...
We demonstrate the use of several code implementations of the Mellin-Barnes method available in the ...
In this paper, we consider the two-loop sunset diagram with two different masses, m and M , at space...
International audienceIn this work, we consider expressions for the masses and decay constants of th...
In this work, we consider expressions for the masses and decay constants of the pseudoscalar mesons ...
From the computation of three-point singlet correlators in the two-matrix model, we obtain an explic...
We show how to compute the two-loop sunset integrals at finite volume, for non-degenerate masses and...
For certain dimensionally-regulated one-, two- and three-loop diagrams, problems of constructing the...
For certain dimensionally-regulated one-, two- and three-loop diagrams, problems of constructing the...
Fleischer J, Kotikov AV, Veretin OL. Analytic two-loop results for self-energy- and vertex-type diag...
We integrate three-loop sunrise-type vacuum diagrams in D0=4 dimensions with four different masses u...