We calculate the polarized massive operator matrix element $A_{gq}^{(3)}(N)$ to 3-loop order in Quantum Chromodynamics analytically at general values of the Mellin variable $N$ both in the single- and double-mass case in the Larin scheme. It is a transition function required in the variable flavor number scheme at $O(\alpha_s^3)$. We also present the results in momentum fraction space
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inela...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
We calculate the gluonic massive operator matrix elements in the unpolarized and polarized cases, $A...
We calculate the massive polarized three-loop pure singlet operator matrix element $A_{Qq}^{(3), \rm...
We calculate the gluonic massive operator matrix elements in the unpolarized and polarized cases, A$...
We compute the two-mass contributions to the polarized massive operator matrix element $A_{gg,Q}^{(3...
We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inela...
We present the two-mass QCD contributions to the polarized pure singlet operator matrix element at t...
We calculate the two-mass QCD contributions to the massive operator matrix element $A_{gg,Q}$ at $\m...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
The $O(\alpha_s^3 T_F^2 C_F (C_A))$ contributions to the transition matrix element $A_{gg,Q}$ releva...
Contributions to heavy flavour transition matrix elements in the variable flavour number scheme are ...
Starting at 3-loop order, the massive Wilson coefficients for deep-inelastic scattering and the mass...
We calculate the two-mass QCD contributions to the massive operator matrix element Agg,Q at O(αs3) i...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inela...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
We calculate the gluonic massive operator matrix elements in the unpolarized and polarized cases, $A...
We calculate the massive polarized three-loop pure singlet operator matrix element $A_{Qq}^{(3), \rm...
We calculate the gluonic massive operator matrix elements in the unpolarized and polarized cases, A$...
We compute the two-mass contributions to the polarized massive operator matrix element $A_{gg,Q}^{(3...
We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inela...
We present the two-mass QCD contributions to the polarized pure singlet operator matrix element at t...
We calculate the two-mass QCD contributions to the massive operator matrix element $A_{gg,Q}$ at $\m...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
The $O(\alpha_s^3 T_F^2 C_F (C_A))$ contributions to the transition matrix element $A_{gg,Q}$ releva...
Contributions to heavy flavour transition matrix elements in the variable flavour number scheme are ...
Starting at 3-loop order, the massive Wilson coefficients for deep-inelastic scattering and the mass...
We calculate the two-mass QCD contributions to the massive operator matrix element Agg,Q at O(αs3) i...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...
We compute the logarithmic contributions to the polarized massive Wilson coefficients for deep-inela...
We calculate the massive flavor non-singlet Wilson coefficient for the heavy flavor contributions to...