We present preliminary results of the non-perturbative renormalization group (RG) running of the flavor non-singlet tensor operator. We employ the $chi$SF scheme for $N_f=3$ QCD using ensembles generated by the ALPHA collaboration for the computation of the quark mass running. The $chi$SF property of automatic $O(a)$ improvement prevents the $O(a)$ mixing of the correlation functions
Tensor currents are the only quark bilinear operators lacking a non-perturbative determination of th...
We determine from first principles the quark mass anomalous dimension in Nf=3 QCD between the ele...
Abstract Tensor currents are the only quark bilinear operators lacking a non-perturbative determinat...
We present preliminary results of the non-perturbative renormalization group (RG) running of the fl...
We present preliminary results of the non-perturbative renormalization group (RG) running of the fla...
We present our progress in the non-perturbative O(a) improvement and renormalization of tensor curre...
We present our progress in the non-perturbative O(a) improvement and renormalization of tensor curre...
ALPHA CollaborationWe study the renormalization group (RG) running of the quark mass, for Nf=3 QCD w...
We present our preliminary results for the computation of the non-perturbative running of renormaliz...
We compute the nonperturbative quark mass RG-running in the range ΛQCD⪅μ⪅MW for Nf=3 massless QCD wi...
We determine from first principles the quark mass anomalous dimension in $N_{\scriptstyle \mathrm{f}...
We compute the nonperturbative quark mass RG-running in the range $Lambda_{QCD}lessapproxmulessappr...
Tensor currents are the only quark bilinear operators lacking a non-perturbative determination of th...
Abstract We determine from first principles the quark mass anomalous dimension in $$N_{\scriptstyle ...
We determine from first principles the quark mass anomalous dimension in $$N_{\scriptstyle \mathrm{f...
Tensor currents are the only quark bilinear operators lacking a non-perturbative determination of th...
We determine from first principles the quark mass anomalous dimension in Nf=3 QCD between the ele...
Abstract Tensor currents are the only quark bilinear operators lacking a non-perturbative determinat...
We present preliminary results of the non-perturbative renormalization group (RG) running of the fl...
We present preliminary results of the non-perturbative renormalization group (RG) running of the fla...
We present our progress in the non-perturbative O(a) improvement and renormalization of tensor curre...
We present our progress in the non-perturbative O(a) improvement and renormalization of tensor curre...
ALPHA CollaborationWe study the renormalization group (RG) running of the quark mass, for Nf=3 QCD w...
We present our preliminary results for the computation of the non-perturbative running of renormaliz...
We compute the nonperturbative quark mass RG-running in the range ΛQCD⪅μ⪅MW for Nf=3 massless QCD wi...
We determine from first principles the quark mass anomalous dimension in $N_{\scriptstyle \mathrm{f}...
We compute the nonperturbative quark mass RG-running in the range $Lambda_{QCD}lessapproxmulessappr...
Tensor currents are the only quark bilinear operators lacking a non-perturbative determination of th...
Abstract We determine from first principles the quark mass anomalous dimension in $$N_{\scriptstyle ...
We determine from first principles the quark mass anomalous dimension in $$N_{\scriptstyle \mathrm{f...
Tensor currents are the only quark bilinear operators lacking a non-perturbative determination of th...
We determine from first principles the quark mass anomalous dimension in Nf=3 QCD between the ele...
Abstract Tensor currents are the only quark bilinear operators lacking a non-perturbative determinat...