Three-loop anomalous dimension of the non-singlet transversity operator in QCD
From MaRDI portal
Publication:1949616
DOI10.1016/j.nuclphysb.2012.06.010zbMath1262.81211arXiv1203.1022OpenAlexW2027620405MaRDI QIDQ1949616
Publication date: 8 May 2013
Published in: Nuclear Physics. B (Search for Journal in Brave)
Full work available at URL: https://arxiv.org/abs/1203.1022
Related Items (12)
Anomalous dimensions of gauge fields and gauge coupling beta-functions in the standard model at three loops ⋮ Off-forward anomalous dimensions of non-singlet transversity operators ⋮ Six-loop anomalous dimension of twist-two operators in planar \( \mathcal{N}=4 \) SYM theory ⋮ Three loop massive operator matrix elements and asymptotic Wilson coefficients with two different masses ⋮ The three-loop splitting functions \(P_{q g}^{(2)}\) and \(P_{g g}^{(2, \operatorname{N}_{\operatorname{F}})}\) ⋮ The 3-loop non-singlet heavy flavor contributions and anomalous dimensions for the structure function \(\mathrm{F}_2(\mathrm{x, Q}^{\mathrm{2}})\) and transversity ⋮ The three-loop splitting functions in QCD: the helicity-dependent case ⋮ Four-loop non-singlet splitting functions in the planar limit and beyond ⋮ Non-planar universal anomalous dimension of twist-two operators with general Lorentz spin at four loops in \(\mathcal{N} = 4\) SYM theory ⋮ The three-loop unpolarized and polarized non-singlet anomalous dimensions from off shell operator matrix elements ⋮ Large-\(n_{f}\) contributions to the four-loop splitting functions in QCD ⋮ Non-planar anomalous dimension of twist-2 operators: higher moments at four loops
Uses Software
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