scholarly journals Five-loop fermion anomalous dimension for a general gauge group from four-loop massless propagators

2017 ◽  
Vol 2017 (4) ◽  
Author(s):  
P.A. Baikov ◽  
K.G. Chetyrkin ◽  
J.H. Kühn
2017 ◽  
Vol 48 (12) ◽  
pp. 2331
Author(s):  
T. Luthe ◽  
A. Maier ◽  
P. Marquard ◽  
Y. Schröder

2017 ◽  
Vol 2017 (1) ◽  
Author(s):  
Thomas Luthe ◽  
Andreas Maier ◽  
Peter Marquard ◽  
York Schröder

1989 ◽  
Vol 04 (13) ◽  
pp. 1257-1276 ◽  
Author(s):  
G.P. KORCHEMSKY

The asymptotics of the evolution kernels Pab(z) of parton distributions is investigated as z→1. It is proven that to all orders of perturbative QCD, [Formula: see text] where [Formula: see text] is the cusp anomalous dimension of the contour functionals in the fundamental (α=“quark”) and adjoint (α=“gluon”) representations of gauge group and, to the lowest orders, Cα are related to the anomalous dimension of a quark field in the axial gauge and the beta function of QCD by a simple equation.


2021 ◽  
Vol 2021 (12) ◽  
Author(s):  
Luis F. Alday ◽  
Shai M. Chester ◽  
Tobias Hansen

Abstract We study the stress tensor four-point function for $$ \mathcal{N} $$ N = 4 SYM with gauge group G = SU(N), SO(2N + 1), SO(2N) or USp(2N) at large N . When G = SU(N), the theory is dual to type IIB string theory on AdS5× S5 with complexified string coupling τs, while for the other cases it is dual to the orbifold theory on AdS5× S5/ℤ2. In all cases we use the analytic bootstrap and constraints from localization to compute 1-loop and higher derivative tree level corrections to the leading supergravity approximation of the correlator. We give perturbative evidence that the localization constraint in the large N and finite complexified coupling τ limit can be written for each G in terms of Eisenstein series that are modular invariant in terms of τs ∝ τ, which allows us to fix protected terms in the correlator in that limit. In all cases, we find that the flat space limit of the correlator precisely matches the type IIB S-matrix. We also find a closed form expression for the SU(N) 1-loop Mellin amplitude with supergravity vertices. Finally, we compare our analytic predictions at large N and finite τ to bounds from the numerical bootstrap in the large N regime, and find that they are not saturated for any G and any τ , which suggests that no physical theory saturates these bootstrap bounds.


2007 ◽  
Vol 2007 (09) ◽  
pp. 058-058 ◽  
Author(s):  
Ian Jack ◽  
D.R. Timothy Jones ◽  
Philipp Kant ◽  
Luminita Mihaila

2016 ◽  
Vol 2016 (7) ◽  
Author(s):  
Thomas Luthe ◽  
Andreas Maier ◽  
Peter Marquard ◽  
York Schröder

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