U(1) gauge theory on non-commutative Minkowski space-time in the Feynman-'t Hooft background gauge is studied. In particular, UV divergences and non-commutative IR divergent contributions to the two, three and four-point functions are explicitly computed at one loop. We show that the negative sign of the beta function results from paramagnetism --producing UV charge anti-screening-- prevailing over diamagnetism --giving rise toUV charge screening. This dominance in the field theory setting corresponds to tachyon magnification dominance in the string theory framework. Our calculations provide an explicit realization of UV/IR mixing and lead to an IR renormalization of the coupling constant, where now paramagnetic contributions produce screen...
Here we discuss the ultraviolet and infrared aspects of the noncommutative counterpart of QED, which...
It is argued that the quadratic and linear non-commutative IR divergences that occur in U(1) theory ...
AbstractWe prove that the β-function of the Grosse–Wulkenhaar model including a magnetic field vanis...
U(1) gauge theory on non-commutative Minkowski spacetime in the Feynman-'t Hooft background gauge is...
Using Dimensional Regularization (DR) for some two-point functions of a prototype Non-Comutative (NC...
AbstractUsing Dimensional Regularization (DR) for some two-point functions of a prototype Non-Commut...
In these lectures we give a concise introduction to the ideas of renormalon calculus in QED and QCD....
We review the extrapolation of the single-particle string spectrum on AdS(5)xS(5) to the Higher Spin...
We rediscuss the recent controversy on a possible Chern-Simons like term generated through radiative...
We construct contact interactions for bosonic and spinning strings. In the tensionless limit of the ...
The three-dimensional noncommutative supersymmetric QED is investigated within the superfield approa...
If QCD is renormalized by minimal subtraction (MS), at higher orders, the strong coupling constant a...
We present in analytic form the matching conditions for the strong-coupling constant alpha_s^(n_f)(m...
It has recently been shown that the observation by the PVLAS collaboration of an anomalously large r...
We compute the dependence on the classical action "gauge" parameters of the beta functions of the st...
Here we discuss the ultraviolet and infrared aspects of the noncommutative counterpart of QED, which...
It is argued that the quadratic and linear non-commutative IR divergences that occur in U(1) theory ...
AbstractWe prove that the β-function of the Grosse–Wulkenhaar model including a magnetic field vanis...
U(1) gauge theory on non-commutative Minkowski spacetime in the Feynman-'t Hooft background gauge is...
Using Dimensional Regularization (DR) for some two-point functions of a prototype Non-Comutative (NC...
AbstractUsing Dimensional Regularization (DR) for some two-point functions of a prototype Non-Commut...
In these lectures we give a concise introduction to the ideas of renormalon calculus in QED and QCD....
We review the extrapolation of the single-particle string spectrum on AdS(5)xS(5) to the Higher Spin...
We rediscuss the recent controversy on a possible Chern-Simons like term generated through radiative...
We construct contact interactions for bosonic and spinning strings. In the tensionless limit of the ...
The three-dimensional noncommutative supersymmetric QED is investigated within the superfield approa...
If QCD is renormalized by minimal subtraction (MS), at higher orders, the strong coupling constant a...
We present in analytic form the matching conditions for the strong-coupling constant alpha_s^(n_f)(m...
It has recently been shown that the observation by the PVLAS collaboration of an anomalously large r...
We compute the dependence on the classical action "gauge" parameters of the beta functions of the st...
Here we discuss the ultraviolet and infrared aspects of the noncommutative counterpart of QED, which...
It is argued that the quadratic and linear non-commutative IR divergences that occur in U(1) theory ...
AbstractWe prove that the β-function of the Grosse–Wulkenhaar model including a magnetic field vanis...