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We study the quantization of the noncommutative selfdual \phi^3 model in 4 dimensions, by mapping it to a Kontsevich model. The model is shown to be renormalizable, provided one additional counterterm is included compared to the…

High Energy Physics - Theory · Physics 2009-11-11 H. Grosse , H. Steinacker

Field theories on deformed spaces suffer from the IR/UV mixing and renormalization is generically spoiled. In work with R. Wulkenhaar, one of us realized a way to cure this disease by adding one more marginal operator. We review these…

High Energy Physics - Theory · Physics 2008-11-26 Harald Grosse , Michael Wohlgenannt

We consider a scalar $\phi^4$ theory on canonically deformed Euclidean space in 4 dimensions with an additional oscillator potential. This model is known to be renormalisable. An exterior gauge field is coupled in a gauge invariant manner…

High Energy Physics - Theory · Physics 2008-11-26 Harald Grosse , Michael Wohlgenannt

We define four 3x3 commuting contractions which do not dilate to commuting isometries. However they do satisfy the scalar von Neumann inequality. These matrices are all nilpotent of order 2. We also show that any three $3\times3$ commuting…

Operator Algebras · Mathematics 2014-02-26 Man Duen Choi , Kenneth R. Davidson

The simplest non commutative renormalizable field theory, the $\phi_4^4$ model on four dimensional Moyal space with harmonic potential is asymptotically safe at one loop, as shown by H. Grosse and R. Wulkenhaar. We extend this result up to…

High Energy Physics - Theory · Physics 2008-11-26 Margherita Disertori , Vincent Rivasseau

We identify new families of renormalizable of tensor models from anterior renormalizable tensor models via a mapping capable of reducing or increasing the rank of the theory without having an effect on the renormalizability property.…

High Energy Physics - Theory · Physics 2013-11-08 Joseph Ben Geloun , Etera R. Livine

In this paper we elaborate on the translation-invariant renormalizable Phi^4 theory in 4-dimensional non-commutative space which was recently introduced by the Orsay group. By explicitly performing Feynman graph calculations at one loop and…

High Energy Physics - Theory · Physics 2011-07-19 Daniel N. Blaschke , Francois Gieres , Erwin Kronberger , Thomas Reis , Manfred Schweda , Rene I. P. Sedmik

Explicit two-loop calculations in noncommutative $\phi^4_4$ theory are presented. It is shown that the model is two-loop renormalizable.

High Energy Physics - Theory · Physics 2008-11-26 I. Ya. Aref'eva , D. M. Belov , A. S. Koshelev

Irreversibility theorems -- such as the $A$-theorem -- establish a hierarchy among fixed points of the renormalization group flow. The strongest thesis of this type of theorems would be that there exists a scalar function $A$ (generally…

High Energy Physics - Theory · Physics 2026-05-27 Lorenzo Benfatto , Omar Zanusso

We briefly review the r\^ole played by algebraic structures like combinatorial Hopf algebras in the renormalizability of (noncommutative) quantum field theory. After sketching the commutative case, we analyze the noncommutative…

Combinatorics · Mathematics 2011-03-28 Adrian Tanasa

Traditionally, covariant scalar field theory models are either super renormalizable, strictly renormalizable, or nonrenormalizable. The goal of `Mixed Models' is to make sense of sums of these distinct examples, e.g.,…

High Energy Physics - Theory · Physics 2017-02-01 John R. Klauder

We show that if $X$ is an indecomposable $PD_3$-complex and $\pi_1(X) is the fundamental group of a reduced finite graph of finite groups but is not virtually cyclic then $X$ is orientable, the underlying graph is a tree, all the edge…

Geometric Topology · Mathematics 2014-07-22 J. A. Hillman

A noncommutative Feynman graph is a ribbon graph and can be drawn on a genus $g$ 2-surface with a boundary. We formulate a general convergence theorem for the noncommutative Feynman graphs in topological terms and prove it for some classes…

High Energy Physics - Theory · Physics 2009-10-31 Iouri Chepelev , Radu Roiban

We consider the O(N)-symmetric phi4 theory in two and three dimensions and determine the nonperturbative mass renormalization needed to obtain the phi4 continuum theory. The required nonperturbative information is obtained by resumming…

High Energy Physics - Theory · Physics 2015-12-22 Andrea Pelissetto , Ettore Vicari

Non(anti)commutative gauge theories are supersymmetric Yang-Mills and matter system defined on a deformed superspace whose coordinates obey non(anti)commutative algebra. We prove that these theories in four dimensions with N=1/2…

High Energy Physics - Theory · Physics 2009-11-10 Oleg Lunin , Soo-Jong Rey

We construct multiplicative renormalization for the Epstein--Glaser renormalization scheme in perturbative Algebraic Quantum Field Theory: To this end, we fully combine the Connes--Kreimer renormalization framework with the Epstein--Glaser…

Mathematical Physics · Physics 2025-12-11 Jonah Epstein , Arne Hofmann , David Prinz

We review here the construction of a translation-invariant scalar model which was proved to be perturbatively renormalizable on Moyal space. Some general considerations on nonlocal renormalizability are given. Finally, we present…

High Energy Physics - Theory · Physics 2010-06-09 Adrian Tanasa

The simplest non commutative renormalizable field theory, the $\phi_4$ model on four dimensional Moyal space with harmonic potential is asymptotically safe up to three loops, as shown by H. Grosse and R. Wulkenhaar, M. Disertori and V.…

High Energy Physics - Theory · Physics 2008-11-26 M. Disertori , R. Gurau , J. Magnen , V. Rivasseau

We prove the first nontrivial reconstruction theorem for modular tensor categories: the category associated to any twisted Drinfeld double of any finite group, can be realised as the representation category of a completely rational…

Quantum Algebra · Mathematics 2018-05-01 David E. Evans , Terry Gannon

We develop a new formalism to study nonlinear evolution in the growth of large-scale structure, by following the dynamics of gravitational clustering as it builds up in time. This approach is conveniently represented by Feynman diagrams…

Astrophysics · Physics 2009-11-13 M. Crocce , R. Scoccimarro