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Very high energy physics needs a coherent description of the four fundamental forces. Non-commutative geometry is a promising mathematical framework which already allowed to unify the general relativity and the standard model, at the…

Mathematical Physics · Physics 2009-12-07 Fabien Vignes-Tourneret

We show that the real massive Klein-Gordon theory admits a description in terms of states on various timelike hypersurfaces and amplitudes associated to regions bounded by them. This realizes crucial elements of the general boundary…

High Energy Physics - Theory · Physics 2008-11-26 Robert Oeckl

In this paper, we derive the Carrollian amplitude in the framework of bulk reduction. The Carrollian amplitude is shown to relate to the scattering amplitude by a Fourier transform in this method. We propose Feynman rules to calculate the…

High Energy Physics - Theory · Physics 2024-07-31 Wen-Bin Liu , Jiang Long , Xiao-Quan Ye

Noncommutative (NC) quantum field theory is the subject of many analyses on formal and general aspects looking for deviations and, therefore, potential noncommutative spacetime effects. Within of this large class, we may now pay some…

High Energy Physics - Theory · Physics 2014-04-04 R. Bufalo , T. R. Cardoso , B. M. Pimentel

Definition of Feynman integrals as solutions of some well defined systems of differential equations is proposed. This definition is equivalent to usual one but needs no regularization and application of $R$-operation. It is argued that…

High Energy Physics - Theory · Physics 2007-05-23 F. A. Lunev

In this article we consider theta-expanded noncommutative gauge field theory, constructed at the first order in noncommutative parameter theta, as an effective, anomaly free theory, with one-loop renormalizable gauge sector. Related…

High Energy Physics - Phenomenology · Physics 2008-11-26 Josip Trampetic

Renormalization procedure is generalized to be applicable for non renormalizable theories. It is shown that introduction of an extra expansion parameter allows to get rid of divergences and express physical quantities as series of finite…

High Energy Physics - Theory · Physics 2008-02-03 J. Gegelia , G. Japaridze , N. Kiknadze , K. Turashvili

We demonstrate the renormalisability of quantum field theories in four dimensions with elementary self-interacting Dirac fermions and to leading order in the limit of many fermion flavours $N_{\rm f}$. Starting from the underlying…

High Energy Physics - Theory · Physics 2026-03-25 Charlie Cresswell-Hogg , Daniel F. Litim

We investigate the relationship between the universal topological polynomials for graphs in mathematics and the parametric representation of Feynman amplitudes in quantum field theory. In this first paper we consider translation invariant…

Mathematical Physics · Physics 2011-01-03 T. Krajewski , V. Rivasseau , A. Tanasa , Zhituo Wang

We study differential equations for Feynman amplitudes and we show that the corresponding D-module is isomorphic to a GKZ D-modules. We show that the sheaf of solutions to the D-module is isomorphic to a certain relative homology and the…

Mathematical Physics · Physics 2016-06-24 Emad Nasrollahpoursamami

Following Feynman's successful treatment of the polaron problem we apply the same variational principle to quenched QED in the worldline formulation. New features arise from the description of fermions by Grassmann trajectories, the…

High Energy Physics - Theory · Physics 2009-10-31 C. Alexandrou , R. Rosenfelder , A. W. Schreiber

We develop a general framework for quantum field theory on noncommutative spaces, i.e., spaces with quantum group symmetry. We use the path integral approach to obtain expressions for $n$-point functions. Perturbation theory leads us to…

High Energy Physics - Theory · Physics 2009-10-31 Robert Oeckl

A statistical ensemble of neural networks can be described in terms of a quantum field theory (NN-QFT correspondence). The infinite-width limit is mapped to a free field theory, while finite N corrections are mapped to interactions. After…

High Energy Physics - Theory · Physics 2022-12-23 Harold Erbin , Vincent Lahoche , Dine Ousmane Samary

Computations in renormalizable perturbative quantum field theories reveal mathematical structures which go way beyond the formal structure which is usually taken as underlying quantum field theory. We review these new structures and the…

High Energy Physics - Theory · Physics 2009-11-07 Dirk Kreimer

We show that renormalized non-commutative scalar field theories do not reduce to their planar sector in the limit of large non-commutativity. This follows from the fact that the RG equation of the Wilson-Polchinski type which describes the…

High Energy Physics - Theory · Physics 2009-11-10 C. Becchi , S. Giusto , C. Imbimbo

We show how, modulo the distinction between the antipode and the "twisted" or "renormalized" antipode, Connes and Kreimer's algebraic paradigm trivializes the proofs of equivalence of the (corrected) Dyson-Salam, Bogoliubov-Parasiuk-Hepp…

High Energy Physics - Theory · Physics 2009-11-10 Hector Figueroa , Jose M. Gracia-Bondia

We propose a new formalism for quantum field theory which is neither based on functional integrals, nor on Feynman graphs, but on marked trees. This formalism is constructive, i.e. it computes correlation functions through convergent rather…

High Energy Physics - Theory · Physics 2015-05-13 R. Gurau , J. Magnen , V. Rivasseau

We consider the noncommutative extension of the BF theory in two spacetime dimensions. We show that the introduction of the noncommutative parameter \theta_{\mu\nu}, already at first order in the analytical sector, induces infinitely many…

High Energy Physics - Theory · Physics 2008-11-26 Alberto Blasi , Nicola Maggiore , Michele Montobbio

This paper gives a review of Connes-Kreimer formulation of perturbative renormalization in Quantum Field Theory. We begin with the derivation of the Feynman calculus, the Hopf algebra structure on Feynman diagrams and we show the natural…

Mathematical Physics · Physics 2007-05-23 Herintsitohaina Ratsimbarison

The paper presents the representation of quantum field theory without introduction of infinity bare masses and coupling constants of fermions. Counter-terms, compensating for divergent quantities in self-energy diagrams of fermions and…

General Physics · Physics 2015-02-03 V. P. Neznamov
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