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Related papers: Feynman Diagrams and Lax Pair Equations

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In a previous work, hep-th/0501245, we introduced characters and classes built out of the M-theory four-form and the Pontrjagin classes, which we used to express the Chern-Simons and the one-loop terms in a way that makes the topological…

High Energy Physics - Theory · Physics 2010-04-05 Hisham Sati

The asymptotic nature of perturbative expansions in quantum field theory can arise from the factorial growth in the number of Feynman diagrams with loop order, as with instantons, or from a series of individual diagrams whose values grow…

High Energy Physics - Theory · Physics 2025-12-11 Luen Clingerman , Matthew D. Schwartz

The method of Feynman-Kac perturbation of quantum stochastic processes has a long pedigree, with the theory usually developed within the framework of processes on von Neumann algebras. In this work, the theory of operator spaces is…

Operator Algebras · Mathematics 2024-07-10 Alexander C. R. Belton , Stephen J. Wills

We develop fully noncommutative Feynman-Kac formulae by employing quantum stochastic processes. To this end we establish some theory for perturbing quantum stochastic flows on von Neumann algebras by multiplier cocycles. Multiplier cocycles…

Functional Analysis · Mathematics 2018-01-18 Alexander C. R. Belton , J. Martin Lindsay , Adam G. Skalski

Under the Neumann constraints, each equation of the KdV hierarchy is decomposed into two finite dimensional systems, including the well-known Neumann model. Like in the case of the Bargmann constraint, the explicit Lax representations are…

Exactly Solvable and Integrable Systems · Physics 2015-06-26 Ruguang Zhou

This paper provides a primer in quantum field theory (QFT) based on Hopf algebra and describes new Hopf algebraic constructions inspired by QFT concepts. The following QFT concepts are introduced: chronological products, S-matrix, Feynman…

High Energy Physics - Theory · Physics 2014-11-18 Christian Brouder

We relate the author's Lie cobracket in the module additively generated by loops on a surface with the Connes-Kreimer Lie bracket in the module additively generated by trees. To this end we introduce a pre-Lie coalgebra and a (commutative)…

High Energy Physics - Theory · Physics 2009-11-10 Vladimir Turaev

In this work we discuss the connection between Feynman integrals and Fox functions. Illustrative examples are given.

High Energy Physics - Phenomenology · Physics 2024-05-30 Giampiero Passarino

We construct natural representations of the Connes-Kreimer Lie algebras on rooted trees/Feynman graphs arising from Hecke correspondences in the categories $\LRF, \LFG$ constructed by K. Kremnizer and the author. We thus obtain the…

Quantum Algebra · Mathematics 2009-09-08 Matthew Szczesny

We prove a neat factorization property of Feynman graphs in covariant perturbation theory. The contribution of the graph to the effective action is written as a product of a massless scalar momentum integral that only depends on the basic…

High Energy Physics - Phenomenology · Physics 2023-09-27 Gero von Gersdorff

Problems occurring in physically important non-trivial examples of loop calculations are discussed. A procedure of deriving expansions of two-loop self-energy diagrams with different masses is constructed. The cases of small and large…

High Energy Physics - Phenomenology · Physics 2007-05-23 A. I. Davydychev

A new powerful method to calculate Feynman diagrams is proposed. It consists in setting up a Taylor series expansion in the external momenta squared (in general multivariable). The Taylor coefficients are obtained from the original diagram…

High Energy Physics - Phenomenology · Physics 2011-08-17 J. Fleischer , O. V. Tarasov

The integrand of any multi-loop integral is characterised after Feynman parametrisation by two polynomials. In this review we summarise the properties of these polynomials. Topics covered in this article include among others: Spanning trees…

High Energy Physics - Phenomenology · Physics 2015-05-18 Christian Bogner , Stefan Weinzierl

The finite Pfaff lattice is given by commuting Lax pairs involving a finite matrix L (zero above the first subdiagonal) and a projection onto Sp(N). The lattice admits solutions such that the entries of the matrix L are rational in the time…

Exactly Solvable and Integrable Systems · Physics 2007-05-23 Mark Adler , Vadim B. Kuznetsov , Pierre van Moerbeke

We use mixed Hodge structures to investigate Feynman amplitudes as functions of external momenta and masses.

High Energy Physics - Theory · Physics 2010-07-27 Spencer Bloch , Dirk Kreimer

Using a fermionic version of the Lax pair formulation, we construct an integrable small-polaron model with general open boundary conditions. The Lax pair and the boundary supermatrices $K_{\pm}$ for the model are obtained. This provides a…

Strongly Correlated Electrons · Physics 2017-09-27 Xi-Wen Guan , Uwe Grimm , Rudolf A. Roemer

We give a general procedure to construct algebro-geometric Feynman rules, that is, characters of the Connes-Kreimer Hopf algebra of Feynman graphs that factor through a Grothendieck ring of immersed conical varieties, via the class of the…

High Energy Physics - Theory · Physics 2011-03-22 Paolo Aluffi , Matilde Marcolli

We present the explicit formulae relating Hopf maps with Wigner's little groups. They, particularly, explain simple action of group on a fiber for the first and second Hopf fibrations, and present most simplified form for the third one.…

High Energy Physics - Theory · Physics 2011-07-18 Ruben Mkrtchyan , Armen Nersessian , Vahagn Yeghikyan

We show explicitly how to construct the quantum Lax pair for systems with open boundary conditions. We demonstrate the method by applying it to the Heisenberg XXZ model with general integrable boundary terms.

solv-int · Physics 2010-11-16 A. Lima-Santos

The general lines of the derivation and the main properties of the master equations for the master amplitudes associated to a given Feynman graph are recalled. Some results for the 2-loop self-mass graph with 4 propagators are then…

High Energy Physics - Theory · Physics 2007-05-23 M. Caffo , H. Czyz , S. Laporta , E. Remiddi