A GENERALIZATION OF SYMANZIK POLYNOMIALS
MASTER THESIS, UNDER THE SUPERVISION OF OMID AMINI MATTHIEU PIQUEREZ
- Abstract. Symanzik polynomials are defined on Feynman graphs. They are used in quan-
tum field theory to compute Feynman amplitudes. But they also appear in mathematics in various domains. For example, in article [3], first Symanzik is obtained in a dual theorem of the well-known Kirchhoff’s matrix tree theorem. This article use the result, see [12] and [11], stating that Symanzik polynomials compute the volume of the tropical Jacobian of a metric
- graph. Another important example is article [1], where Theorem 1.1 studies the variation of
the ratio of two Symanzik polynomials, and this theorem has consequences studied in [2]. In this paper, we generalize Symanzik polynomials to simplicial complexes and study their basic properties and applications. For example, we obtain some geometric invariants which compute interesting data on triangulable surfaces. These invariants do not depend on the chosen triangulation. Actually, the Symanzik polynomials can even be defined for any matrices on a PID, for different ranks and with more parameters. The duality relation with what we call Kirchhoff polynomials, as well as Theorem 1.1 of [1], extend to this more general case. In order to show that theorem, we will make great use of oriented matroids. We give a complete classification
- f the connected component of the exchange graph of a matroid, and use that to prove a
boundedness of variation result for Symanzik rational fractions, extending Theorem 1.1 of [1] to our setting.
- 1. Introduction
Symanzik polynomials appear naturally in quantum fields theory for computing Feynman
- amplitudes. They are defined on Feynman graphs. Let G = (V, E) be a graph with vertex set
V and edge set R. Let p = (pv)v∈V ∈ Rn such that each pv, called the external momentum of v ∈ V , is an element of RD, for some positive integer D. RD is endowed with a Minkowski bilinear form. We suppose that
v∈V pv = 0. Such a pair (G, p) is called a Feynman graph.
In this paper we will only consider the case D = 1, but the results can be extended to the more general setting as in [2]. The first Symanzik polynomial, denoted ψG is defined as (1) ψG(x) :=
- T∈T
- e∈T
xe, where T denoted the set of spanning subtrees of G, where the product is on all edges of G which are not in T, and where x = (xe)e∈E is a collection of variables. The second Symanzik polynomial, denoted φG, is defined as (2) φG(p, x) :=
- F∈SF2
q(F)
- e∈F
xe,
Date: April 23, 2018.
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