2013
DOI: 10.4310/cntp.2013.v7.n2.a2
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A chord diagram expansion coming from some Dyson-Schwinger equations

Abstract: We give an expression for the solution to propagator-type DysonSchwinger equations with one primitive at 1 loop as an expansion over rooted connected chord diagrams. Along the way we give a refinement of a classical recurrence of rooted connected chord diagrams, and a representation in terms of binary trees.

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Cited by 24 publications
(82 citation statements)
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“…Different theories with isomorphic diagrammatics only show their difference in their dependence on the coefficients of the expansions of the regularized Feynman integrals of the primitive 1 Feynman graphs of the theory contributing to the Dyson-Schwinger equation. These coefficients are the f i of [11] and our previous work [3] and are the a k,i of [7], a notation which we will also use in the present paper. The way these coefficients come in is well-controlled; for example in all cases the full H k depends only on coefficients coming from the first k terms of expansions of primitive graphs with at most k + 1 loops (this is clear and long-known in physics and is also an immediate corollary of the main results of [11] and [7]).…”
Section: Introductionmentioning
confidence: 99%
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“…Different theories with isomorphic diagrammatics only show their difference in their dependence on the coefficients of the expansions of the regularized Feynman integrals of the primitive 1 Feynman graphs of the theory contributing to the Dyson-Schwinger equation. These coefficients are the f i of [11] and our previous work [3] and are the a k,i of [7], a notation which we will also use in the present paper. The way these coefficients come in is well-controlled; for example in all cases the full H k depends only on coefficients coming from the first k terms of expansions of primitive graphs with at most k + 1 loops (this is clear and long-known in physics and is also an immediate corollary of the main results of [11] and [7]).…”
Section: Introductionmentioning
confidence: 99%
“…These coefficients are the f i of [11] and our previous work [3] and are the a k,i of [7], a notation which we will also use in the present paper. The way these coefficients come in is well-controlled; for example in all cases the full H k depends only on coefficients coming from the first k terms of expansions of primitive graphs with at most k + 1 loops (this is clear and long-known in physics and is also an immediate corollary of the main results of [11] and [7]). Furthermore, we can prove for all sufficiently large k which terms will dominate H k .…”
Section: Introductionmentioning
confidence: 99%
See 3 more Smart Citations