2008
DOI: 10.1088/1751-8113/41/31/315401
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On conformal invariant integrals involving spin one-half and spin-one particles

Abstract: We consider the evaluation of D-dimensional conformal invariant integrals which involve spin one-half and spin-one particles. The star-triangle relation for the massless Yukawa theory is derived, and the longitudinal part of the three-point Green function of massless QED is determined to the lowest order in position space. The operator algebraic method of calculating massless Feynman integrals is used for the evaluation.

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Cited by 8 publications
(40 citation statements)
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“…Nevertheless, the three-point function of dressed mean gluons of Refs. [13,14,15] can be fixed by conformal symmetry in analogy to [27,28,29,30,31], however, we cannot find higher-point correlators of the dressed mean fields from this Green's function by using ST identity.…”
Section: Introductionmentioning
confidence: 90%
“…Nevertheless, the three-point function of dressed mean gluons of Refs. [13,14,15] can be fixed by conformal symmetry in analogy to [27,28,29,30,31], however, we cannot find higher-point correlators of the dressed mean fields from this Green's function by using ST identity.…”
Section: Introductionmentioning
confidence: 90%
“…A relation previously derived in Refs. [16] and [17] also involved two spinors and one vector field. But there are two important differences between that relation and the relation (18) above.…”
Section: Star-triangle Relation With Two Spinors and One Vector Fieldmentioning
confidence: 99%
“…(18), which is to be presented now, will be along the same lines as followed in Refs. [16] and [17]. We are thus going to use the operator algebraic method due to Isaev [15] which reduces Feynman integrals to products of position and momentum operatorsq i andp i taken between position eigenstates.…”
Section: Star-triangle Relation With Two Spinors and One Vector Fieldmentioning
confidence: 99%
“…Later, this property was generalized via the MB transform to any threepoint Green's function in the massless theory for arbitrary space-time dimension [9,13]. Due to this invariance with respect to Fourier transformation, UD functions appear in the results of calculations of the Green's functions in position space [14,15,16,17,18,19,20].…”
Section: Introductionmentioning
confidence: 99%