1980
DOI: 10.1016/0550-3213(80)90103-0
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Renormalizability of phase factors in non-abelian gauge theory

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Cited by 330 publications
(464 citation statements)
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“…The exponent E equals a sum over web diagrams, d, each given by a group factor multiplied by a diagrammatic integral, In momentum space we can write the exponent E as the integral over a single, overall loop momentum that runs through the web and the cusp vertex, assuming that all loop integrals internal to the web have already been carried out. The web is defined to include the necessary counterterms of the gauge theory [8,30,33,34]. Taking into account the boost invariance of the cusp for massless loop velocities, and the invariance of the ordered exponentials under rescalings of the velocities β i , we have for the exponent the form,…”
Section: Exponentiation and Momentum Space Websmentioning
confidence: 99%
“…The exponent E equals a sum over web diagrams, d, each given by a group factor multiplied by a diagrammatic integral, In momentum space we can write the exponent E as the integral over a single, overall loop momentum that runs through the web and the cusp vertex, assuming that all loop integrals internal to the web have already been carried out. The web is defined to include the necessary counterterms of the gauge theory [8,30,33,34]. Taking into account the boost invariance of the cusp for massless loop velocities, and the invariance of the ordered exponentials under rescalings of the velocities β i , we have for the exponent the form,…”
Section: Exponentiation and Momentum Space Websmentioning
confidence: 99%
“…In particular, all colour factors appearing in the exponent correspond to connected graphs [93]. There are two complementary approaches to exponentiation: one is based on evolution equations [2-15, 18, 19, 21-40], which are ultimately a consequence of multiplicative renormalizability [94][95][96][97], and the second is a diagrammatic approach, the direct computation of the exponent in terms of webs [93,[98][99][100][101][102][103][104]. Following ref.…”
Section: Jhep04(2014)044mentioning
confidence: 99%
“…The first constant term may be included in the self energies of the heavy quarks [41,42]. An unlimited extension of a linear potential to large distances would lead to too strong a van der Waals force between hadrons [43] so that the potential should cease to be linear and fall off at large distances as remarked in the beginning of this subsection.…”
Section: T He CCC and The Linear Potentialmentioning
confidence: 99%