1974
DOI: 10.1016/0003-4916(74)90448-5
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On the energy-momentum tensor in gauge field theories

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Cited by 146 publications
(120 citation statements)
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“…The work is a natural extension and an application of remarkable classical studies [8,9,10,11] of the energy momentum tensor and of the corresponding trace anomaly in gauge theories.…”
Section: Introductionmentioning
confidence: 98%
See 1 more Smart Citation
“…The work is a natural extension and an application of remarkable classical studies [8,9,10,11] of the energy momentum tensor and of the corresponding trace anomaly in gauge theories.…”
Section: Introductionmentioning
confidence: 98%
“…If we allow only conformally coupled scalars and operators only up to dimension-4 in the Langrangian [8] [9], the EMT is uniquely defined by gravity and takes the form of a symmetric and (on-shell) conserved expression. In the massless limit, which in our case is equivalent to dealing with an unbroken theory (i.e.…”
Section: Introductionmentioning
confidence: 99%
“…As mentioned above, it is mandatory to choose the value χ = 1/6 for any insertion of the EMT on the correlators of the Standard Model. These are found to be ultraviolet finite only if T µν I is included [16][17][18]. We will be dealing with the T ff vertex, where T denotes the EMT and f ≡ ν f a neutrino of flavour f , and work in the limit of zero mass of the neutrinos.…”
Section: Gravitational Interaction Of Neutrinosmentioning
confidence: 99%
“…Following figure 10, we recall that the VE lens equation is based on the geometrical relation [29,30] P S = P I − SI, (6.17) which gives 18) under the assumption that the point R in figure 10 lies on the vertical plane of the lens. θ I is the angle at which the image is viewed by the observer and β is the unlensed angular position of the source.…”
Section: Nonlinear Effects In Strong Deflectionsmentioning
confidence: 99%
“…8 The additive renormalization of U can be understood as follows. Writing the unimproved SUSY current as j = (j + ∆j) − ∆j ≡ j improved − ∆j, with ∆j given by (7) and c = −2/3 therein, it is the superconformal current [27] j improved which is protected from renormalization [39], but the multiplet of improvement terms associated to ∆j is not (compare with the renormalization of an unimproved energy-momentum tensor [40,41,42,43,44]). In the presence of monopoles, the relevant SUSY current is the unimproved one, hence the appearance of infinite renormalizations.…”
mentioning
confidence: 99%