1984
DOI: 10.1016/0034-4877(84)90005-3
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On the structure of the conformal covariant N-point functions

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Cited by 11 publications
(18 citation statements)
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“…Thus, it will be convenient to use the spin-chain frame instead of the string frame. There is a map between the excitations in one frame to the other and our strategy will be to evaluate the hexagon form factor in the string frame using the definitions and crossing rules given above and apply the map 12 We thank Shota Komatsu for informing us about the transformations of the fermionic excitations.…”
Section: A2 String and Spin Chain Framesmentioning
confidence: 99%
“…Thus, it will be convenient to use the spin-chain frame instead of the string frame. There is a map between the excitations in one frame to the other and our strategy will be to evaluate the hexagon form factor in the string frame using the definitions and crossing rules given above and apply the map 12 We thank Shota Komatsu for informing us about the transformations of the fermionic excitations.…”
Section: A2 String and Spin Chain Framesmentioning
confidence: 99%
“…(cos θ − it sin θ) m , (B.3)of the normalized Gegenbauer polynomial derived shortly, we find the result(3.26) 11. This formula is found in the seventh edition of[47].…”
mentioning
confidence: 58%
“…Their conjecture implies that the finite part F n , c.f. (113) has the same functional form as at one loop, F (1) n , multiplied by the (coupling-dependent) cusp anomalous dimension, 31 Strictly speaking, the preceding calculation proves (123) up to terms vanishing as O( ) only, since we used 4-dimensional cuts. To extend the derivation to O( ) terms one could use D-dimensional cuts.…”
Section: Results Of Perturbative Calculationsmentioning
confidence: 90%
“…is the invariant mass of two adjacent gluons with indices i and i + 1, and the periodicity condition 28 . From (113) we can see that MHV amplitudes contain two interesting pieces of information: the cusp anomalous dimension Γ cusp in the double pole term, and an a priori arbitrary function of the momentum invariants in the finite part. What makes the latter particularly interesting is that it turns out not to be arbitrary, but seems to have a very simple form, as we will discuss in Sect.…”
Section: Infrared Divergencesmentioning
confidence: 99%