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1999
DOI: 10.1016/s0550-3213(99)00583-0
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One-loop splitting amplitudes in gauge theory

Abstract: We recompute the functions describing the collinear factorization of one-loop amplitudes using the unitarity-based method. We present the results in a form suitable for use as an ingredient in two-loop calculations. We also present a function summarizing the behavior at one loop in both the soft and collinear limits.

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Cited by 207 publications
(266 citation statements)
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References 39 publications
(39 reference statements)
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“…Since the splitting matrix Sp (1) , and in particle I C , is the only part of the virtuals that depend on s 12 , we can focus only on this term. The divergent terms in the (UV-renormalized) 1-loop splitting matrix are [43] …”
Section: Jhep03(2014)119mentioning
confidence: 99%
“…Since the splitting matrix Sp (1) , and in particle I C , is the only part of the virtuals that depend on s 12 , we can focus only on this term. The divergent terms in the (UV-renormalized) 1-loop splitting matrix are [43] …”
Section: Jhep03(2014)119mentioning
confidence: 99%
“…Explicit results for the splitting amplitudes Split (1) in d = 4−2ǫ dimensions (or, equivalently, the results to all orders in the ǫ expansion) were obtained in Refs. [12,25].…”
Section: Introductionmentioning
confidence: 99%
“…On the other hand, the requirement of building m-jets from (m + 1)-partons allows one of the final state partons to become unresolved, leading to implicit local infrared singularities which become explicit only after integration over the unresolved patch of the final state (m + 1)-parton phase space. The single unresolved infrared singularity structure of one-and two-loop amplitudes has been studied in [78][79][80][81][82][83][84][85][86][87][88][89][90].…”
Section: Real-virtual Antenna Subtraction At Nnlomentioning
confidence: 99%
“…In single unresolved limits, the behaviour of (m+3)-parton one-loop amplitudes is described by the sum of two different contributions [78][79][80][81][82]: a single unresolved tree-level factor times a (m + 2)-parton one-loop amplitude and a single unresolved one-loop factor times a (m+2)-parton tree-level amplitude, as illustrated in Figure 1. Accordingly, we construct the one-loop single unresolved subtraction term from products of tree-and one-loop antenna functions with one-loop and tree-amplitudes respectively.…”
Section: One-loop Single-unresolved Contributions: Dσ V Sa N N Lomentioning
confidence: 99%