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Multigluonic scattering amplitudes of heavy quarks

High Energy Physics - Phenomenology · Submitted 11 Aug 2005

abstract compiled · 2026-09-23 · no language-model review

The authors' main claim Then, we show that in the heavy top quark effective theory the holomorfic component of the Higgs $\to q \bar{q} + n$-gluon amplitude vanish for helicity conserving configurations.

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arXiv IDhep-ph/0508138 (version 1)
Pith IDBC3UCGWL, Pith's permanent record of this paper and its review
CitationGerman Rodrigo. "Multigluonic scattering amplitudes of heavy quarks." arXiv:hep-ph/0508138 (2005). https://pith.science/paper/BC3UCGWL
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arXiv listing abstract v1. Results and the main claim are underlined; .

We consider heavy quark and antiquark off-shell spinorial currents with emission of an arbitrary number of gluons of positive helicity. From this results we calculate the corresponding on-shell scattering amplitude and the quark-antiquark vector current. Then, we show that in the heavy top quark effective theory the holomorfic component of the Higgs $\to q \bar{q} + n$-gluon amplitude vanish for helicity conserving configurations.

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#sentencerolethe authors' own workstates the main conclusionstrength
s0 We consider heavy quark and antiquark off-shell spinorial currents with emission of an arbitrary number of gluons of positive helicity. contribution 0.95 0.81 0.05 asserted 0.81
s1 From this results we calculate the corresponding on-shell scattering amplitude and the quark-antiquark vector current. contribution 0.48 0.94 0.10 asserted 1.00
s2 Then, we show that in the heavy top quark effective theory the holomorfic component of the Higgs $\to q \bar{q} + n$-gluon amplitude vanish for helicity conserving configurations. result 0.99 0.92 0.64 asserted 1.00

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The paper
Original abstract

We consider heavy quark and antiquark off-shell spinorial currents with emission of an arbitrary number of gluons of positive helicity. From this results we calculate the corresponding on-shell scattering amplitude and the quark-antiquark vector current. Then, we show that in the heavy top quark effective theory the holomorfic component of the Higgs $\to q \bar{q} + n$-gluon amplitude vanish for helicity conserving configurations.

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14 arXiv papers cite this in 16 sentences

Each citing sentence is taken from the citing paper's LaTeX source and typed by Pith's classifier. A label appears at probability 0.8 or more (0.95 for support), a contest at 0.7 or more; the quoted words are the citing authors'. How each label was checked · JSON

Papers citing it · 8 sentences without a confident label

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  • Each such split introduces a relative factor of [equation] It follows that we can write the full amplitude as [equation] This should be compared to the known expression for this amplitude [ref] (see also [ref] ), [equation] We have confirmed the equivalence of these two expressions numerically for $n=3,4,5,6$.

    The Coulomb-branch S-matrix from massless amplitudes · Examples · 1.00

  • [ref] , which take [equation] where $|q±⟩$ is a Weyl spinor for an arbitrary null vector $q$, and $p^♭$ is the null projection of $p$ obtained by subtracting a vector proportional to $q$.

    The MHV QCD Lagrangian · Massive polarisation spinors · 0.98

  • As an example of such massive amplitudes, let us present our result for the all-$n$ tower of tree-level $W$-$W$-gluon amplitudes:[ All-$n$ results for certain amplitudes with two massive states have been given previously in the literature [ref] , but in a different representation that involves quite elaborate sums.

    Massive amplitudes on the Coulomb branch of N=4 SYM · Introduction · 0.94

Cites it as background 4 papers

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