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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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The abstract, sentence by sentence
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.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| 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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References
How the literature uses it
14 arXiv papers cite this in 16 sentences
Papers citing it · 8 sentences without a confident label
Uses its method or tool 1 paper
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The implementation of the Kleiss-Stirling scheme appropriate for the case where we have pairs of massive particles is due to Rodrigo [ref] .
QCD corrections to the hadronic production of a heavy quark pair and a W-boson including decay correlations · Special choice for massive spinors · 0.94
Compares with it 3 papers
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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
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[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
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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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One could ask the question whether similar techniques can be used in QCD, whether they are of any practical use, and in fact to which degree they were already included in previous work, such as for example at the foundation of parton shower algorithms (new or well established) [ref] or for other, fundamental or phenomenological applications [ref] .
Gauge invariant sub-structures of tree-level double-emission exact QCD spin amplitudes · Introduction · 0.96
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The application to massive particles is less explored, although processes involving massive quarks were calculated in [ref] and massive gauge bosons in [ref] .
The Rise of SMEFT On-shell Amplitudes · Introduction · 0.86
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The spinor-helicity method applied to massive fermions has been well studied and we refer the reader to Refs. [ref] for further details and other approaches.
Two-loop leading colour QCD helicity amplitudes for top quark pair production in the gluon fusion channel · Helicity amplitudes for massive fermions · 1.00
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