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All-Multiplicity Amplitudes with Massive Scalars
High Energy Physics - Theory · Submitted 29 Jul 2005
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We compute two infinite series of tree-level amplitudes with a massive scalar pair and an arbitrary number of gluons.
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The abstract, sentence by sentence
We compute two infinite series of tree-level amplitudes with a massive scalar pair and an arbitrary number of gluons. We provide results for amplitudes where all gluons have identical helicity, and amplitudes with one gluon of opposite helicity. These amplitudes are useful for unitarity-based one-loop calculations in nonsupersymmetric gauge theories generally, and QCD in particular.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We compute two infinite series of tree-level amplitudes with a massive scalar pair and an arbitrary number of gluons. | contribution 0.97 | 0.96 | 0.46 | asserted 1.00 |
| s1 | We provide results for amplitudes where all gluons have identical helicity, and amplitudes with one gluon of opposite helicity. | result 0.68 | 0.95 | 0.20 | asserted 1.00 |
| s2 | These amplitudes are useful for unitarity-based one-loop calculations in nonsupersymmetric gauge theories generally, and QCD in particular. | interpretation 1.00 | 0.21 | 0.20 | asserted 0.99 |
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The paper
Original abstract
We compute two infinite series of tree-level amplitudes with a massive scalar pair and an arbitrary number of gluons. We provide results for amplitudes where all gluons have identical helicity, and amplitudes with one gluon of opposite helicity. These amplitudes are useful for unitarity-based one-loop calculations in nonsupersymmetric gauge theories generally, and QCD in particular.
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References
How the literature uses it
20 arXiv papers cite this in 33 sentences
Papers citing it · 24 sentences without a confident label
Uses its method or tool 2 papers
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The rational part contribution to a scalar amplitude can be extracted by introducing an effective mass $μ^2$ for the scalar and by evaluating the integral coefficient in four dimensions with the tree-level amplitudes for massive scalars [ref] .
Simplicity in the Structure of QED and Gravity Amplitudes · Absence of rational terms · 0.90
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The required tree level amplitudes have been generated using on-shell recursion relations literature [ref] .
Direct Extraction Of One Loop Rational Terms · Remaining helicity configurations · 0.99
Compares with it 4 papers
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Evaluated on the solution to the scattering equations, this gives: [equation] We can now evaluate the amplitude for different helicity assignments: [equation] These expressions match the results obtained in [ref] .
Massive ambitwistor-strings; twistorial models · Amplitudes · 0.99
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Using the prescription [ref] for both the internal off-shell momenta and the external scalars, the remaining two diagrams give (using the notation $y_i,j=k_i,j^2-m^2$) [equation] This can be shown to be equivalent to the known result [ref] .
Deriving CSW rules for massive scalar legs and pure Yang-Mills loops · Tree level examples · 0.98
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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
Cites it as background 2 papers
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After initial explorations of BCFW recursion for amplitudes with massive particles [ref] , it was shown that amplitudes in QCD with massive quarks can be constructed using at most three-line shifts [ref] whereas the on-shell constructibility of amplitudes in massive, power-counting renormalizable theories using all-line shifts was proven in [ref] .
On-shell constructibility of Born amplitudes in spontaneously broken gauge theories · Introduction · 0.85
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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
Discussion
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