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Single spin asymmetries from a gluonic background in the Drell-Yan process
High Energy Physics - Phenomenology · Submitted 2 Oct 1997
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Both gluonic poles and time-reversal odd distribution functions can lead to the same single spin asymmetries.
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The abstract, sentence by sentence
We discuss the effects of so-called gluonic poles in twist-three hadronic matrix elements, as first considered by Qiu and Sterman, in the Drell-Yan process. These effects cannot be distinguished from those of time-reversal odd distribution functions, although time-reversal invariance is not broken by the presence of gluonic poles. Both gluonic poles and time-reversal odd distribution functions can lead to the same single spin asymmetries. We explicitly show the connection between gluonic poles and large distance gluon fields, identify the possible single spin asymmetries in the Drell-Yan process and discuss the role of intrinsic transverse momentum of the partons.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the effects of so-called gluonic poles in twist-three hadronic matrix elements, as first considered by Qiu and Sterman, in the Drell-Yan process. | contribution 0.56 | 0.48 | 0.08 | asserted 0.73 |
| s1 | These effects cannot be distinguished from those of time-reversal odd distribution functions, although time-reversal invariance is not broken by the presence of gluonic poles. | interpretation 0.50 | 0.17 | 0.24 | asserted 1.00 |
| s2 | Both gluonic poles and time-reversal odd distribution functions can lead to the same single spin asymmetries. | result 0.78 | 0.22 | 0.42 | hedged possibility 0.77 |
| s3 | We explicitly show the connection between gluonic poles and large distance gluon fields, identify the possible single spin asymmetries in the Drell-Yan process and discuss the role of intrinsic transverse momentum of the partons. | contribution 1.00 | 0.92 | 0.25 | asserted 0.99 |
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The paper
Original abstract
We discuss the effects of so-called gluonic poles in twist-three hadronic matrix elements, as first considered by Qiu and Sterman, in the Drell-Yan process. These effects cannot be distinguished from those of time-reversal odd distribution functions, although time-reversal invariance is not broken by the presence of gluonic poles. Both gluonic poles and time-reversal odd distribution functions can lead to the same single spin asymmetries. We explicitly show the connection between gluonic poles and large distance gluon fields, identify the possible single spin asymmetries in the Drell-Yan process and discuss the role of intrinsic transverse momentum of the partons.
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References
How the literature uses it
14 arXiv papers cite this in 23 sentences
Papers whose main result relates to this one's
States the same result 1 paper
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Even though time-reversal invariance is not broken, the effects of such poles cannot be distinguished from those of time-reversal odd distribution functions.
Papers citing it · 14 sentences without a confident label
Uses its data or values 1 paper
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The derived relations are verified numerically using unpolarized TMDs from the recent N4LL extraction ART23 [ref] , demonstrating the consistency of the method. * The first TMM provides information about the distribution of the average transverse momentum shift of partons [ref] , and it is expressed via collinear distributions of twist three.
Transverse momentum moments · Introduction · 0.81
Compares with it 2 papers
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We extract the imaginary part of the pole by using the formula [equation] Collecting all the pieces we finally arrive at the following polarized differential cross section, [equation] This provides the asymmetry [equation] which, as already stated above, is just half of the result ([ref]) obtained in Refs. [ref] .
Transverse single spin asymmetry in the Drell-Yan process · Asymmetry derived in covariant gauge · 0.97
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In the second step, we collect by $k_T$ and $p_T$ to simplify the comparison with Eq. (4.5) in Bacchetta:2006tn, which reads [Compared to their original notation, we have exchanged $↔$, and used that their unit vector $ĥ = P⃗_hT / P_hT = (1, 0)$ in our conventions.] [equation] Comparing WUU_oursWUU_theirs, we find agreement if [equation] which is precisely relation_eom that results from the QCD equations of motion [ref] .
Factorization for Azimuthal Asymmetries in SIDIS at Next-to-Leading Power · Illustration for $W_UU^cosϕ_h$ · 0.89
Cites it as background 5 papers
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Among the leading-twist TMD PDFs, the Sivers function [ref] is one of the most interesting and it is widely investigated in $p^↑p →h X$ inclusive processes [ref] .
Estimates for the single-spin asymmetries in $p^{\uparrow}p \to J/\psi X$ process at PHENIX RHIC and SPD NICA · Introduction · 1.00
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The quark-gluon-quark distributions are real-valued functions that satisfy the symmetry relations [equation] Often it is convenient to use the following combination [equation] In the literature one can find different notations for these distributions [ref] .
Sivers, Boer-Mulders and worm-gear distributions at next-to-leading order · Collinear distributions of twist-three · 0.99
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For example, the transverse momentum dependent (TMD) parton distribution functions (PDF) and fragmentation functions (FF) [ref] were introduced, and a TMD factorization formalism [ref] was developed.
Flavor, transverse momentum, and azimuthal dependence of charged pion multiplicities in SIDIS with 10.6 GeV electrons · Theoretical interpretation · 0.88
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