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DVCS off deuteron and twist three contributions

High Energy Physics - Phenomenology · Submitted 12 Nov 2010

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

The authors' main claim We discuss the role of twist three contributions for restoring the QED gauge invariance of the amplitude corresponding to this process.

how it is stated · asserted 0.71 read the record →

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arXiv ID1011.2853 (version 1)
Pith IDURNYKVSH, Pith's permanent record of this paper and its review
CitationB.Pire, I.V.Anikin, O.V.Teryaev, R.S.Pasechnik. "DVCS off deuteron and twist three contributions." arXiv:1011.2853 (2010). https://pith.science/paper/URNYKVSH
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.

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Compiled by classifier-1.13-20260917 via OpenRouter, question bank abstract-p1-20260923, 2026-09-23: 1 request, 2,884 input tokens, $0.0001 reported.

What the abstract itself states, as probabilities: claims first 0.03 · states limitation 0.08 · human participants 0.02 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.03 · compares with prior results 0.05 · mentions code or data availability 0.01.

The abstract, sentence by sentence

arXiv listing abstract v1. Results and the main claim are underlined; .

We study the deeply virtual Compton scattering off a spin-one particle, which is exemplified by the case of coherent scattering on a deuteron target. We discuss the role of twist three contributions for restoring the QED gauge invariance of the amplitude corresponding to this process. We consider both kinematical and dynamical sources of twist three generalized parton distributions.

background contribution method result interpretation main claim

What the classifier reports for each sentence. The number is the probability it gave the label.
#sentencerolethe authors' own workstates the main conclusionstrength
s0 We study the deeply virtual Compton scattering off a spin-one particle, which is exemplified by the case of coherent scattering on a deuteron target. contribution 0.95 0.72 0.05 asserted 0.97
s1 We discuss the role of twist three contributions for restoring the QED gauge invariance of the amplitude corresponding to this process. contribution 0.91 0.64 0.24 asserted 0.71
s2 We consider both kinematical and dynamical sources of twist three generalized parton distributions. contribution 0.98 0.77 0.08 asserted 0.73

What kind of paper the classifier reports this is: theoretical result 1.00 · evidence from proof or derivation 0.80.

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Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. Every number in the measurements table is the authors', checked by code. Record as JSON

The paper
Original abstract

We study the deeply virtual Compton scattering off a spin-one particle, which is exemplified by the case of coherent scattering on a deuteron target. We discuss the role of twist three contributions for restoring the QED gauge invariance of the amplitude corresponding to this process. We consider both kinematical and dynamical sources of twist three generalized parton distributions.

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References
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1 arXiv paper cite this in 2 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

What it cites

Cites as background 1 paper
  • One of the main reasons of this interest is the fact that the DVCS process gives information about a new type of parton distributions, called generalized parton distributions (GPDs) which allow to extract much information about the quark and gluon structure of hadrons, particularly its spin structure [ref] , and to allow a femtophotography of nuclei [ref] .

    Angular momentum sum rule in nuclei · Introduction. · 0.84

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