pith. sign in

arxiv: 1906.08681 · v1 · pith:AFKFEK5Mnew · submitted 2019-06-20 · ✦ hep-ph

Off-shell initial state effects and gauge invariance in the Drell-Yan process

Pith reviewed 2026-05-25 19:36 UTC · model grok-4.3

classification ✦ hep-ph
keywords Drell-Yan processgauge invarianceoff-shell effectshelicity structure functionstransverse momentumparton modelQED
0
0 comments X

The pith

The transverse momentum of initial-state partons can be included in the Drell-Yan process while preserving QED gauge invariance for the helicity structure functions.

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The paper examines how to account for the transverse momentum of initial-state partons in the Drell-Yan process. It shows that this can be done in a manner that keeps the helicity structure functions consistent with QED gauge invariance. This approach also clarifies connections to the conventional transverse momentum dependent parton model. A sympathetic reader would care because accurate inclusion of such effects is important for precise predictions at colliders where partons carry significant transverse motion. The work extends the treatment to off-shell initial states without losing gauge symmetry.

Core claim

The helicity structure functions in the Drell-Yan process can be treated within a framework that incorporates the transverse momentum of initial-state partons in a way that maintains full compatibility with QED gauge invariance, and this treatment relates directly to the standard transverse momentum dependent parton model formalism.

What carries the argument

The inclusion of transverse momentum for initial-state partons in a gauge-invariant manner for the helicity structure functions.

If this is right

  • Drell-Yan cross sections can be calculated with transverse momentum effects included without violating gauge invariance.
  • The helicity structure functions remain well-defined and satisfy the expected QED relations.
  • Connections to the transverse momentum dependent parton model become clearer for practical use.
  • Predictions for lepton pair production can incorporate initial-state transverse motion consistently.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Similar gauge-invariant treatments could be applied to other processes involving initial-state partons at high energies.
  • This might improve the accuracy of parton distribution function extractions from collider data.
  • Further work could test the approach by comparing predicted angular distributions against measurements.

Load-bearing premise

That including the transverse momentum of initial-state partons does not break QED gauge invariance in the helicity structure functions of the Drell-Yan process.

What would settle it

An explicit computation of the structure functions that reveals non-cancellation of gauge-dependent terms when transverse momentum is included.

Figures

Figures reproduced from arXiv: 1906.08681 by Maxim Nefedov, Vladimir Saleev.

Figure 1
Figure 1. Figure 1: Diagrams contributing to the Multi-Regge limit of the process (3.2) in the model theory. Two diagrams where photon interacts with the opposite proton and spectator lines also should be added. and in the Multi-Regge limit: S ≫ Q 2 ∼ q 2 T one has (P ′ 1 ) + ≃ P + 1 = √ S, (P ′ 2 ) − ≃ P − 2 = √ S, qT ∼ q ± ≪ √ S. In this limit, only diagrams in the [PITH_FULL_IMAGE:figures/full_fig_p004_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: Predictions for unpolarized Drell-Yan SFs F (1) UU , F (2) UU and F (cos 2φ) UU in pp-collisions at √ S = 24 GeV [10]. Solid lines with uncertainty bands – PRA predictions. Dashed lines – predictions in the QOS￾scheme [3] for the default scale-choice. Short-dashed line - plot of the (−F (cos2φ) UU ) in the QOS scheme, since this SF in QOS scheme is negative at low qT . Eq. (3.4) is just the Eq. (7) from ou… view at source ↗
read the original abstract

The Helicity Structure Functions in the Drell-Yan process are discussed in a framework of Parton Reggeization Approach, which includes the transverse momentum of initial-state partons in a way compatible with QED gauge-invariance. Relationships with conventional Transverse Momentum Dependent Parton Model formalism are clarified.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

1 major / 0 minor

Summary. The manuscript discusses the helicity structure functions in the Drell-Yan process within the Parton Reggeization Approach (PRA). The central claim is that the PRA incorporates the transverse momentum of initial-state partons in a manner compatible with QED gauge invariance. The paper also aims to clarify the relationships between this framework and the conventional Transverse Momentum Dependent (TMD) parton model formalism.

Significance. If the claimed gauge-invariant treatment of off-shell initial-state effects holds, the work would be significant for high-energy QCD phenomenology. It would provide a consistent way to include transverse momentum effects in Drell-Yan calculations without violating gauge invariance, potentially improving predictions for helicity structure functions and offering a bridge between the PRA and TMD approaches.

major comments (1)
  1. [Abstract] Abstract: The central claim of compatibility with QED gauge invariance when including off-shell initial-state transverse momentum is asserted, but the abstract (and visible text) contains no equations, derivations, or technical steps. This prevents verification of whether the PRA construction actually preserves gauge invariance or reduces to a self-consistent but untested framework, which is load-bearing for the paper's main assertion.

Simulated Author's Rebuttal

1 responses · 0 unresolved

We thank the referee for their report. We address the single major comment below.

read point-by-point responses
  1. Referee: [Abstract] Abstract: The central claim of compatibility with QED gauge invariance when including off-shell initial-state transverse momentum is asserted, but the abstract (and visible text) contains no equations, derivations, or technical steps. This prevents verification of whether the PRA construction actually preserves gauge invariance or reduces to a self-consistent but untested framework, which is load-bearing for the paper's main assertion.

    Authors: Abstracts are concise summaries by design and conventionally omit equations or derivations to remain accessible; the technical construction showing how the Parton Reggeization Approach preserves QED gauge invariance for off-shell initial-state partons is given in full in the body of the manuscript. Readers are expected to consult the main text for verification of the central claim. We do not believe the absence of technical steps from the abstract itself undermines the paper. revision: no

Circularity Check

0 steps flagged

No significant circularity detected

full rationale

The abstract states that the Parton Reggeization Approach includes initial-state transverse momentum compatibly with QED gauge invariance for Drell-Yan helicity structure functions and clarifies relations to the TMD formalism. No derivation chain, equations, fitted parameters, or self-citations are supplied in the provided text that reduce any claimed result to its inputs by construction. The central assertion concerns compatibility with an external principle (gauge invariance), which is not shown to be internally defined or fitted from the target observables. Absent any quoted load-bearing step that matches the enumerated circularity patterns, the derivation is treated as self-contained.

Axiom & Free-Parameter Ledger

0 free parameters · 0 axioms · 0 invented entities

No information available from the abstract to identify free parameters, axioms, or invented entities.

pith-pipeline@v0.9.0 · 5562 in / 1079 out tokens · 27946 ms · 2026-05-25T19:36:15.423491+00:00 · methodology

discussion (0)

Sign in with ORCID, Apple, or X to comment. Anyone can read and Pith papers without signing in.

Lean theorems connected to this paper

Citations machine-checked in the Pith Canon. Every link opens the source theorem in the public Lean library.

What do these tags mean?
matches
The paper's claim is directly supported by a theorem in the formal canon.
supports
The theorem supports part of the paper's argument, but the paper may add assumptions or extra steps.
extends
The paper goes beyond the formal theorem; the theorem is a base layer rather than the whole result.
uses
The paper appears to rely on the theorem as machinery.
contradicts
The paper's claim conflicts with a theorem or certificate in the canon.
unclear
Pith found a possible connection, but the passage is too broad, indirect, or ambiguous to say the theorem truly supports the claim.

Reference graph

Works this paper leans on

13 extracted references · 13 canonical work pages · 10 internal anchors

  1. [1]

    Dilepton production from polarized hadron hadron collisions

    S. Arnold, A. Metz and M. Schlegel, Phys. Rev. D 79, 034005, arXiv:hep-ph/0809.2262, (2009)

  2. [2]

    J. C. Collins, D. E. Soper, Phys. Rev. D 16, 2219, (1977)

  3. [3]

    Off-shell initial state effects, gauge invariance and angular distributions in the Drell-Yan process

    M. Nefedov and V . Saleev, Phys. Lett. B 790, 551, arXiv:hep-ph/1810.04061, (2019)

  4. [4]

    M. A. Nefedov, N. N. Nikolaev and V . A. Saleev, Phys. Rev. D 87, 014022, arXiv:hep-ph/1211.5539, (2013)

  5. [5]

    J. C. Collins, F oundations of perturbative QCD, Cambridge University Press, Cambridge, (2011)

  6. [6]

    Time-reversal odd distribution functions in leptoproduction

    D. Boer and P . J. Mulders, Phys. Rev. D 57, 5780, arXiv:hep-ph/9711485, (1998)

  7. [7]

    V . S. Fadin, V . E. Sherman, JETP Lett. 23 599 (1976); V . S. Fadin, V . E. Sherman, Sov. Phys. JETP45 861 (1977)

  8. [8]

    A. V . Bogdan and V . S. Fadin, Nucl. Phys. B 740, 36, arXiv:hep-ph/0601117, (2006)

  9. [9]

    D. Boer, T. van Daal, J. R. Gaunt, T. Kasemets and P . J. Muld ers, SciPost Phys. 3, 040, arXiv:hep-ph/1709.04935, (2017)

  10. [10]

    I. A. Savin et al., EPJ Web Conf. 85, 02039, arXiv:hep-ph/1408.3959, (2015)

  11. [11]

    M. A. Kimber, A. D. Martin, M. G. Ryskin, Phys. Rev. D 63, 114027, arXiv:hep-ph/0101348, (2001)

  12. [12]

    A. D. Martin, W . J. Stirling, R. S. Thorne, G. Watt, Eur. P hys. J. C 63, 189, arXiv:hep-ph/0901.0002, (2009)

  13. [13]

    L. Y . Zhu, et al., Phys. Rev. Lett. 102, 182001, arXiv:hep-ph/0811.4589, (2009). 5