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TQ4Q2.0 Fragmentation Functions for Fully Heavy Tetraquark Production

High Energy Physics - Phenomenology · Submitted 3 Sep 2026 · 77 references

Pith's verdict: Honest, self-referential proceedings summary: the only new content is two figure panels, and the signature intrinsic-charm claim rests on a deferred same-author Landau–Yang argument.

T0 · AI review

How this review was made: An AI referee (deepseek/deepseek-v4-flash) read the paper on September 8, 2026 and answered a fixed list of questions about it. T0 is the starting level every paper gets. The levels describe how deeply Pith has checked the paper, never the authors.

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  3. T2 Compute The paper's code or calculations re-run with the same results.
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  5. T4 Proof Those claims proved, and the proof checked by computer.

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arXiv ID2609.04049 (version 1)
Pith IDRE62X3VO, Pith's permanent record of this paper and its review
CitationFrancesco Giovanni Celiberto. "TQ4Q2.0 Fragmentation Functions for Fully Heavy Tetraquark Production." arXiv:2609.04049 (2026). https://pith.science/paper/RE62X3VO
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Claim paper

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Referee report
The paper

The paper claims

Axial-vector all-charm tetraquark fragmentation is an intrinsic-charm probe.

The reading

This paper constructs TQ4Q2.0, a new set of collinear fragmentation functions for fully heavy tetraquarks, covering scalar, axial-vector, and tensor configurations. The functions are built from NRQCD initial conditions at the starting scale and evolved across heavy-flavor thresholds using the HF-NRevo scheme, with both perturbative missing-order uncertainties and nonperturbative long-distance matrix-element variations propagated through a 100-member replica ensemble. The central claim is that the axial-vector $1^{+-}$ channel is dominated by charm-quark fragmentation because the gluon channel is forbidden by the Landau-Yang constraint and other partonic contributions are strongly suppressed. This makes axial-vector tetraquark production a selective probe of intrinsic charm in the proton, especially in forward kinematics at the LHC and future colliders. If correct, TQ4Q2.0 provides an uncertainty-aware baseline that connects exotic-hadron spectroscopy directly to proton partonic structure.

What carries the argument

The central machinery is the combination of NRQCD factorization (separating short-distance coefficients from color-composite long-distance matrix elements) with the HF-NRevo threshold-aware DGLAP evolution scheme. The fragmentation functions are initialized at scale $\mu_F = 2m_Q$ using NLO NRQCD inputs for all parton channels, then evolved to higher scales. Uncertainties are quantified by a 100-member Monte-Carlo-like replica ensemble that samples fragmentation-scale variations and LDME variations, propagated through the full evolution. The specific suppression of the gluon channel for the axial-vector $1^{+-}$ state follows from the Landau-Yang theorem applied to NRQCD, which is the mechanism that gives the charm-initiated channel its special sensitivity to intrinsic charm.

Extended reading notes

Core claim

The paper establishes TQ4Q2.0 as a full set of collinear fragmentation functions for fully heavy tetraquarks, derived from NLO NRQCD factorization for all relevant partonic channels and evolved through the HF-NRevo scheme. A key discovery is that the axial-vector $T_{4c}(1^{+-})$ state has no gluon-initiated fragmentation contribution at the initial scale due to the Landau-Yang constraint, and non-constituent-quark contributions are suppressed by charge conjugation. This forces the charm-quark fragmentation channel to dominate, making axial-vector tetraquark production uniquely sensitive to the intrinsic charm component of the proton wave function. The paper also provides a joint propagation of perturbative missing higher-order uncertainties and nonperturbative LDME uncertainties via a 100-member replica ensemble, enabling direct phenomenological applications.

Load-bearing premise

The paper assumes that the gluon fragmentation channel for the axial-vector tetraquark is exactly forbidden by the Landau-Yang constraint and that non-constituent-quark contributions are negligible due to charge conjugation, so that charm fragmentation completely dominates the production.

Editorial extensions

If this is right

  • TQ4Q2.0 provides predictions for scalar, axial-vector, and tensor fully heavy tetraquark production at the LHC, HL-LHC, and FCC with full uncertainty bands, enabling direct comparison with upcoming measurements.
  • The axial-vector channel's charm dominance means that a measurement of $T_{4c}(1^{+-})$ production, especially in forward configurations, can serve as a clean test of the intrinsic-charm hypothesis independent of other channels like $Z+c$ or prompt $D$ mesons.
  • The all-parton setup allows studies of channel competition: for scalar and tensor states gluon and heavy-quark channels both contribute, so their relative strength probes the shape of the parton distributions at large $x$.
  • The uncertainty quantification methodology (F-MHOU + LDME replicas) can be applied to other heavy-hadron fragmentation function sets, improving the reliability of exotic-hadron phenomenology.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • If the axial-vector channel truly isolates intrinsic charm, then a measurement of $p p \to T_{4c}(1^{+-}) + X$ at the LHC can be used to extract the intrinsic charm PDF, providing a complementary constraint to global PDF fits.
  • The Landau-Yang suppression of gluon fragmentation might generalize to other $J^{PC}$ states (e.g., $0^{-+}$, $2^{-+}$) for which gluon fragmentation is forbidden, identifying a class of exotic hadrons that are natural probes of intrinsic heavy flavor.
  • The uncertainty framework in TQ4Q2.0 could be extended to pentaquark and triply-heavy baryon fragmentation functions, as the author has already begun to do in parallel work, potentially creating a unified set of exotic-hadron fragmentation functions.
Original abstract

We investigate the fragmentation dynamics underlying the production of fully heavy tetraquarks by means of the TQ4Q2.0 collinear FF set, covering scalar ($0^{++}$), axial-vector ($1^{+-}$), and tensor ($2^{++}$) configurations. The fragmentation inputs are determined within NRQCD factorization for the complete set of relevant partonic channels and are subsequently evolved across heavy-flavor thresholds through the HF-NRevo scheme. Perturbative uncertainties associated with fragmentation-scale variations are consistently propagated together with nonperturbative effects encoded in color-composite long-distance matrix elements. Attention is devoted to the axial-vector sector, whose fragmentation pattern makes it especially sensitive to intrinsic-charm contributions at LHC and FCC energies. TQ4Q2.0 therefore provides an uncertainty-aware framework for exploring fully heavy tetraquark production over a broad kinematic range and for connecting exotic-hadron spectroscopy with the partonic structure of the proton.

The compiled record

The paper's own sentences, arranged, kept beside the review and separate from it. 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.

Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 4,414 input tokens.

What the abstract itself states, as probabilities: claims first 0.04 · states limitation 0.22 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.04 · compares with prior results 0.06 · mentions code or data availability 0.06.

The abstract, sentence by sentence

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

We investigate the fragmentation dynamics underlying the production of fully heavy tetraquarks by means of the TQ4Q2.0 collinear FF set, covering scalar ($0^{++}$), axial-vector ($1^{+-}$), and tensor ($2^{++}$) configurations. The fragmentation inputs are determined within NRQCD factorization for the complete set of relevant partonic channels and are subsequently evolved across heavy-flavor thresholds through the HF-NRevo scheme. Perturbative uncertainties associated with fragmentation-scale variations are consistently propagated together with nonperturbative effects encoded in color-composite long-distance matrix elements. Attention is devoted to the axial-vector sector, whose fragmentation pattern makes it especially sensitive to intrinsic-charm contributions at LHC and FCC energies. TQ4Q2.0 therefore provides an uncertainty-aware framework for exploring fully heavy tetraquark production over a broad kinematic range and for connecting exotic-hadron spectroscopy with the partonic structure of the proton.

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 investigate the fragmentation dynamics underlying the production of fully heavy tetraquarks by means of the TQ4Q2.0 collinear FF set, covering scalar ($0^{++}$), axial-vector ($1^{+-}$), and tensor ($2^{++}$) configurations. contribution 0.99 0.92 0.09 asserted 0.98
s1 The fragmentation inputs are determined within NRQCD factorization for the complete set of relevant partonic channels and are subsequently evolved across heavy-flavor thresholds through the HF-NRevo scheme. method 1.00 0.84 0.05 asserted 1.00
s2 Perturbative uncertainties associated with fragmentation-scale variations are consistently propagated together with nonperturbative effects encoded in color-composite long-distance matrix elements. method 0.98 0.80 0.06 asserted 1.00
s3 Attention is devoted to the axial-vector sector, whose fragmentation pattern makes it especially sensitive to intrinsic-charm contributions at LHC and FCC energies. interpretation 0.35 0.47 0.09 asserted 0.97
s4 TQ4Q2.0 therefore provides an uncertainty-aware framework for exploring fully heavy tetraquark production over a broad kinematic range and for connecting exotic-hadron spectroscopy with the partonic structure of the proton. interpretation 0.64 0.72 0.67 asserted 0.99

What kind of paper the classifier reports this is: method or tool 0.75 · evidence from simulation or computation 0.93.

What was examined, and what was not

sources read
  • arXiv listing abstract v1
not examined
  • full text
  • figures and tables
  • references and citing sentences
  • relations to other papers
levels run
  • P abstract
not run
  • S sections
  • T body sentences
  • C citations
  • R cross-paper relations

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

Figures
Figure 1. TQ4Q2.0 FFs as functions of 𝑧 for charm-initiated (left) and gluon-initiated (right) production of axial-vector 𝑇4𝑐 (1 +−) (upper) and tensor 𝑇4𝑐 (2 ++) (lower) states at representative energy scales. The main panels display the combined F-MHOU and LDME uncertainty bands, while the lower panels disentangle the corresponding F-MHOU replica envelopes and LDME variations, normalized to the respective central predictions. tative TQ4Q2.0 results for charm- (left) and gluon-initiated (right) fragmentation into all-charm tetraquarks at different energy scales. Upper panels refer to the…

Figures reproduced from arXiv:2609.04049 by the authors.

References
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Found among the papers closest to this one by title and main claim. Pith's classifier compared each pair's main results and a second model family confirmed the relation; checked against two further families, shown conflicts agreed 118 times in 120 and shown same results 218 times in 239. The quoted sentence is the other paper's main claim.

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Discussion

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