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Analysis of Fully-Heavy and Hidden-Heavy Tetraquarks in Anisotropic Plasma Using the Generalized Fractional Derivatives

High Energy Physics - Phenomenology · Submitted 20 Jun 2026

Pith's verdict: Applies GFD and PGFNU to tetraquark masses and dissociation in anisotropic plasma as a tunable phenomenological model with clear numerical trends but no first-principles justification.

T0 · AI review

How this review was made: An AI referee (grok-4.3) read the paper on June 26, 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.

  1. T0 AI review An AI read the paper and answered a fixed list of questions.
  2. T1 Audit Automatic checks that the references and files the paper relies on exist and match.
  3. T2 Compute The paper's code or calculations re-run with the same results.
  4. T3 Formal statement The claims written out in a formal math language a computer can read.
  5. T4 Proof Those claims proved, and the proof checked by computer.

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arXiv ID2606.23732 (version 3)
Pith IDKOHYFNYP, Pith's permanent record of this paper and its review
CitationE. M. Khokha, H. M. Fath-Allah, M. Abu-shady. "Analysis of Fully-Heavy and Hidden-Heavy Tetraquarks in Anisotropic Plasma Using the Generalized Fractional Derivatives." arXiv:2606.23732 (2026). https://pith.science/paper/KOHYFNYP
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Referee report
The paper

The paper claims

The generalized fractional derivative framework models tetraquark spectroscopy and dissociation in anisotropic plasma, agreeing with prior studies.

The reading

This paper applies the generalized fractional derivative (GFD) structure to solve the radial Schrödinger equation for tetraquarks in anisotropic plasma using an extended Cornell potential with Debye screening and anisotropy. The parametric generalised fractional Nikiforov-Uvarov (PGFNU) technique is used to find that binding potential and dissociation energy increase with anisotropy but decrease with temperature. Lower fractional orders lead to more strongly bound systems than in classical quantum mechanics. Mass spectra are calculated for cc cbar cbar, bb bbar bbar, and mixed systems in fractional and classical regimes. The GFD is shown to be an effective basis for modeling hadronic systems in complex contexts with agreement to earlier studies.

What carries the argument

Generalized fractional derivative (GFD) structure and the parametric generalised fractional Nikiforov-Uvarov (PGFNU) technique for solving the radial Schrödinger equation with extended Cornell potential.

Extended reading notes

Core claim

The radial Schrödinger equation with an extended Cornell potential that includes Debye screening and plasma anisotropy is solved by applying the parametric generalised fractional Nikiforov-Uvarov (PGFNU) technique within the generalized fractional derivative structure, yielding mass spectra and showing that the binding potential of the systems and the dissociation energy increase with the anisotropy parameter and decrease with temperature, with systems more strongly bound at lower fractional orders than in classical quantum mechanics.

Load-bearing premise

The extended Cornell potential with Debye screening and anisotropy terms, together with the generalized fractional derivative replacement in the radial Schrödinger equation, correctly captures the confinement dynamics of tetraquarks in anisotropic plasma.

Original abstract

Investigating the spectroscopy and thermal stability of exotic multiquark states provides crucial insights into the fundamental confinement mechanisms of quantum chromodynamics (QCD) under extreme regimes. This work presents an innovative study of the spectroscopy and dissociation of fully-heavy tetraquarks in an anisotropic plasma via the generalized fractional derivative (GFD) structure. The radial Schr\"odinger equation (SE) with an extended Cornell potential that includes Debye screening and plasma anisotropy into account is solved by applying the parametric generalised fractional Nikiforov-Uvarov (PGFNU) technique. The analysis of systems consisting of $cc\bar c\bar c$ and $bb\bar{b}\bar{b}$ shows that the binding potential of the systems and the dissociation energy increase with the anisotropy parameter and decrease with temperature. The fractional paradigm also shows that when the fractional orders are lower, the systems will be more strongly bound than in classical quantum mechanics. Furthermore, the mass spectra for all considered tetraquark configurations, including the $cc\bar{c}\bar{c}$, $bb\bar{b}\bar{b}$, $c\bar{q}c\bar{q}$, and $b\bar{q}b\bar{q}$ systems, are calculated for both ground and excited states. These calculations were performed across both the fractional and classical regimes. The findings indicate that the GFD framework provides an effective mathematical basis for modelling hadronic systems in complex contexts, and they demonstrate significant agreement with earlier theoretical studies.

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, 6,544 input tokens.

What the abstract itself states, as probabilities: claims first 0.09 · states limitation 0.07 · human participants 0.01 · controlled comparison 0.37 · randomized assignment 0.01 · states quantitative result 0.10 · compares with prior results 0.89 · mentions code or data availability 0.02.

The abstract, sentence by sentence

arXiv listing abstract v3. Results and the main claim are underlined; .

Investigating the spectroscopy and thermal stability of exotic multiquark states provides crucial insights into the fundamental confinement mechanisms of quantum chromodynamics (QCD) under extreme regimes. This work presents an innovative study of the spectroscopy and dissociation of fully-heavy tetraquarks in an anisotropic plasma via the generalized fractional derivative (GFD) structure. The radial Schr\"odinger equation (SE) with an extended Cornell potential that includes Debye screening and plasma anisotropy into account is solved by applying the parametric generalised fractional Nikiforov-Uvarov (PGFNU) technique. The analysis of systems consisting of $cc\bar c\bar c$ and $bb\bar{b}\bar{b}$ shows that the binding potential of the systems and the dissociation energy increase with the anisotropy parameter and decrease with temperature. The fractional paradigm also shows that when the fractional orders are lower, the systems will be more strongly bound than in classical quantum mechanics. Furthermore, the mass spectra for all considered tetraquark configurations, including the $cc\bar{c}\bar{c}$, $bb\bar{b}\bar{b}$, $c\bar{q}c\bar{q}$, and $b\bar{q}b\bar{q}$ systems, are calculated for both ground and excited states. These calculations were performed across both the fractional and classical regimes. The findings indicate that the GFD framework provides an effective mathematical basis for modelling hadronic systems in complex contexts, and they demonstrate significant agreement with earlier theoretical studies.

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 Investigating the spectroscopy and thermal stability of exotic multiquark states provides crucial insights into the fundamental confinement mechanisms of quantum chromodynamics (QCD) under extreme regimes. background 1.00 0.06 0.03 asserted 0.99
s1 This work presents an innovative study of the spectroscopy and dissociation of fully-heavy tetraquarks in an anisotropic plasma via the generalized fractional derivative (GFD) structure. contribution 1.00 0.94 0.06 asserted 0.98
s2 The radial Schr\"odinger equation (SE) with an extended Cornell potential that includes Debye screening and plasma anisotropy into account is solved by applying the parametric generalised fractional Nikiforov-Uvarov (PGFNU) technique. method 1.00 0.92 0.04 asserted 1.00
s3 The analysis of systems consisting of $cc\bar c\bar c$ and $bb\bar{b}\bar{b}$ shows that the binding potential of the systems and the dissociation energy increase with the anisotropy parameter and decrease with temperature. result 1.00 0.94 0.35 asserted 1.00
s4 The fractional paradigm also shows that when the fractional orders are lower, the systems will be more strongly bound than in classical quantum mechanics. result 0.96 0.86 0.16 asserted 0.98
s5 Furthermore, the mass spectra for all considered tetraquark configurations, including the $cc\bar{c}\bar{c}$, $bb\bar{b}\bar{b}$, $c\bar{q}c\bar{q}$, and $b\bar{q}b\bar{q}$ systems, are calculated for both ground and excited states. contribution 0.49 0.95 0.06 asserted 1.00
s6 These calculations were performed across both the fractional and classical regimes. method 0.91 0.91 0.03 asserted 0.97
s7 The findings indicate that the GFD framework provides an effective mathematical basis for modelling hadronic systems in complex contexts, and they demonstrate significant agreement with earlier theoretical studies. interpretation 0.97 0.87 0.73 asserted 0.84

What kind of paper the classifier reports this is: theoretical result 0.90 · evidence from proof or derivation 0.56.

What was examined, and what was not

sources read
  • arXiv listing abstract v3
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. Plot of the dissociation energy of p-state of ccc¯c¯ with T and different values of ξ at (a) θ = 0, α = 0.01, (b) θ = 0, α = 1, (c) θ = 90, α = 0.01 and (d) θ = 90, α = 1 14
Figure 2. Plot of the dissociation energy of p-state of bb¯b ¯b with T and different values of ξ at (a) θ = 0, α = 0.01, (b) θ = 0, α = 1, (c) θ = 90, α = 0.01 and (d) θ = 90, α = 1 15

Figures reproduced from arXiv:2606.23732 by the authors.

Discussion

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