Pith. sign in

REVIEW 4 cited by

Hadron spectroscopy at STCF

Not yet reviewed by Pith; the record is open.

Re-run · record.json Download PDF Read on arXiv ↗

This paper has not been read by Pith yet. Machine review is queued; the pith claim, tier, and objections will appear here once it completes.

SPECIMEN: schema-true, not a live event

T0 review · schema-true

One-sentence machine reading of the paper's core claim.

pith:XXXXXXXX · record.json · timestamp

arxiv 2203.07141 v2 pith:TMOPQXL7 submitted 2022-03-14 hep-ph

Feng-Kun Guo , Haiping Peng , Ju-Jun Xie , Xiaorong Zhou This is my paper · ORCID
classification hep-ph
keywords hadronspectroscopystcfcolorconfinementessentialhadronsinteraction
verification ladder T0 review T1 audit T2 compute T3 formal
0 comments
read the original abstract

Despite that quantum chromodynamics, the theory of strong interaction, has colorful quarks and gluons as its basic degrees of freedom, all fundamental particles participating the strong interaction that can be directly detected in experiments are colorless or color-singlet hadrons. This phenomenon is called color confinement. Because of that, the study of hadron spectroscopy is essential in improving our understanding of the nonperturbative regime of QCD and to reveal the mechanism of color confinement. The high-luminosity electron-positron collision machine under discussion, Super tau-Charm Facility (STCF), can play an essential role in hadron spectroscopy by discovering new hadron resonances and measuring properties of known hadrons with an unprecedented precision. In the following, we will discuss briefly the topics on hadron spectroscopy that will be investigated at STCF.

Discussion (0). Continue with ORCID to comment.

Forward citations

Cited by 4 Pith papers

Reviewed papers in the Pith corpus that reference this work. Sorted by Pith novelty score. Full citation record

  1. Diffusion Monte Carlo study of deuteron-like fully light hexaquarks

    hep-ph 2026-07 conditional novelty 5.0 of 10

    Within the AL1 constituent-quark model, compact uuuddd hexaquarks lie well above baryon–baryon thresholds while dibaryon-like states are near-threshold molecular candidates, one deuteron-like but unbound by ~12 MeV.

  2. Roles of the $N(1535)$ and $a_0(980)$ in the process $\Lambda_c^+ \to \pi^+\eta n$

    hep-ph 2025-01 conditional novelty 5.0 of 10

    A chiral unitary calculation predicts near-threshold N(1535) and a0(980) signals in Λc+ → π+ηn, with B(Λc→a0 n)/B(Λc→π+ηn) ≈ 0.313.

  3. Triply heavy tetraquarks $\bar{b}c\bar{q}c$ and $\bar{c}b\bar{q}b$ in a constituent quark model

    hep-ph 2025-07 conditional novelty 4.0 of 10

    A constituent quark model predicts dozens of narrow tetraquark resonances in the mixed beauty-charm systems \bar{b}c\bar{q}c and \bar{c}b\bar{q}b.

  4. Predictions for Bottomonium from a Relativistic Screened Potential Model

    hep-ph 2025-01 conditional novelty 4.0 of 10

    A screened relativistic potential model reproduces many low-lying bottomonium masses and proposes S-D mixing assignments for Upsilon(10355), Upsilon(10580), Upsilon(10753), Upsilon(10860), and Upsilon(11020).

Pith tools