Spin-2 QQQ̅s̅ Tetraquarks in QCD Sum Rules
Abstract
The JP=2+ ccc̅s̅ and bbb̅s̅ tetraquarks are studied in parallel within the two-point QCD Sum Rules framework using the same symmetric axial-vector⊗axial-vector interpolating current. The current-specific OPE sectors retained through dimension seven within the stated background-field truncation are evaluated with a common symbolic construction, with the bottom channel obtained by the heavy-flavour replacement c→ b. The same pole-dominance and OPE-convergence criteria are imposed in both channels. The adopted charm region is √(s0)=5.7GeV with 3.6≤ MB2≤4.3GeVsq, whereas the bottom region is √(s0)=14.3GeV with 9.8≤ MB2≤10.8GeVsq. At representative Borel points, the extracted masses are 5.239GeV and 13.832GeV, respectively. After the QCD-input, continuum-threshold, and Borel-window variations are combined, the final results are mccc̅s̅, 2+=5.239±0.061GeV and mbbb̅s̅, 2+=13.832±0.059GeV.
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BibTeX
@misc{akan2026spin2,
title = {{Spin-2 $QQ\bar Q\bar s$ Tetraquarks in QCD Sum Rules}},
author = {Tarik Akan},
howpublished = {arXiv},
year = {2026},
month = sep,
doi = {10.48550/arxiv.2609.36925},
eprint = {2609.36925},
archivePrefix = {arXiv},
url = {https://arxiv.org/abs/2609.36925},
note = {CC BY 4.0},
}
RIS
TY - UNPB
TI - Spin-2 QQQ̅s̅ Tetraquarks in QCD Sum Rules
AU - Tarik Akan
PY - 2026
DA - 2026/09/29
PB - arXiv
DO - 10.48550/arxiv.2609.36925
UR - https://arxiv.org/abs/2609.36925
AB - The J^P=2^+ ccc̅s̅ and bbb̅s̅ tetraquarks are studied in parallel within the two-point QCD Sum Rules framework using the same symmetric axial-vector⊗axial-vector interpolating current. The current-specific OPE sectors retained through dimension seven within the stated background-field truncation are evaluated with a common symbolic construction, with the bottom channel obtained by the heavy-flavour replacement c→ b. The same pole-dominance and OPE-convergence criteria are imposed in both channels. The adopted charm region is √(s_0)=5.7GeV with 3.6≤ M_B^2≤4.3GeVsq, whereas the bottom region is √(s_0)=14.3GeV with 9.8≤ M_B^2≤10.8GeVsq. At representative Borel points, the extracted masses are 5.239GeV and 13.832GeV, respectively. After the QCD-input, continuum-threshold, and Borel-window variations are combined, the final results are m_ccc̅s̅, 2^+=5.239±0.061GeV and m_bbb̅s̅, 2^+=13.832±0.059GeV.
ER -