- Open Access
violation in decays: A comparative analysis of triplet and sextet diquarks
Phys. Rev. D 114, 035037 – Published 28 August, 2026
DOI: https://doi.org/10.1103/zjgc-l23x
Abstract
Recent measurements of the charge-parity asymmetry in the decay by CMS Collaboration, , and by LHCb, , suggest possible deviations from Standard Model expectations, which predict asymmetries below the percent level. This singly Cabibbo-suppressed decay is particularly sensitive to new physics, as the leading amplitudes vanish in the exact U-spin symmetry limit and the process is dominated by W-exchange topologies. We investigate scalar diquark contributions to this decay, comparing color-sextet and color-triplet representations. We find that the color-sextet diquark, characterized by a symmetric color structure , avoids color suppression and can generate asymmetries in the range 0.5%–1.5% for a diquark mass of order 1 TeV. In contrast, the color-triplet contribution is strongly suppressed due to destructive interference from its antisymmetric color structure. We further show that a flavor hierarchy in the sextet couplings, with , can simultaneously account for the observed deviation from the U-spin sum rule in and and the measured asymmetry in . These results identify color-sextet scalar diquarks as viable candidates for explaining enhanced violation in charm decays.
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References (41)
- R. Aaij et al. (LHCb Collaboration), J. High Energy Phys. 02 (2026) 253.
- R. Aaij et al. (LHCb Collaboration), Phys. Rev. Lett. 122, 211803 (2019).
- A. Hayrapetyan et al. (CMS Collaboration), Eur. Phys. J. C 84, 1264 (2024).
- U. Nierste and S. Schacht, Phys. Rev. D 92, 054036 (2015).
- Y. Grossman, A. L. Kagan, and Y. Nir, Phys. Rev. D 75, 036008 (2007).
- H.-Y. Cheng and C.-W. Chiang, Phys. Rev. D 85, 034036 (2012).
- R. Aaij et al. (LHCb Collaboration), Phys. Rev. Lett. 122, 211803 (2019).
- R. Aaij et al. (LHCb Collaboration), Phys. Rev. Lett. 131, 091802 (2023).
- R. Aaij et al. (LHCb Collaboration), Phys. Rev. D 104, 072010 (2021).
- C.-H. Chen, C.-Q. Geng, and W. Wang, Phys. Rev. D 85, 077702 (2012).
- J. Brod, A. L. Kagan, and J. Zupan, J. High Energy Phys. 10 (2012) 161.
While the physical decay involves strange () and down () quarks, theorists use the -quark operator as a reference point to isolate the flavor-symmetric part of the exchange diagram [4].
- G. F. Giudice, B. Gripaios, and R. Sundrum, J. High Energy Phys. 08 (2011) 055.
- E. Golowich, J. Hewett, S. Pakvasa, and A. A. Petrov, Phys. Rev. D 76, 095009 (2007).
- I. Doršner, S. Fajfer, A. Greljo, J. Kamenik, and N. Košnik, Phys. Rep. 641, 1–68 (2016).
- T. Feldmann, S. Nandi, and A. Soni, J. High Energy Phys. 06 (2012) 007.
- M. Gronau, Phys. Lett. B 730, 221 (2014).
- G. Hiller, M. Jung, and S. Schacht, Phys. Rev. D 87, 014024 (2013).
- R. Aaij, A. S. W. Abdelmotteleb et al. (The LHCb Collaboration), J. High Energy Phys. 02 (2026) 253.
- S. Fajfer, J. F. Kamenik, and I. Nišandžić, Phys. Rev. D 85, 094025 (2012).
- U. Nierste and S. Schacht, Phys. Rev. D 92, 054036 (2015).
- A. F. Falk, A. L. Kagan, Y. Nir, and G. Perez, Phys. Rev. D 65, 054034 (2002).
- T. Inami and C. S. Lim, Prog. Theor. Phys. 65, 297 (1981); 65, 1772(E) (1981).
- Y. Aoki et al. (Flavour Lattice Averaging Group (FLAG) Collaboration), Eur. Phys. J. C 82, 869 (2022).
- Y. S. Amhis et al. (HFLAV Collaboration), Phys. Rev. D 107, 052008 (2023).
- A. J. Buras and E. Venturini, Acta Phys. Pol. B 53, 6-A1 (2021).
- G. Buchalla, A. J. Buras, and M. E. Lautenbacher, Rev. Mod. Phys. 68, 1125 (1996).
- M. Ablikim et al. (BESIII Collaboration), Phys. Rev. D 105, L071102 (2022).
- R. L. Workman et al. (Particle Data Group Collaboration), Prog. Theor. Exp. Phys. 2022, 083C01 (2022).
- M. Kramer, T. Plehn, M. Spira, and P. M. Zerwas, Phys. Rev. D 71, 057503 (2005).
- A. M. Sirunyan et al. (CMS Collaboration), Phys. Rev. D 100, 112007 (2019).
- G. Aad et al. (ATLAS Collaboration), Phys. Rev. D 108, 112005 (2023).
- A. M. Sirunyan et al. (CMS Collaboration), J. High Energy Phys. 08 (2018) 130.
- C. D. Froggatt and H. B. Nielsen, Nucl. Phys. B147, 277 (1979).
- L. E. Ibanez and G. G. Ross, Phys. Lett. B 332, 100 (1994).
- A. J. Buras, M. Misiak, and J. Urban, Nucl. Phys. B586, 397 (2000); B1002, 116529(E) (2024).
- A. J. Buras and J. Girrbach, Acta Phys. Pol. B 43, 1427 (2012).
- I. Adachi et al. (Belle-II Collaboration), Phys. Rev. D 112, L031101 (2025).
- N. K. Nisar et al. (Belle Collaboration), Phys. Rev. Lett. 112, 211601 (2014).
- R. Aaij et al. (LHCb Collaboration), Phys. Rev. D 104, L031102 (2021).
- R. Aaij et al. (LHCb Collaboration), Phys. Rev. Lett. 112, 202001 (2014).