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Baryons, skyrmions, and -periodicity anomaly in chiral and vectorlike gauge theories
Phys. Rev. D 113, 105005 – Published 11 May, 2026
DOI: https://doi.org/10.1103/brm8-v5cc
Abstract
In this paper, we study the baryons and solitons of chiral and vectorlike gauge theories with matter in mixed one- and two-index representations. Focusing on the color-flavor locked (CFL) phase, we compute the topology of the coset of their low-energy effective field theory (EFT). We find that in the chiral models under consideration, skyrmions are always absent. We also show, however, that some of these models admit heavy baryons that are expected to be stable, because their decay into the lighter degrees of freedom of the EFT is forbidden by the unbroken symmetry group. This mismatch suggests that some deeper dynamical mechanism must be responsible with either the instability of the seemingly stable heavy baryons or the unreliability of the Skyrme model in the low-energy EFT. In the vectorlike models all the expected baryons are mirrored by skyrmions. Then we turn to the study of domain walls. We determine some aspects of their dynamics by matching the -periodicity anomaly. We find that, for complete CFL, the -periodicity anomaly is always matched without introducing new dynamical degrees of freedom in the low-energy EFT. If part of the color group is unbroken, new dynamical degrees of freedom must be added to the low-energy EFT in the domain-wall background with few exceptions.
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References (67)
- S. Bolognesi, K. Konishi, and A. Luzio, J. High Energy Phys. 09 (2020) 001.
- S. Bolognesi, K. Konishi, and A. Luzio, Phys. Rev. D 103, 094016 (2021).
Being the quark bilinear charged both under color and flavor symmetries, its condensation breaks the two groups into a diagonal subgroup. Such a mechanism is known as color-flavor locking.
- S. Bolognesi, K. Konishi, A. Luzio, and M. Orso, Phys. Rev. D 110, 114037 (2024).
The hadronic spectrum in chiral gauge theories has recently been considered in [6, 7].
- A. H. Kristensen and T. A. Ryttov, Phys. Rev. D 110, 014012 (2024).
- S. Girmohanta, T. A. Ryttov, and R. Shrock, Phys. Rev. D 99, 116022 (2019).
- T. H. R. Skyrme, Nucl. Phys. 31, 556 (1962).
- E. Witten, Nucl. Phys. B160, 57 (1979).
- G. S. Adkins, C. R. Nappi, and E. Witten, Nucl. Phys. B228, 552 (1983).
- S. Bolognesi, Phys. Rev. D 75, 065030 (2007).
- A. Cherman and T. D. Cohen, J. High Energy Phys. 12 (2006) 035.
- Z. Komargodski, arXiv:1812.09253.
- F. Bigazzi, A. L. Cotrone, and A. Olzi, J. High Energy Phys. 02 (2023) 194.
- A. Karasik, Symmetry 14, 2347 (2022).
- F. Lin and Y.-L. Ma, J. High Energy Phys. 05 (2024) 270.
Such a TQFT provides degrees of freedom to the edge of the disk.
- C. Córdova, D. S. Freed, H. T. Lam, and N. Seiberg, SciPost Phys. 8, 001 (2020).
- C. Córdova, D. S. Freed, H. T. Lam, and N. Seiberg, SciPost Phys. 8, 002 (2020).
- M. M. Anber and E. Poppitz, J. High Energy Phys. 11 (2019) 063.
- R. Kitano and R. Matsudo, J. High Energy Phys. 03 (2021) 023.
- J. Frohlich, G. Morchio, and F. Strocchi, Phys. Lett. 97B, 249 (1980).
- J. Frohlich, G. Morchio, and F. Strocchi, Nucl. Phys. B190, 553 (1981).
- S. Elitzur, Phys. Rev. D 12, 3978 (1975).
- S. R. Coleman, J. Wess, and B. Zumino, Phys. Rev. 177, 2239 (1969).
- C. G. Callan, Jr., S. R. Coleman, J. Wess, and B. Zumino, Phys. Rev. 177, 2247 (1969).
- S. Weinberg, Phys. Rev. D 13, 974 (1976); 19, 1277(A) (1979).
- H. Leutwyler, Ann. Phys. (N.Y.) 235, 165 (1994).
A familiar setting where there is continuity between the CFL regime and a strongly coupled regime is finite density QCD with three flavors. In that case, depending on the chemical potential, it is more convenient to use the CFL description [30] or a chiral Lagrangian description. However, the two regimes are believed to be connected, and the qualitative features match [31].
- M. G. Alford, K. Rajagopal, and F. Wilczek, Nucl. Phys. B537, 443 (1999).
- T. Schäfer and F. Wilczek, Phys. Rev. Lett. 82, 3956 (1999).
In the notation of Sec. pp1-s2, corresponds to the , collectively and corresponds to the and collectively.
- K. Yonekura, J. High Energy Phys. 03 (2021) 057.
- R. Brower, S. Chandrasekharan, J. W. Negele, and U. J. Wiese, Phys. Lett. B 560, 64 (2003).
- S. Aoki, H. Fukaya, S. Hashimoto, and T. Onogi, Phys. Rev. D 76, 054508 (2007).
- S. Bolognesi, K. Konishi, and A. Luzio, J. High Energy Phys. 08 (2023) 125.
To prove this point, it is necessary to consider the entire global structure of the symmetry group. In other words, to correctly background gauge the symmetry.
This is one of the simplest realizations of the NAM paradigm [4].
The two-dimensional -tensor acting on spinor indices is defined through the conventions .
- S. Weinberg and E. Witten, Phys. Lett. 96B, 59 (1980).
Which cannot be weakly coupled, as shown in [42] using exact functional RG methods.
- H.-L. Li, Á. Pastor-Gutiérrez, S. Vatani, and L.-X. Xu, J. High Energy Phys. 12 (2025) 020.
It is cumbersome to write the global form of the faithful symmetry group for such models [2].
- S. Bolognesi, K. Konishi, and A. Luzio, J. High Energy Phys. 08 (2021) 028.
- C. Vafa and E. Witten, Phys. Rev. Lett. 53, 535 (1984).
- A. Armoni, G. Shore, and G. Veneziano, Nucl. Phys. B740, 23 (2006).
With and , the main purpose of [46, 48] was to have a large planar equivalence of multiflavor QCD with supersymmetric YM.
- A. Armoni, M. Shifman, G. Shore, and G. Veneziano, Phys. Lett. B 741, 184 (2015).
- T. H. R. Skyrme, Proc. R. Soc. A 260, 127 (1961).
- E. Witten, Nucl. Phys. B223, 422 (1983).
- J. Goldstone and F. Wilczek, Phys. Rev. Lett. 47, 986 (1981).
- M. M. Anber and E. Poppitz, J. High Energy Phys. 04 (2020) 097.
- T. Nakajima, T. Sakai, and R. Yokokura, J. High Energy Phys. 01 (2023) 175.
In the notation of Sec. pp1-s2, corresponds to the , collectively and corresponds to the and collectively.
This is true also in the chiral gauge theories of Sec. 3 where the number of flavors is constrained to grow linearly with and the limit is a Veneziano limit. The key observation is that in all these cases the -matrix becomes trivial when .
- G. R. Dvali and M. A. Shifman, Phys. Lett. B 396, 64 (1997); 407, 452(E) (1997).
- G. Gabadadze and M. A. Shifman, Phys. Rev. D 61, 075014 (2000).
- E. Witten, Nucl. Phys. B507, 658 (1997).
- A. Armoni and T. J. Hollowood, J. High Energy Phys. 07 (2005) 043.
- A. Armoni and M. Shifman, Nucl. Phys. B664, 233 (2003).
- J. Preskill and A. Vilenkin, Phys. Rev. D 47, 2324 (1993).
- M. Eto, Y. Hirono, and M. Nitta, Prog. Theor. Exp. Phys. 2014, 33B01 (2014).
- M. Eto and M. Nitta, J. High Energy Phys. 09 (2022) 077.
- P.-S. Hsin and N. Seiberg, J. High Energy Phys. 09 (2016) 095.
The check is not rigorous because it is not possible to determine if such solitons are solutions of finite energy, and within the regime of validity of the IR EFT.
- A. Hatcher, Algebraic Topology (Cambridge University Press, Cambridge, England, 2002), pp. xii+544.
- N. E. Steenrod, The Topology of Fibre Bundles (Princeton University Press, 1951).