- Letter
- Open Access
Constructing on-shell operator basis for all masses and spins
Phys. Rev. D 107, L111901 – Published 27 June, 2023
DOI: https://doi.org/10.1103/PhysRevD.107.L111901
Abstract
We propose a theory to systematically construct a complete set of on-shell effective operator bases involving massive particles with any spins. The amplitude bases involving massive fields can be factorized into two charged and neutral parts under the little groups of massive particles, respectively. The complete bases of these two parts can be constructed by the Young diagrams of Lorentz subgroup and global symmetry ( is the number of external particles), respectively, without any redundancies. The corresponding effective field theory bases with the lowest dimension can be obtained by eliminating the linear correlation bases from a complete but redundant set of bases with all possible polarization tensors. Based on this theory, the amplitude bases involving identical particles can be constructed by a matrix projection method. A generic massive effective field theory can thus be constructed automatically by computer programs.
Physics Subject Headings (PhySH)
Article Text
Supplemental Material
References (41)
- K. G. Wilson, Phys. Rev. D 3, 1818 (1971).
- G. ’t Hooft, NATO Sci. Ser. B 59, 135 (1980).
- F. Zwicky, Helv. Phys. Acta 6, 110 (1933).
- V. C. Rubin and W. K. Ford, Jr., Astrophys. J. 159, 379 (1970).
- R. Davis, Jr., D. S. Harmer, and K. C. Hoffman, Phys. Rev. Lett. 20, 1205 (1968).
- B. Pontecorvo, Zh. Eksp. Teor. Fiz. 33, 549 (1957) [Sov. Phys. JETP 6, 429 (1957)].
- Z. Bern, J. Parra-Martinez, and E. Sawyer, J. High Energy Phys. 10 (2020) 211.
- M. Jiang, T. Ma, and J. Shu, J. High Energy Phys. 01 (2021) 101.
- J. Elias Miró, J. Ingoldby, and M. Riembau, J. High Energy Phys. 09 (2020) 163.
- P. Baratella, C. Fernandez, and A. Pomarol, Nucl. Phys. B959, 115155 (2020).
- C. Cheung, K. Kampf, J. Novotny, and J. Trnka, Phys. Rev. Lett. 114, 221602 (2015).
- C. Cheung, K. Kampf, J. Novotny, C. H. Shen, and J. Trnka, J. High Energy Phys. 02 (2017) 020.
- I. Low, Phys. Rev. D 91, 105017 (2015).
- I. Low, Phys. Rev. D 91, 116005 (2015).
- H. Elvang, D. Z. Freedman, and M. Kiermaier, J. High Energy Phys. 11 (2010) 016.
- Y. Shadmi and Y. Weiss, J. High Energy Phys. 02 (2019) 165.
- T. Ma, J. Shu, and M. L. Xiao, Chin. Phys. C 47, 023105 (2023).
- H. L. Li, Z. Ren, J. Shu, M. L. Xiao, J. H. Yu, and Y. H. Zheng, Phys. Rev. D 104, 015026 (2021).
- B. Henning and T. Melia, Phys. Rev. D 100, 016015 (2019).
- A. Falkowski and R. Rattazzi, J. High Energy Phys. 10 (2019) 255.
- T. Cohen, N. Craig, X. Lu, and D. Sutherland, J. High Energy Phys. 03 (2021) 237.
- J. Goodman, M. Ibe, A. Rajaraman, W. Shepherd, T. M. P. Tait, and H. B. Yu, Phys. Rev. D 82, 116010 (2010).
- Q. H. Cao, C. R. Chen, C. S. Li, and H. Zhang, J. High Energy Phys. 08 (2011) 018.
- J. M. Zheng, Z. H. Yu, J. W. Shao, X. J. Bi, Z. Li, and H. H. Zhang, Nucl. Phys. B854, 350 (2012).
- J. Aebischer, W. Altmannshofer, E. E. Jenkins, and A. V. Manohar, J. High Energy Phys. 06 (2022) 086.
- E. Del Nobile and F. Sannino, Int. J. Mod. Phys. A 27, 1250065 (2012).
- B. Bellazzini, F. Riva, J. Serra, and F. Sgarlata, J. High Energy Phys. 10 (2019) 189.
- A. Falkowski, G. Isabella, and C. S. Machado, SciPost Phys. 10, 101 (2021).
- G. Durieux, T. Kitahara, C. S. Machado, Y. Shadmi, and Y. Weiss, J. High Energy Phys. 12 (2020) 175.
- H. L. Li, Z. Ren, M. L. Xiao, J. H. Yu, and Y. H. Zheng, J. High Energy Phys. 11 (2021) 003.
- Z. Y. Dong, T. Ma, J. Shu, and Y. H. Zheng, Phys. Rev. D 106, 116010 (2022).
- E. Witten, Commun. Math. Phys. 252, 189 (2004).
- N. Arkani-Hamed, T. C. Huang, and Y. t. Huang, J. High Energy Phys. 11 (2021) 070.
In this work we follow the following convention for filling YD: , so the higher spin particle should be labeled by a larger number (in this example, we label the spinors of by the largest number among the four legs).
- See Supplemental Materials at http://link.aps.org/supplemental/10.1103/PhysRevD.107.L111901 for rigorous proof of amplitude basis independence and an example for constructing bases.
The MLGNS bases of should contain at least four massive right-handed spinors to contract the bare indices of and four massive left-handed spinors to be massive LG neutral. So the lowest dimension of the bases with should be .
- B. Feng, A. Hanany, and Y. H. He, J. High Energy Phys. 03 (2007) 090.
- R. M. Fonseca, Phys. Rev. D 101, 035040 (2020).
Reference [40] uses a graphic method to construct the massive amplitude bases.
- S. De Angelis, J. High Energy Phys. 08 (2022) 299.
- Z. Y. Dong, T. Ma, J. Shu, and Z. Z. Zhou, arXiv:2211.16515.