期刊
JOURNAL OF HIGH ENERGY PHYSICS
卷 -, 期 4, 页码 -出版社
SPRINGER
DOI: 10.1007/JHEP04(2021)113
关键词
Lattice QCD; Kaon Physics
资金
- UK Research and Innovation Future Leader Fellowship [MR/T019956/1]
- European projects [H2020-MSCA-ITN2019//860881-HIDDeN]
- Spanish project [FPA2017-85985-P]
- Generalitat Valenciana [PROMETEO/2019/083]
- European Union Horizon 2020 research and innovation program under the Marie Sklodowska-Curie grant [713673]
- La Caixa Foundation [100010434, LCF/BQ/IN17/11620044]
- Generalitat Valenciana through the plan GenT program [CIDEGENT/2019/040]
- United States Department of Energy (USDOE) [DE-SC0011637]
- UKRI [MR/T019956/1] Funding Source: UKRI
This paper discusses the relations between finite-volume matrix elements and infinite-volume decay amplitudes for processes with three spinless, degenerate particles, providing a strategy for extracting three-hadron decay amplitudes using lattice QCD. It is pointed out that solving integral equations is necessary to obtain the physical decay amplitude due to nontrivial finite-state interactions. The article derives results in a simplified theory with three identical particles and presents generalizations needed to study phenomenologically relevant three-pion decays.
We derive relations between finite-volume matrix elements and infinite-volume decay amplitudes, for processes with three spinless, degenerate and either identical or non-identical particles in the final state. This generalizes the Lellouch-Luscher relation for two-particle decays and provides a strategy for extracting three-hadron decay amplitudes using lattice QCD. Unlike for two particles, even in the simplest approximation, one must solve integral equations to obtain the physical decay amplitude, a consequence of the nontrivial finite-state interactions. We first derive the result in a simplified theory with three identical particles, and then present the generalizations needed to study phenomenologically relevant three-pion decays. The specific processes we discuss are the CP-violating K -> 3 pi weak decay, the isospin-breaking eta -> 3 pi QCD transition, and the electromagnetic gamma (*) -> 3 pi amplitudes that enter the calculation of the hadronic vacuum polarization contribution to muonic g - 2.
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