lepton flavor violating decays into axion like particles
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3rd International Conference on Charged Lepton Flavor Violation Lepton-flavor-violating decays into axion-like particles Lorenzo Calibbi (Nankai University) Mainly based on work in progress with D. Redigolo, R. Ziegler, and J. Zupan Kyushu


  1. 3rd International Conference on Charged Lepton Flavor Violation Lepton-flavor-violating decays into axion-like particles Lorenzo Calibbi (Nankai University) Mainly based on work in progress with D. Redigolo, R. Ziegler, and J. Zupan Kyushu University, Fukuoka June 18 th 2019

  2. Motivation Belle/BaBar Mu3e I Mu3e II Definitely worth to keep searching, but… Lorenzo Calibbi (Nankai) LFV into ALPs

  3. Motivation Belle/BaBar Mu3e I Mu3e II What if we haven’t looked (enough) in the right place? Lorenzo Calibbi (Nankai) LFV into ALPs

  4. Introduction Assume there is a light , invisible , new particle “ a” with FV couplings to leptons Light : Invisible : • Neutral m a < m μ , m τ • Feebly coupled (long-lived) CLFV modes would then be μ → e a , τ → μ a , μ → e γ a , etc . Interesting interplay with cosmo/astro: • DM candidate? (if long-lived enough) • Bounds from star cooling/supernovae (if light and feeble enough) Lorenzo Calibbi (Nankai) LFV into ALPs

  5. Lepton-flavor-violating ALPs Why should a be light and feebly-coupled? That’s natural, if it is the (pseudo) Nambu-Goldstone boson (PNGB) of a broken global U(1), aka an axion-like particle (ALP) Examples: Global symmetry: PNGB: • Lepton Number Majoron • Peccei-Quinn Axion Wilczek ‘82 • Flavor symmetry Familon Pilaftsis ‘93 … Feng et al. ‘97 Equivalent possibility: light Z ′ of a local U(1), e.g. L i -L j (with g ≪ 1) Heeck ‘16 Lorenzo Calibbi (Nankai) LFV into ALPs

  6. <latexit sha1_base64="+IolpgmdWYoOPH+Lgq5kmoxRFSI=">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</latexit> Lepton-flavor-violating ALPs Where does lepton flavor violation come from? General couplings to leptons: L a `` = @ µ a C V ij ` i � µ ` j + C A � � ij ` i � µ � 5 ` j 2 f a • If lepton U(1) charges are flavor non-universal naturally flavor-violating couplings • Alternatively, loop-induced flavor-violating couplings Explicit examples at the end of the talk… Lorenzo Calibbi (Nankai) LFV into ALPs

  7. <latexit sha1_base64="+IolpgmdWYoOPH+Lgq5kmoxRFSI=">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</latexit> Lepton-flavor-violating ALPs Where does lepton flavor violation come from? General couplings to leptons: Shift symmetry (PNGB!) → m a from (small) explicit U(1) breaking L a `` = @ µ a C V ij ` i � µ ` j + C A � � ij ` i � µ � 5 ` j 2 f a U(1)-breaking scale → coupling suppression • If lepton U(1) charges are flavor non-universal naturally flavor-violating couplings • Alternatively, loop-induced flavor-violating couplings Explicit examples at the end of the talk… Lorenzo Calibbi (Nankai) LFV into ALPs

  8. <latexit sha1_base64="+IolpgmdWYoOPH+Lgq5kmoxRFSI=">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</latexit> <latexit sha1_base64="UgJGgFEiKJwhr5AYNxEv5pPyXI=">ACKXicbVDLSgMxFM3UV62vqks3wSIQpmpgi6rBXFZwT6g0w6ZNPGZh5NMoWSzu+48VfcKCjq1h8xfSDaeiBwOdcbu5xI0aFNM0PI7W0vLK6l7PbGxube9kd/eqIow5JhUcspDXSQIowGpSCoZqUecIN9lpOb2SmO/NiBc0DC4k8OINH3UCahHMZJacrLFa0fR+8Qm/ZgObI8jrArQc1CibNHnUo1KLVNJplRqwBP4Fi4/BGSxMnmzLw5AVwk1ozkwAxlJ/tit0Mc+ySQmCEhGpYZyaZCXFLMSJKxY0EihHuoQxqaBsgnoqkmlybwSCt6IVcv0DCifp7QiFfiKHv6qSPZFfMe2PxP68RS+iqWgQxZIEeLrIixmUIRzXBtuUEyzZUBOEOdV/hbiLdF1Sl5vRJVjzJy+SaiFvneYLt2e54tWsjQ4AIfgGFjgHBTBDSiDCsDgATyBV/BmPBrPxrvxOY2mjNnMPvgD4+sb5WoOw=</latexit> <latexit sha1_base64="DnXvEscDeIybi8iGp/syNEWX9+Y=">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</latexit> LFV decays into ALPs: model-independent approach L a `` = @ µ a C V ij ` i � µ ` j + C A � � ij ` i � µ � 5 ` j 2 f a This generic Lagrangian induces 2-body LFV decays such as: ! 2 m 3 1 − m 2 1 2 f a ` i a Γ ( ` i → ` j a ) = F ij ≡ q F 2 m 2 16 ⇡ ij | 2 + | C A | C V ij | 2 ij ` i Feng et al. ‘97 Goal: constrain the effective LFV scales F ij using experimental data • Which experiments? • What are the future prospects? Lorenzo Calibbi (Nankai) LFV into ALPs

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