Abstract
The KOTO experiment recently reported four candidate events in the signal region of K_{L}→π^{0}νν[over ¯] search, where the standard model only expects 0.10±0.02 events. If confirmed, this requires physics beyond the standard model to enhance the signal. We examine various new physics interpretations of the result including these: (1)heavy new physics boosting the standard model signal, (2)reinterpretation of "νν[over ¯]" as a new light long-lived particle, or (3)reinterpretation of the whole signal as the production of a new light long-lived particle at the fixed target. We study the above explanations in the context of a generalized new physics Grossman-Nir bound coming from the K^{+}→π^{+}νν[over ¯] decay, bounded by data from the E949 and the NA62 experiments.
Highlights
The KOTO experiment recently reported four candidate events in the signal region of KL → π0ννsearch, where the standard model only expects 0.10 Æ 0.02 events
We examine various new physics interpretations of the result including these: (1) heavy new physics boosting the standard model signal, (2) reinterpretation of “νν” as a new light long-lived particle, or (3) reinterpretation of the whole signal as the production of a new light long-lived particle at the fixed target
We study the above explanations in the context of a generalized new physics Grossman-Nir bound coming from the Kþ → πþννdecay, bounded by data from the E949 and the NA62 experiments
Summary
Teppei Kitahara ,1,2 Takemichi Okui ,3,4 Gilad Perez, Yotam Soreq ,1,6 and Kohsaku Tobioka 3,4. The KOTO experiment recently reported four candidate events in the signal region of KL → π0ννsearch, where the standard model only expects 0.10 Æ 0.02 events. If confirmed, this requires physics beyond the standard model to enhance the signal. Within the SM, these are suppressed by a loop factor, the GIM mechanism [2], and the CKM elements, and predicted to have branching ratios smaller than 10−10 [3,4,5] These processes are being currently probed by the KOTO and the NA62 experiments, both aim to reach the corresponding SM sensitivity. BðKþ → πþννÞNA62 1⁄4 0.47þ−00..4772ð< 2.44Þ × 10−10; ð2Þ at the 68 (95) % CL for two-sided (one-sided) limit, consistent the SM prediction of BðKþ → πþννÞ 1⁄4 ð8.4 Æ 1.0Þ × 10−11
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