{"title":"KOTO实验中碘化铯量热计的改进","authors":"N. Shimizu","doi":"10.7566/jpscp.27.011004","DOIUrl":null,"url":null,"abstract":"The KOTO experiment, conducted at J-PARC (Ibaraki Japan), is set to observe the rare decay KL → πνν̄. The branching ratio is heavily suppressed in the Standard model (SM) and the experimental observation may reveal hints from physics beyond the SM. The observed signature ofKL → πνν̄ is two γ’s produced from a π and no other signal. Thus the KOTO detector consists of an electromagnetic calorimeter and hermetic veto counters.","PeriodicalId":228570,"journal":{"name":"Proceedings of the 5th International Workshop on New Photon-Detectors (PD18)","volume":"12 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"2019-11-14","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Upgrade of the Cesium Iodide Calorimeter for the KOTO Experiment\",\"authors\":\"N. Shimizu\",\"doi\":\"10.7566/jpscp.27.011004\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"The KOTO experiment, conducted at J-PARC (Ibaraki Japan), is set to observe the rare decay KL → πνν̄. The branching ratio is heavily suppressed in the Standard model (SM) and the experimental observation may reveal hints from physics beyond the SM. The observed signature ofKL → πνν̄ is two γ’s produced from a π and no other signal. Thus the KOTO detector consists of an electromagnetic calorimeter and hermetic veto counters.\",\"PeriodicalId\":228570,\"journal\":{\"name\":\"Proceedings of the 5th International Workshop on New Photon-Detectors (PD18)\",\"volume\":\"12 1\",\"pages\":\"0\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2019-11-14\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"0\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"Proceedings of the 5th International Workshop on New Photon-Detectors (PD18)\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.7566/jpscp.27.011004\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"Proceedings of the 5th International Workshop on New Photon-Detectors (PD18)","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.7566/jpscp.27.011004","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
Upgrade of the Cesium Iodide Calorimeter for the KOTO Experiment
The KOTO experiment, conducted at J-PARC (Ibaraki Japan), is set to observe the rare decay KL → πνν̄. The branching ratio is heavily suppressed in the Standard model (SM) and the experimental observation may reveal hints from physics beyond the SM. The observed signature ofKL → πνν̄ is two γ’s produced from a π and no other signal. Thus the KOTO detector consists of an electromagnetic calorimeter and hermetic veto counters.