In this work we study the weak decays of $$\Xi _{cc}\rightarrow \Xi _c$$ and $$\Xi _{cc}\rightarrow \Xi '_c$$ in the light-front quark model. Generally, a naive, but reasonable conjecture suggests that the cc subsystem in $$\Xi _{cc}$$ ( us pair in $$\Xi ^{(')}_c$$ ) stands as a diquark with definite spin and color assignments. During the concerned processes, the diquark of the initial state is not a spectator, namely must be broken. A Racah transformation would decompose the original (cc)q into a combination of c(cq) components. Thus we may deal with the decaying c quark alone while keeping the (cq) subsystem as a spectator. With the re-arrangement of the inner structure we calculate the form factors numerically and then obtain the rates of semi-leptonic decays and non-leptonic decays, which will be measured in the future.
{ "_oai": { "updated": "2020-11-11T09:59:16Z", "id": "oai:repo.scoap3.org:52761", "sets": [ "EPJC" ] }, "authors": [ { "affiliations": [ { "country": "China", "value": "School of Science, Tianjin University, Tianjin, 300072, China", "organization": "Tianjin University" } ], "surname": "Ke", "email": "khw020056@tju.edu.cn", "full_name": "Ke, Hong-Wei", "given_names": "Hong-Wei" }, { "affiliations": [ { "country": "China", "value": "School of Science, Tianjin University, Tianjin, 300072, China", "organization": "Tianjin University" } ], "surname": "Lu", "given_names": "Fang", "full_name": "Lu, Fang" }, { "affiliations": [ { "country": "China", "value": "School of Science, Tianjin University, Tianjin, 300072, China", "organization": "Tianjin University" } ], "surname": "Liu", "email": "xiaohai.liu@tju.edu.cn", "full_name": "Liu, Xiao-Hai", "given_names": "Xiao-Hai" }, { "affiliations": [ { "country": "China", "value": "School of Physics, Nankai University, Tianjin, 300071, China", "organization": "Nankai University" } ], "surname": "Li", "email": "lixq@nankai.edu.cn", "full_name": "Li, Xue-Qian", "given_names": "Xue-Qian" } ], "titles": [ { "source": "Springer", "title": "Study on $$\\Xi _{cc}\\rightarrow \\Xi _c$$ <math><mrow><msub><mi>\u039e</mi><mrow><mi>cc</mi></mrow></msub><mo>\u2192</mo><msub><mi>\u039e</mi><mi>c</mi></msub></mrow></math> and $$\\Xi _{cc}\\rightarrow \\Xi '_c$$ <math><mrow><msub><mi>\u039e</mi><mrow><mi>cc</mi></mrow></msub><mo>\u2192</mo><msubsup><mi>\u039e</mi><mi>c</mi><mo>\u2032</mo></msubsup></mrow></math> weak decays in the light-front quark model" } ], "dois": [ { "value": "10.1140/epjc/s10052-020-7699-y" } ], "publication_info": [ { "page_end": "11", "journal_title": "European Physical Journal C", "material": "article", "journal_volume": "80", "artid": "s10052-020-7699-y", "year": 2020, "page_start": "1", "journal_issue": "2" } ], "$schema": "http://repo.scoap3.org/schemas/hep.json", "acquisition_source": { "date": "2020-11-11T10:30:56.472212", "source": "Springer", "method": "Springer", "submission_number": "784d5db2240011ebbd0e02163e01809a" }, "page_nr": [ 11 ], "license": [ { "url": "https://creativecommons.org/licenses//by/4.0", "license": "CC-BY-4.0" } ], "copyright": [ { "holder": "The Author(s)", "year": "2020" } ], "control_number": "52761", "record_creation_date": "2020-02-17T16:30:29.779532", "_files": [ { "checksum": "md5:d01ee947cd5ad6dba81920abc2165598", "filetype": "xml", "bucket": "0881a92e-2d58-487e-a8ac-60146584aa00", "version_id": "3da09f85-a937-4102-ab0a-5645045a44ff", "key": "10.1140/epjc/s10052-020-7699-y.xml", "size": 17749 }, { "checksum": "md5:a4d0d10c421f09bcc0838fe0f523dbf5", "filetype": "pdf/a", "bucket": "0881a92e-2d58-487e-a8ac-60146584aa00", "version_id": "8ff75d26-f8af-4194-8129-c461fbc8f7b0", "key": "10.1140/epjc/s10052-020-7699-y_a.pdf", "size": 539327 } ], "collections": [ { "primary": "European Physical Journal C" } ], "abstracts": [ { "source": "Springer", "value": "In this work we study the weak decays of $$\\Xi _{cc}\\rightarrow \\Xi _c$$ <math><mrow><msub><mi>\u039e</mi><mrow><mi>cc</mi></mrow></msub><mo>\u2192</mo><msub><mi>\u039e</mi><mi>c</mi></msub></mrow></math> and $$\\Xi _{cc}\\rightarrow \\Xi '_c$$ <math><mrow><msub><mi>\u039e</mi><mrow><mi>cc</mi></mrow></msub><mo>\u2192</mo><msubsup><mi>\u039e</mi><mi>c</mi><mo>\u2032</mo></msubsup></mrow></math> in the light-front quark model. Generally, a naive, but reasonable conjecture suggests that the cc subsystem in $$\\Xi _{cc}$$ <math><msub><mi>\u039e</mi><mrow><mi>cc</mi></mrow></msub></math> ( us pair in $$\\Xi ^{(')}_c$$ <math><msubsup><mi>\u039e</mi><mi>c</mi><mrow><msup><mo>(</mo><mo>\u2032</mo></msup><mo>)</mo></mrow></msubsup></math> ) stands as a diquark with definite spin and color assignments. During the concerned processes, the diquark of the initial state is not a spectator, namely must be broken. A Racah transformation would decompose the original (cc)q into a combination of c(cq) components. Thus we may deal with the decaying c quark alone while keeping the (cq) subsystem as a spectator. With the re-arrangement of the inner structure we calculate the form factors numerically and then obtain the rates of semi-leptonic decays and non-leptonic decays, which will be measured in the future." } ], "imprints": [ { "date": "2020-02-17", "publisher": "Springer" } ] }