{"title":"具有M\\ \\ obius畴壁夸克的Nf=3 QCD中的D介子半光子形状因子","authors":"T. Kaneko, B. Colquhoun, H. Fukaya, S. Hashimoto","doi":"10.1051/epjconf/201817513007","DOIUrl":null,"url":null,"abstract":"We present our calculation of D \\to pi and D \\to K semileptonic form factors in Nf = 2+1 lattice QCD. We simulate three lattice cutoffs 1/a \\sim 2.5, 3.6 and 4.5 GeV with pion masses as low as 230 MeV. The M\\\"obius domain-wall action is employed for both light and charm quarks. We present our results for the vector and scalar form factors and discuss their dependence on the lattice spacing, light quark masses and momentum transfer.","PeriodicalId":8440,"journal":{"name":"arXiv: High Energy Physics - Lattice","volume":"27 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2017-11-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"13","resultStr":"{\"title\":\"D meson semileptonic form factors in Nf=3 QCD with M\\\\\\\"obius domain-wall quarks\",\"authors\":\"T. Kaneko, B. Colquhoun, H. Fukaya, S. Hashimoto\",\"doi\":\"10.1051/epjconf/201817513007\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We present our calculation of D \\\\to pi and D \\\\to K semileptonic form factors in Nf = 2+1 lattice QCD. We simulate three lattice cutoffs 1/a \\\\sim 2.5, 3.6 and 4.5 GeV with pion masses as low as 230 MeV. The M\\\\\\\"obius domain-wall action is employed for both light and charm quarks. We present our results for the vector and scalar form factors and discuss their dependence on the lattice spacing, light quark masses and momentum transfer.\",\"PeriodicalId\":8440,\"journal\":{\"name\":\"arXiv: High Energy Physics - Lattice\",\"volume\":\"27 1\",\"pages\":\"\"},\"PeriodicalIF\":0.0000,\"publicationDate\":\"2017-11-30\",\"publicationTypes\":\"Journal Article\",\"fieldsOfStudy\":null,\"isOpenAccess\":false,\"openAccessPdf\":\"\",\"citationCount\":\"13\",\"resultStr\":null,\"platform\":\"Semanticscholar\",\"paperid\":null,\"PeriodicalName\":\"arXiv: High Energy Physics - Lattice\",\"FirstCategoryId\":\"1085\",\"ListUrlMain\":\"https://doi.org/10.1051/epjconf/201817513007\",\"RegionNum\":0,\"RegionCategory\":null,\"ArticlePicture\":[],\"TitleCN\":null,\"AbstractTextCN\":null,\"PMCID\":null,\"EPubDate\":\"\",\"PubModel\":\"\",\"JCR\":\"\",\"JCRName\":\"\",\"Score\":null,\"Total\":0}","platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv: High Energy Physics - Lattice","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/10.1051/epjconf/201817513007","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
D meson semileptonic form factors in Nf=3 QCD with M\"obius domain-wall quarks
We present our calculation of D \to pi and D \to K semileptonic form factors in Nf = 2+1 lattice QCD. We simulate three lattice cutoffs 1/a \sim 2.5, 3.6 and 4.5 GeV with pion masses as low as 230 MeV. The M\"obius domain-wall action is employed for both light and charm quarks. We present our results for the vector and scalar form factors and discuss their dependence on the lattice spacing, light quark masses and momentum transfer.