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Measurement of the integrated luminosity of data samples collected during 2019-2022 by the Belle Ⅱ experiment
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作者 I.Adachi L.Aggarwal +407 位作者 H.Ahmed J.K.Ahn H.Aihara N.Akopov A.Aloisio N.Althubiti N.Anh Ky D.M.Asner H.Atmacan T.Aushev V.Aushev M.Aversano R.Ayad V.Babu H.Bae S.Bahinipati P.Bambade Sw.Banerjee M.Barrett J.Baudot A.Baur A.Beaubien F.Becherer J.Becker J.V.Bennett F.U.Bernlochner V.Bertacchi M.Bertemes E.Bertholet M.Bessner S.Bettarini B.Bhuyan F.Bianchi L.Bierwirth T.Bilka D.Biswas A.Bobrov D.Bodrov J.Borah A.Boschetti A.Bozek P.Branchini T.E.Browder A.Budano S.Bussino Q.Campagna M.Campajola L.Cao G.Casarosa C.Cecchi J.Cerasoli M.-C.Chang P.Chang R.Cheaib P.Cheema B.G.Cheon K.Chilikin K.Chirapatpimol H.-E.Cho K.Cho S.-J.Cho S.-K.Choi S.Choudhury J.Cochran L.Corona J.X.Cui S.Das E.De La Cruz-Burelo S.A.De La Motte G.de Marino G.De Nardo G.De Pietro R.de Sangro M.Destefanis S.Dey R.Dhamija A.Di Canto F.Di Capua J.Dingfelder Z.Doležal I.Domínguez Jiménez T.V.Dong K.Dort D.Dossett S.Dubey K.Dugic G.Dujany P.Ecker D.Epifanov J.Eppelt P.Feichtinger T.Ferber T.Fillinger C.Finck G.Finocchiaro A.Fodor F.Forti A.Frey B.G.Fulsom A.Gabrielli E.Ganiev M.Garcia-Hernandez R.Garg G.Gaudino V.Gaur A.Gaz A.Gellrich G.Ghevondyan D.Ghosh H.Ghumaryan G.Giakoustidis R.Giordano A.Giri P.Gironella B.Gobbo R.Godang O.Gogota P.Goldenzweig W.Gradl E.Graziani D.Greenwald Z.Gruberová T.Gu K.Gudkova I.Haide S.Halder Y.Han K.Hara T.Hara C.Harris K.Hayasaka H.Hayashii S.Hazra C.Hearty M.T.Hedges A.Heidelbach I.Heredia de la Cruz M.Hernández Villanueva T.Higuchi M.Hoek M.Hohmann R.Hoppe p.horak C.-L.Hsu T.Humair T.Iijima K.Inami N.Ipsita A.Ishikawa R.Itoh M.Iwasaki W.W.Jacobs D.E.Jaffe E.-J.Jang Q.P.Ji S.Jia Y.Jin A.Johnson K.K.Joo H.Junkerkalefeld M.Kaleta D.Kalita J.Kandra K.H.Kang G.Karyan T.Kawasaki F.Keil C.Kiesling C.-H.Kim D.Y.Kim J.-Y.Kim K.-H.Kim Y.-K.Kim Y.J.Kim H.Kindo K.Kinoshita P.Kodyš T.Koga S.Kohani K.Kojima A.Korobov S.Korpar E.Kovalenko R.Kowalewski P.Križan P.Krokovny T.Kuhr R.Kumar K.Kumara A.Kuzmin Y.-J.Kwon S.Lacaprara Y.-T.Lai K.Lalwani T.Lam L.Lanceri J.S.Lange M.Laurenza K.Lautenbach R.Leboucher M.J.Lee C.Lemettais P.Leo D.Levit P.M.Lewis C.Li L.K.Li S.X.Li W.Z.Li Y.Li Y.B.Li Y.P.Liao J.Libby J.Lin M.H.Liu Q.Y.Liu Z.Q.Liu D.Liventsev S.Longo T.Lueck C.Lyu Y.Ma M.Maggiora S.P.Maharana R.Maiti S.Maity G.Mancinelli R.Manfredi E.Manoni M.Mantovano D.Marcantonio S.Marcello C.Marinas C.Martellini A.Martens A.Martini T.Martinov L.Massaccesi M.Masuda K.Matsuoka D.Matvienko S.K.Maurya J.A.McKenna R.Mehta F.Meier M.Merola C.Miller M.Mirra S.Mitra K.Miyabayashi G.B.Mohanty S.Mondal S.Moneta H.-G.Moser R.Mussa I.Nakamura M.Nakao Y.Nakazawa M.Naruki D.Narwal Z.Natkaniec A.Natochii M.Nayak G.Nazaryan M.Neu C.Niebuhr S.Nishida S.Ogawa Y.Onishchuk H.Ono P.Pakhlov G.Pakhlova E.Paoloni S.Pardi K.Parham H.Park J.Park K.Park S.-H.Park B.Paschen A.Passeri S.Patra T.K.Pedlar R.Peschke R.Pestotnik L.E.Piilonen G.Pinna Angioni P.L.M.Podesta-Lerma T.Podobnik S.Pokharel C.Praz S.Prell E.Prencipe M.T.Prim H.Purwar P.Rados G.Raeuber S.Raiz N.Rauls M.Reif S.Reiter M.Remnev L.Reuter I.Ripp-Baudot G.Rizzo S.H.Robertson M.Roehrken J.M.Roney A.Rostomyan N.Rout S.Sandilya L.Santelj Y.Sato V.Savinov B.Scavino M.Schnepf C.Schwanda A.J.Schwartz Y.Seino A.Selce K.Senyo J.Serrano C.Sfienti W.Shan C.Sharma C.P.Shen X.D.Shi T.Shillington T.Shimasaki J.-G.Shiu D.Shtol B.Shwartz A.Sibidanov F.Simon J.B.Singh J.Skorupa R.J.Sobie M.Sobotzik A.Soffer A.Sokolov E.Solovieva W.Song S.Spataro B.Spruck M.Starič P.Stavroulakis S.Stefkova R.Stroili Y.Sue M.Sumihama K.Sumisawa W.Sutcliffe N.Suwonjandee H.Svidras M.Takahashi M.Takizawa U.Tamponi K.Tanida F.Tenchini A.Thaller O.Tittel R.Tiwary E.Torassa K.Trabelsi I.Ueda K.Unger Y.Unno K.Uno S.Uno P.Urquijo Y.Ushiroda S.E.Vahsen R.van Tonder K.E.Varvell M.Veronesi A.Vinokurova V.S.Vismaya L.Vitale V.Vobbilisetti R.Volpe A.Vossen M.Wakai S.Wallner E.Wang M.-Z.Wang Z.Wang A.Warburton S.Watanuki C.Wessel E.Won X.P.Xu B.D.Yabsley S.Yamada W.Yan S.B.Yang J.Yelton J.H.Yin K.Yoshihara C.Z.Yuan L.Zani B.Zhang V.Zhilich J.S.Zhou Q.D.Zhou X.Y.Zhou V.I.Zhukova R.Zlebcík The Belle Ⅱ Collaboration 《Chinese Physics C》 2025年第1期7-18,共12页
series of data samples was collected with the Belle Ⅱ detector at the SuperKEKB collider from March 2019 to June 2022.We determine the integrated luminosities of these data samples using three distinct methodologies ... series of data samples was collected with the Belle Ⅱ detector at the SuperKEKB collider from March 2019 to June 2022.We determine the integrated luminosities of these data samples using three distinct methodologies involving Bhabha(e^(+)e^(-)→e^(+)e^(-)(ny),digamma(e^(+)e^(-)→γγ(nγ),and dimuon(e^(+)e^(-)→μ^(+)μ^(-)(nγ)events.The total integrated luminosity obtained with Bhabha,digamma,and dimuon events is(426.88±0.03±2.61)fb^(-1),(429.28±0.03±2.62)fb^(-1),and(423.99±0.04±3.83)fb^(-1),where the first uncertainties are statistical and the second are systematic.The resulting total integrated luminosity obtained from the combination of the three methods is(427.87±2.01)fb^(-1). 展开更多
关键词 integrated luminosity Bhabha digamma dimuon BelleⅡ
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Intermodal frequency generation in silicon-rich silicon nitride waveguides 被引量:4
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作者 C.LACAVA T.DOMINGUEZ BUCIO +6 位作者 A.Z.KHOKHAR p.horak Y.JUNG F.Y.GARDES D.J.RICHARDSON P.PETROPOULOS F.PARMIGIANI 《Photonics Research》 SCIE EI CSCD 2019年第6期615-621,共7页
Dispersion engineering in optical waveguides allows applications relying on the precise control of phase matching conditions to be implemented. Although extremely effective over relatively narrow band spectral regions... Dispersion engineering in optical waveguides allows applications relying on the precise control of phase matching conditions to be implemented. Although extremely effective over relatively narrow band spectral regions,dispersion control becomes increasingly challenging as the bandwidth of the process of interest increases.Phase matching can also be achieved by exploiting the propagation characteristics of waves exciting different spatial modes of the same waveguide. Phase matching control in this case relies on achieving very similar propagation characteristics across two, and even more, waveguide modes over the wavelengths of interest, which may be rather far from one another. We demonstrate here that broadband(>40 nm) four-wave mixing can be achieved between pump waves and a signal located in different bands of the communications spectrum(separated by50 nm) by exploiting interband nonlinearities. Our demonstration is carried out in the silicon-rich silicon nitride material platform, which allows flexible device engineering, allowing for strong effective nonlinearity at telecommunications wavelengths without deleterious nonlinear-loss effects. 展开更多
关键词 Intermodal FREQUENCY silicon-rich silicon NITRIDE WAVEGUIDES
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