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Objective frequency-specific hearing thresholds definition for medicolegal purposes in case of occupational NIHL: ASSR outperforms CERA 被引量:2
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作者 P.H.DeJonckere B.Millet +2 位作者 R.Van Gool a.martens J.Lebacq 《Journal of Otology》 CSCD 2021年第4期210-219,共10页
Audiological use of the 40 Hz-ASSR (auditory steady state responses) could be valuable for objectivelyestimating the frequency-specific threshold in adults undergoing an expertise examination for medicolegal and/or co... Audiological use of the 40 Hz-ASSR (auditory steady state responses) could be valuable for objectivelyestimating the frequency-specific threshold in adults undergoing an expertise examination for medicolegal and/or compensation purposes. The present prospective study was set up to clarify the relationship between the thresholds obtained by cortical evoked response audiometry (CERA) and by 40 HzASSR, in the same ears, within a large homogeneous sample of 164 subjects (328 ears) with NIHL andwell documented exposure to noise. All these subjects claimed financial compensation for occupationalNIHL, and there was a suspicion of exaggeration of the reported NIHLs. ASSR thresholds show a goodcorrelation with the CERA thresholds. However, a systematic shift is noticed, ASSR thresholds being onaverage (1e2 e 3 kHz) 4.38 dB lower (i.e. showing less hearing loss) than CERA thresholds. Moreover, thebinaural multiple ASSR technique allows a considerable time gain when compared to the CERA. 展开更多
关键词 Objective audiometry CERA ASSR NIHL MEDICOLEGAL
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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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