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| 1 | Methods for a blind analysis of isobar data collected by the STAR collaboration显示文摘In 2018,the STAR collaboration collected data from^(96)_(44)Ru+^(96)_(44)Ru and^(96)_(40)Zr+^(96)_(40)Zr at√^(S)NN=200 Ge V to search for the presence of the chiral magnetic effect in collisions of nuclei.The isobar collision species alternated frequently between 9644 Ru+^(96)_(44)Ru and^(96)_(40)Zr+^(96)_(40)Zr.In order to conduct blind analyses of studies related to the chiral magnetic effect in these isobar data,STAR developed a three-step blind analysis procedure.Analysts are initially provided a'reference sample'of data,comprised of a mix of events from the two species,the order of which respects time-dependent changes in run conditions.After tuning analysis codes and performing time-dependent quality assurance on the reference sample,analysts are provided a species-blind sample suitable for calculating efficiencies and corrections for individual≈30-min data-taking runs.For this sample,species-specific information is disguised,but individual output files contain data from a single isobar species.Only run-by-run corrections and code alteration subsequent to these corrections are allowed at this stage.Following these modifications,the'frozen'code is passed over the fully un-blind data,completing the blind analysis.As a check of the feasibility of the blind analysis procedure,analysts completed a'mock data challenge,'analyzing data from Au+Au collisions at√^(S)NN=27 Ge V,collected in 2018.The Au+Au data were prepared in the same manner intended for the isobar blind data.The details of the blind analysis procedure and results from the mock data challenge are presented. | J.Adam L.Adamczyk J.R.Adams J.K.Adkins G.Agakishiev M.M.Aggarwal Z.Ahammed I.Alekseev D.M.Anderson A.Aparin E.C.Aschenauer M.U.Ashraf F.G.Atetalla A.Attri G.S.Averichev V.Bairathi K.Barish A.Behera R.Bellwied A.Bhasin J.Bielcik J.Bielcikova L.C.Bland I.G.Bordyuzhin J.D.Brandenburg A.V.Brandin J.Butterworth H.Caines M.Calderon de la Barca Sanchez D.Cebra I.Chakaberia P.Chaloupka B.K.Chan F-H.Chang Z.Chang N.Chankova-Bunzarova A.Chatterjee D.Chen J.Chen J.H.Chen X.Chen Z.Chen J.Cheng M.Cherney M.Chevalier S.Choudhury W.Christie X.Chu H.J.Crawford M.Csanad M.Daugherity T.G.Dedovich I.M.Deppner A.A.Derevschikov L.Didenko X.Dong J.L.Drachenberg J.C.Dunlop T.Edmonds N.Elsey J.Engelage G.Eppley S.Esumi O.Evdokimov A.Ewigleben O.Eyser R.Fatemi S.Fazio P.Federic J.Fedorisin C.J.Feng Y.Feng P.Filip E.Finch Y.Fisyak A.Francisco L.Fulek C.A.Gagliardi T.Galatyuk F.Geurts A.Gibson K.Gopal X.Gou D.Grosnick W.Guryn A.I.Hamad A.Hamed S.Harabasz J.W.Harris S.He W.He X.H.He Y.He S.Heppelmann S.Heppelmann N.Herrmann E.Hoffman L.Holub Y.Hong S.Horvat Y.Hu H.Z.Huang S.L.Huang T.Huang X.Huang T.J.Humanic P.Huo G.Igo D.Isenhower W.W.Jacobs C.Jena A.Jentsch Y.Ji J.Jia K.Jiang S.Jowzaee X.Ju E.G.Judd S.Kabana M.L.Kabir S.Kagamaster D.Kalinkin K.Kang D.Kapukchyan K.Kauder H.W.Ke D.Keane A.Kechechyan M.Kelsey Y.V.Khyzhniak D.P.Kikoła C.Kim B.Kimelman D.Kincses T.A.Kinghorn I.Kisel A.Kiselev M.Kocan L.Kochenda L.K.Kosarzewski L.Kramarik P.Kravtsov K.Krueger N.Kulathunga Mudiyanselage L.Kumar S.Kumar R.Kunnawalkam Elayavalli J.H.Kwasizur R.Lacey S.Lan J.M.Landgraf J.Lauret A.Lebedev R.Lednicky J.H.Lee Y.H.Leung C.Li C.Li W.Li W.Li X.Li Y.Li Y.Liang R.Licenik T.Lin Y.Lin M.A.Lisa F.Liu H.Liu P.Liu P.Liu T.Liu X.Liu Y.Liu Z.Liu T.Ljubicic W.J.Llope R.S.Longacre N.S.Lukow S.Luo X.Luo G.L.Ma L.Ma R.Ma Y.G.Ma N.Magdy R.Majka D.Mallick S.Margetis C.Markert H.S.Matis J.A.Mazer N.G.Minaev S.Mioduszewski B.Mohanty I.Mooney Z.Moravcova D.A.Morozov M.Nagy J.D.Nam Md.Nasim K.Nayak D.Neff J.M.Nelson D.B.Nemes M.Nie G.Nigmatkulov T.Niida L.V.Nogach T.Nonaka A.S.Nunes G.Odyniec A.Ogawa S.Oh V.A.Okorokov B.S.Page R.Pak A.Pandav Y.Panebratsev B.Pawlik D.Pawlowska H.Pei C.Perkins L.Pinsky R.L.Pinter J.Pluta J.Porter M.Posik N.K.Pruthi M.Przybycien J.Putschke H.Qiu A.Quintero S.K.Radhakrishnan S.Ramachandran R.L.Ray R.Reed H.G.Ritter O.V.Rogachevskiy J.L.Romero L.Ruan J.Rusnak N.R.Sahoo H.Sako S.Salur J.Sandweiss S.Sato W.B.Schmidke N.Schmitz B.R.Schweid F.Seck J.Seger M.Sergeeva R.Seto P.Seyboth N.Shah E.Shahaliev P.V.Shanmuganathan M.Shao A.I.Sheikh W.Q.Shen S.S.Shi Y.Shi Q.Y.Shou E.P.Sichtermann R.Sikora M.Simko J.Singh S.Singha N.Smirnov W.Solyst P.Sorensen H.M.Spinka B.Srivastava T.D.S.Stanislaus M.Stefaniak D.J.Stewart M.Strikhanov B.Stringfellow A.A.P.Suaide M.Sumbera B.Summa X.M.Sun X.Sun Y.Sun Y.Sun B.Surrow D.N.Svirida P.Szymanski A.H.Tang Z.Tang A.Taranenko T.Tarnowsky J.H.Thomas A.R.Timmins D.Tlusty M.Tokarev C.A.Tomkiel S.Trentalange R.E.Tribble P.Tribedy S.K.Tripathy O.D.Tsai Z.Tu T.Ullrich D.G.Underwood I.Upsal G.Van Buren J.Vanek A.N.Vasiliev I.Vassiliev F.Videbæk S.Vokal S.A.Voloshin F.Wang G.Wang J.S.Wang P.Wang Y.Wang Y.Wang Z.Wang J.C.Webb P.C.Weidenkaff L.Wen G.D.Westfall H.Wieman S.W.Wissink R.Witt Y.Wu Z.G.Xiao G.Xie W.Xie H.Xu N.Xu Q.H.Xu Y.F.Xu Y.Xu Z.Xu Z.Xu C.Yang Q.Yang S.Yang Y.Yang Z.Yang Z.Ye Z.Ye L.Yi K.Yip Y.Yu H.Zbroszczyk W.Zha C.Zhang D.Zhang S.Zhang S.Zhang X.P.Zhang Y.Zhang Y.Zhang Z.J.Zhang Z.Zhang Z.Zhang J.Zhao C.Zhong C.Zhou X.Zhu Z.Zhu M.Zurek M.Zyzak STAR Collaboration Abilene | 2021 | Nuclear Science and Techniques2021，32，5： | 3 |
| 2 | Measurement of away-side broadening with self-subtraction of flow in Au+Au collisions at √sNN=200 GeV显示文摘High transverse momentum(pT)particle production is suppressed owing to the parton(jet)energy loss in the hot dense medium created in relativistic heavy-ion collisions.Redistribution of energy at low-to-modest pT has been difficult to measure,owing to large anisotropic backgrounds.We report a data-driven method for background evaluation and subtraction,exploiting the away-side pseudorapidity gaps,to measure the jetlike correlation shape in Au+Au collisions at √sNN=200 GeV in the STAR experiment.The correlation shapes,for trigger particles pT>3GeV/c and various associated particle pT ranges within 0.5 | L.Adamczyk J.R.Adams J.K.Adkins G.Agakishiev M.M.Aggarwal Z.Ahammed I.Alekseev D.M.Anderson A.Aparin E.C.Aschenauer M.U.Ashraf F.G.Atetalla A.Attri G.S.Averichev V.Bairathi K.Barish A.Behera R.Bellwied A.Bhasin J.Bielcik J.Bielcikova L.C.Bland I.G.Bordyuzhin J.D.Brandenburg A.V.Brandin J.Butterworth H.Caines M.Calderón de la Barca Sánchez D.Cebra I.Chakaberia P.Chaloupka B.K.Chan F-H.Chang Z.Chang N.Chankova-Bunzarova A.Chatterjee D.Chen J.H.Chen X.Chen Z.Chen J.Cheng M.Cherney M.Chevalier S.Choudhury W.Christie X.Chu H.J.Crawford M.Csanád M.Daugherity T.G.Dedovich I.M.Deppner A.A.Derevschikov L.Didenko X.Dong J.L.Drachenberg J.C.Dunlop T.Edmonds N.Elsey J.Engelage G.Eppley S.Esumi O.Evdokimov A.Ewigleben O.Eyser R.Fatemi S.Fazio P.Federic J.Fedorisin C.J.Feng Y.Feng P.Filip E.Finch Y.Fisyak A.Francisco L.Fulek C.A.Gagliardi T.Galatyuk F.Geurts A.Gibson K.Gopal D.Grosnick W.Guryn A.I.Hamad A.Hamed S.Harabasz J.W.Harris S.He W.He X.H.He S.Heppelmann S.Heppelmann N.Herrmann E.Hoffman L.Holub Y.Hong S.Horvat Y.Hu H.Z.Huang S.L.Huang T.Huang X.Huang T.J.Humanic P.Huo G.Igo D.Isenhower W.W.Jacobs C.Jena A.Jentsch Y.JI J.Jia K.Jiang S.Jowzaee X.Ju E.G.Judd S.Kabana M.L.Kabir S.Kagamaster D.Kalinkin K.Kang D.Kapukchyan K.Kauder H.W.Ke D.Keane A.Kechechyan M.Kelsey Y.V.Khyzhniak D.P.Kikoła C.Kim B.Kimelman D.Kincses T.A.Kinghorn I.Kisel A.Kiselev M.Kocan L.Kochenda L.K.Kosarzewski L.Kramarik P.Kravtsov K.Krueger N.Kulathunga Mudiyanselage L.Kumar S.Kumar R.Kunnawalkam Elayavalli J.H.Kwasizur R.Lacey S.Lan J.M.Landgraf J.Lauret A.Lebedev R.Lednicky J.H.Lee Y.H.Leung C.Li W.Li W.Li X.Li Y.Li Y.Liang R.Licenik T.Lin Y.Lin M.A.Lisa F.Liu H.Liu P.Liu P.Liu T.Liu X.Liu Y.Liu Z.Liu T.Ljubicic W.J.Llope R.S.Longacre N.S.Lukow S.Luo X.Luo G.L.Ma L.Ma R.Ma Y.G.Ma N.Magdy R.Majka D.Mallick S.Margetis C.Markert H.S.Matis J.A.Mazer N.G.Minaev S.Mioduszewski B.Mohanty I.Mooney Z.Moravcova D.A.Morozov M.Nagy J.D.Nam Nasim Md K.Nayak D.Neff J.M.Nelson D.B.Nemes M.Nie G.Nigmatkulov T.Niida L.V.Nogach T.Nonaka A.S.Nunes G.Odyniec A.Ogawa S.Oh V.A.Okorokov B.S.Page R.Pak A.Pandav Y.Panebratsev B.Pawlik D.Pawlowska H.Pei C.Perkins L.Pinsky R.L.Pintér J.Pluta J.Porter M.Posik N.K.Pruthi M.Przybycien J.Putschke H.Qiu A.Quintero S.K.Radhakrishnan S.Ramachandran R.L.Ray R.Reed H.G.Ritter O.V.Rogachevskiy J.L.Romero L.Ruan J.Rusnak N.R.Sahoo H.Sako S.Salur J.Sandweiss S.Sato W.B.Schmidke N.Schmitz B.R.Schweid F.Seck J.Seger M.Sergeeva R.Seto P.Seyboth N.Shah E.Shahaliev P.V.Shanmuganathan M.Shao A.I.Sheikh F.Shen W.Q.Shen S.S.Shi Q.Y.Shou E.P.Sichtermann R.Sikora M.Simko J.Singh S.Singha N.Smirnov W.Solyst P.Sorensen H.M.Spinka B.Srivastava T.D.S.Stanislaus M.Stefaniak D.J.Stewart M.Strikhanov B.Stringfellow A.A.P.Suaide M.Sumbera B.Summa X.M.Sun X.Sun Y.Sun Y.Sun B.Surrow D.N.Svirida P.Szymanski A.H.Tang Z.Tang A.Taranenko T.Tarnowsky J.H.Thomas A.R.Timmins D.Tlusty M.Tokarev C.A.Tomkiel S.Trentalange R.E.Tribble P.Tribedy S.K.Tripathy O.D.Tsai Z.Tu T.Ullrich D.G.Underwood I.Upsal G.Van Buren J.Vanek A.N.Vasiliev I.Vassiliev F.Videbæk S.Vokal S.A.Voloshin F.Wang G.Wang J.S.Wang P.Wang Y.Wang Y.Wang Z.Wang J.C.Webb P.C.Weidenkaff L.Wen G.D.Westfall H.Wieman S.W.Wissink R.Witt Y.Wu Z.G.Xiao G.Xie W.Xie H.Xu N.Xu Q.H.Xu Y.F.Xu Y.Xu Z.Xu Z.Xu C.Yang Q.Yang S.Yang Y.Yang Z.Yang Z.Ye Z.Ye L.Yi K.Yip H.Zbroszczyk W.Zha C.Zhang D.Zhang S.Zhang S.Zhang X.P.Zhang Y.Zhang Y.Zhang Z.J.Zhang Z.Zhang Z.Zhang J.Zhao C.Zhong C.Zhou X.Zhu Z.Zhu M.Zurek M.Zyzak | 2020 | Chinese Physics C2020，44，10： | 2 |
| 3 | 由实测双耳脉冲响应计算厅堂声学参数显示文摘为进行耦合空间声场特性及民族音乐厅堂音质的基础声学研究,与日本神户大学安藤四一声学研究室合作,对广州南方剧院进行了双耳脉冲响应及其它主要声学参数的测试,并根据所测得的双耳脉冲响应计算得出一系列重要的厅堂客观声学指标,为进一步进行主观评价,探讨主客观指标之间相互关系以及实现可听化奠定基础。 | 赵越喆 吴硕贤 邱坚珍 S.Sato | 2003 | 电声技术2003，27，7： | 1 |
| 4 | Myocardial infarction and cerebrovascular accident following non‐cardiac surgery: differences in postoperative temporal distribution and risk factors显示文摘 | M.KIKURA F.OIKAWA K.YAMAMOTO T.IWAMOTO K. A.TANAKA S.SATO G.LANDESBERG | 2008 | Journal of Thrombosis and Haemostasis2008，，5： | 1 |
| 5 | Antibacterial activity of plant extracts from azuki beans (Vigna angularis) in vitro显示文摘 | Y.Hori S.Sato A.Hatai | 2006 | Phytother Res2006，，2： | 1 |
| 6 | Preoperative estimation of remnant hepatic function using fusion images obtained by 99mTc‐labelled galactosyl‐human serum albumin liver scintigraphy and computed tomography显示文摘 | Y.Yumoto T.Yagi S.Sato K.Nouso Y.Kobayashi M.Ohmoto E.Yumoto I.Nagaya H.Nakatsukasa | 2010 | Br J Surg2010，，6： | 1 |
| 7 | Improvement of Intergranular Stress Corrosion Crack Susceptibility of Austenite Stainless Steel through Grain Boundary Engineering显示文摘奥氏体不锈钢的 Intergranular 压力腐蚀裂缝危险性通过在高温度水里进行的三点的弯曲测试被评估。试验性的结果证明通过谷物边界工程的低精力巧合地点格子边界的经常、有效的介绍导致了明显的改进内部奥氏体不锈钢的小粒的压力腐蚀裂缝抵抗。 | Weizhong JIN Sen YANG Hiroyuki KOKAWA Zhanjie WANG Yutaka S.Sato | 2007 | Journal of Materials Science & Technology2007，23，6： | 1 |
| 8 | 使用耦合电感器为新型燃料电池车开发燃料电池升压转换器显示文摘目前开发了用于新型燃料电池车(FCV)的电池电压控制单元(FCVCU)。为了缩小电力传动系统尺寸并增加驱动电机功率,需要FCVCU将燃料电池组提供的电压输送到驱动电机。FCVCU电路配置有4个单相斩波电路,平行排列形成四相交错电路。智能功率模块(IPM)是一种完整的碳化硅(SiC)IPM,这是在量产车中首款使用的功率模块,通过增加频率效应缩小设备的尺寸和被动部件损失,从而提高效率。此外,IPM使用耦合电感器来缩小电感器尺寸。结果,与先前的电压控制单元(VCU)电感器相比,每单位功率的电感器体积减少了约30%。该控制装置决定了FCVCU的输入电流和升压速率降低损耗的工作相位数,根据输入电流切换工作相位数,执行驱动相位切换控制,有助于提高VCU的效率。与传统技术相比,这些技术的采用让FCVCU体积尺寸减少了约40%,并且让动力系统安装在前舱罩下的操作更容易实现。 | R.Kitamoto S.Sato H.Nakamura A.Amano 闫红梅(译) | 2019 | 汽车与新动力2019，2，2： | 0 |
| 9 | 中型车用发动机DPR-Ⅱ排气后处理系统显示文摘日本开发了一种不采用尿素溶液的名为“DPR-Ⅱ”的排气后处理系统。该系统采用柴油作为碳氢-选择性催化还原(HC-SCR)的还原剂来减少柴油机排气中的氮氧化物(NOx)。这项基本技术能在宽广的温度范围内产生很好的NOx还原性能,以达到日本2016年排放法规要求。 | 朱炳全(译) | 2019 | 汽车与新动力2019，2，4： | 0 |
| 10 | Fe-36%Ni合金搅拌摩擦焊接头组织与性能的改善显示文摘随着能源业的发展,Fe-36%Ni合金作为结构材料的应用需求越来越广,而电弧焊时存在严重的热裂纹和再热裂纹问题。采用搅拌摩擦焊方法焊接Fe-36%Ni合金可以有效地避免电弧焊带来的裂纹问题,获得成形良好的接头。但已有研究获得的焊缝组织均有晶粒粗化的特点,导致其接头力学性能低于母材。因此,需要解决晶粒粗化问题,寻找组织与性能获得改善的方法。采用控制焊接工艺的方法改善Fe-36%Ni合金搅拌摩擦焊接头的组织和性能。结果表明,在较低的焊接速度下,调整搅拌头转速更适合于控制Fe-36%Ni合金搅拌摩擦焊接头的晶粒尺寸。搅拌头低转速带来较低的焊接热输入,使焊缝具有晶粒尺寸与母材相当或较母材晶粒细化的组织。晶粒尺寸是接头力学性能的主导因素。在400 r/min和2 mm/s的焊接工艺下可获得与母材晶粒尺寸相近、强度和硬度相当、断后伸长率也较高的接头。 | 赵玥 吴爱萍 任家烈 Yutaka S.Sato Hiroyuki Kokawa | 2012 | 焊接2012，，5： | 0 |
| 11 | 低剂量率下高线性能量转移碳离子束辐照人类唾液腺细胞的存活效应显示文摘利用日本千叶重离子医用加速器HIMAC提供的碳离子束,对人类唾液腺细胞(HSG)在剂量率为0.5Gy/h的低剂量率条件下进行了辐照,运用标准的克隆形成法得到了3种不同剂量平均线性能量转移(LET)碳离子束辐照HSG细胞的剂量存活效应.与先前HSG细胞在治癌剂量率(1￣5Gy/min)下对相近剂量平均LET碳离子束辐照的剂量存活效应数据相比,HSG细胞对高LET碳离子束辐射表现出明显的剂量率效应.为在相同条件下得到碳离子束对HSG细胞的相对生物学效应(RBE),利用60Co-#射线在剂量率为0.5Gy/h的条件下辐照了HSG细胞,得到该细胞系对低LET射线响应的剂量存活效应.与先前在治癌剂量率下得到的RBE值相比,低剂量率条件下得到的RBE值总体减小.由实验发现的剂量率效应及低剂量率条件下RBE值的减小,表明由高LET碳离子束造成的辐射损伤在低剂量率条件下也存在着显著的修复效应.据此,对辐射造成细胞致死的原因进行了探讨. | 李强 Y.FURUSAWA M.KANAZAWA M.AOKI E.URAKABE S.SATO | 2005 | 生物化学与生物物理进展2005，32，9： | 0 |
| 12 | 放射性^9C束流不同贯穿深度上的线能谱测量显示文摘为阐述放射性9C束流应用于治癌的物理基础,运用一个球形生物组织等效正比计数器测量了9C束流不同贯穿深度上的线能谱,得到了沿束流贯穿深度上的剂量平均线能分布.将实验测量得到的线能谱转换成为不同传能线密度在吸收剂量中所占份额的分布,得到了该9C束流在不同贯穿深度上的剂量平均传能线密度分布.将生物组织等效正比计数器测量得到的与先前通过平行板正比计数器测量得到的该9C束流的剂量平均传能线密度分布进行比较,发现:在束流入射通道上,两者测量数据符合很好,而在束流Bragg峰附近9C离子的沉积区域,由组织等效正比计数器测量得到的剂量平均传能线密度值大于由平行板正比计数器测量得到的值. | 李强 N.Matsufuji E.Urakabe M.Kanazawa S.Sato | 2005 | 高能物理与核物理2005，29，11： | 0 |
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