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journal of Agricultural science and Technology(B) 2011年第7期1卷 1025-1031页

作者： Y. j. kim s. h. park c. k. kim D. h. Im Y. jang s. s. kim Department of Agricultural Engineering National Academy of Agricultural Science Rural Development Administration Suwon441- 707 Republic of Korea R＆D Engine Team Daedong Industrial Co. Chang Nyong-Kun Kyungnam 635-806 Republic of Korea

A diesel engine for tractor was tested for 250 hours of durability with biodiesel fuel of 100%. An engine test cycle was designed based on the IsO test code of off-road vehicle. Eight test conditions, combination of three engine speeds and eight engine loads, were applied to the engine endurance test, and the engine was operated for eight hours in a day. Power output, fuel consumption rate, exhaust gas quality and particulate matter （Pm） were measured and discussed. For the extensive 250 hours of the tractor diesel engine endurance test no significant changes of power output, fuel consumption rate, exhaust gas quality and Pm were monitored and authors could not find any difference in the engine patterns of the two fuels of BDF100 and light oil. During all the engine endurance test conditions, no abrupt stopping was encountered but because of temperature down by the cold season the endurance test could not carried out for some periods. Pms were collected and the average F＇m was 0.027 g/kw which was far below than Tier 4 diesel engine Pm of 0.3 g/kw h defined by Us EPA Pm of the diesel engine clas,;. Overall even 100% biodiesel can be an alternative fuel for light oil for diesel engine operation with some considerations for cold sea：son use.

关键词： Endurance test biodiesel diesel engine power fuel consumption.

Antineutrino energy spectrum unfolding based on the Daya Bay measurement and its applications

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chinese Physics c 2021年第7期45卷 1-19页

作者： F.P.An A.B.Balantekin m.Bishai s.Blyth g.F.cao j.cao j.F.chang Y.chang h.s.chen s.m.chen Y.chen Y.X.chen j.cheng Z.k.cheng j.j.cherwinka m.c.chu j.P.cummings O.Dalager F.s.Deng Y.Y.Ding m.V.Diwan T.Dohnal D.Dolzhikov j.Dove m.Dvorak D.A.Dwyer j.P.gallo m.gonchar g.h.gong h.gong m.grassi W.Q.gu j.Y.guo L.guo X.h.guo Y.h.guo Z.guo R.W.hackenburg s.hans a m.he k.m.heeger Y.k.heng Y.k.hor Y.B.hsiung B.Z.hu j.R.hu T.hu Z.j.hu h.X.huang j.h.huang X.T.huang Y.B.huang P.huber D.E.jaffe k.L.jen X.L.ji X.P.ji R.A.johnson D.jones L.kang s.h.kettel s.kohn m.kramer T.j.Langford j.lee j.h.c.lee R.T.Lei R.Leitner j.k.c.Leung F.Li h.L.Li j.j.Li Q.j.Li R.h.Li s.Li s.c.Li W.D.Li X.N.Li X.Q.Li Y.F.Li Z.B.Li h.Liang c.j.Lin g.L.Lin s.Lin j.j.Ling j.m.Link26 L.Littenberg B.R.Littlejohn j.c.Liu j.L.Liu j.X.Liu c.Lu h.Q.Lu k.B.Luk B.Z.ma X.B.ma X.Y.ma Y.Q.ma R.c.mandujano c.marshall k.T.mcDonald R.D.mckeown Y.meng j.Napolitano D.Naumov E.Naumova T.m.T.Nguyen j.P.Ochoa-Ricoux A.Olshevskiy h.-R.Pan j.park s.Patton j.c.Peng c.s.j.Pun F.Z.Qi m.Qi X.Qian N.Raper j.Ren c.morales Reveco R.Rosero B.Roskovec X.c.Ruan h.steiner j.L.sun T.Tmej1 k.Treskov W.-h.Tse c.E.Tull B.Viren V.Vorobel c.h.Wang j.Wang m.Wang N.Y.Wang R.g.Wang W.Wang W.Wang X.Wang Y.Wang Y.F.Wang Z.Wang Z.Wang Z.m.Wang h.Y.Wei L.h.Wei L.j.Wen k.Whisnant c.g.White h.L.h.Wong E.Worcester D.R.Wu F.L.Wu Q.Wu W.j.Wu D.m.Xia Z.Q.Xie Z.Z.Xing h.k.Xu j.L.Xu T.Xu T.Xue c.g.Yang L.Yang Y.Z.Yang h.F.Yao m.Ye m.Yeh B.L.Young h.Z.Yu Z.Y.Yu B.B.Yue V.Zavadskyi s.Zeng Y.Zeng L.Zhan c.Zhang F.Y.Zhang h.h.Zhang j.W.Zhang Q.m.Zhang s.Q.Zhang X.T.Zhang Y.m.Zhang Y.X.Zhang Y.Y.Zhang Z.j.Zhang Z.P.Zhang Z.Y.Zhang j.Zhao R.Z.Zhao L.Zhou h.L.Zhuang j.h.Zou Institute of modern Physics East China University of Science and TechnologyShanghai 200337 University of Wisconsin MadisonWisconsin 53706 Brookhaven National Laboratory UptonNew York 11973 Department of Physics Nnational Taiwan UniversityTaipei Institute of high Energy Physics Beijing 100049 National United University Miao-Li Department of Engineering Physics Tsinghua UniversityBeijing 100048 shenzhen University Shenzhen 518061 sun Yat-sen(Zhongshan)University Guangzhou 510275 North china Electric Power University Beijing 102206 chinese University of hong kong Hongkong 999077 siena college LoudonvilleNew York 12211 Department of Physics and Astronomy University of CaliforniaIrvineCalifornia 92697 University of science and Technology of china Hefei 230022 charles University Faculty of Mathematics and PhysicsPrague joint Institute for Nuclear Research DubnaMoscow Region Department of Physics University of Illinois at Urbana-ChampaignUrbanaIllinois 61801 Lawrence Berkeley National Laboratory BerkeleyCalifornia 94720 Department of Physics Illinois Institute of TechnologyChicagoIllinois 60616 Beijing Normal University Beijing 100875 Department of Nuclear science and Technology School of Energy and Power EngineeringXi'an Jiaotong UniversityXi'an 710049 Wright Laboratory and Department of Physics Yale UniversityNew HavenConnecticut 06520 china Institute of Atomic Energy Beijing 102413 shandong University Jinan 250002 guangxi University No.100 Daxue East RoadNanning 530004 center for Neutrino Physics Virginia TechBlacksburgVirginia 24061 Institute of Physics NCTUHsinchu Department of Physics University of CincinnatiCincinnatiOhio 45221 Department of Physics College of Science and TechnologyTemple UniversityPhiladelphiaPennsylvania 19122 Dongguan University of Technology Dongguan 523808 Department of Physics University of CaliforniaBerkeleyCalifornia 94720 Department of Physics The University of Hong KongPokfulamHongkong 999077 school of Physics Nankai UniversityTianjin 300071 Department o

The prediction of reactor antineutrino spectra will play a crucial role as reactor experiments enter the precision *** positron energy spectrum of 3.5 million antineutrino inverse beta decay reactions observed by the Daya Bay experiment,in combination with the fission rates of fissile isotopes in the reactor,is used to extract the positron energy spectra resulting from the fission of specific *** information can be used to produce a precise,data-based prediction of the antineutrino energy spectrum in other reactor antineutrino experiments with different fission fractions than Daya *** positron energy spectra are unfolded to obtain the antineutrino energy spectra by removing the contribution from detector response with the Wiener-sVD unfolding *** results are obtained with other unfolding methods.A technique to construct a data-based prediction of the reactor antineutrino energy spectrum is proposed and *** the reactor fission fractions,the technique can predict the energy spectrum to a 2%*** addition,we illustrate how to perform a rigorous comparison between the unfolded antineutrino spectrum and a theoretical model prediction that avoids the input model bias of the unfolding method.

关键词： reactor antineutrino energy spectrum Daya Bay application

high-Performance Perovskite Quantum Dot solar cells Enabled by Incorporation with Dimensionally Engineered Organic semiconductor

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Nano-micro Letters 2022年第12期14卷 272-285页

作者： seyeong Lim Dae hwan lee hyuntae choi Yelim choi Dong geon lee sung Beom cho seonkyung ko jongmin choi Younghoon kim Taiho park Department of chemical Engineering Pohang University of Science and Technology(POSTECH)Pohang 37673Republic of Korea Department of materials science and Engineering Hanyang UniversitySeoul 04763Republic of Korea center of materials Digitalization Korea Institute of Ceramic Engineering and Technology(KICET)Jinju 52851Republic of Korea Department of materials science and Engineering Ajou UniversitySuwon 16499Republic of Korea Department of Energy science and Engineering Daegu Gyeongbuk Institute of Science and Technology(DGIST)Daegu 42988Republic of Korea Department of chemistry Kookmin UniversitySeoul 02707Republic of Korea

Perovskite quantum dots(PQDs)have been considered promising and effective photovoltaic absorber due to their superior optoelectronic properties and inherent material merits combining perovskites and ***,they exhibit low moisture stability at room humidity(20-30%)owing to many surface defect sites generated by inefficient ligand exchange *** surface traps must be re-passivated to improve both charge transport ability and moisture *** address this issue,PQD-organic semiconductor hybrid solar cells with suitable electrical properties and functional groups might dramatically improve the charge extraction and defect *** organic semiconductors are typically low-dimensional(1D and 2D)and prone to excessive self-aggregation,which limits chemical interaction with *** this work,we designed a new 3D star-shaped semiconducting material(star-TrcN)to enhance the compatibility with *** robust bonding with star-TrcN and PQDs is demonstrated by theoretical modeling and experimental *** star-TrcN-PQD hybrid films show improved cubic-phase stability of csPbI_(3)-PQDs via reduced surface trap states and suppressed moisture *** a result,the resultant devices not only achieve remarkable device stability over 1000 h at 20-30%relative humidity,but also boost power conversion efficiency up to 16.0%via forming a cascade energy band structure.

关键词： csPbI3 quantum dots star-shaped organic semiconductors hybrid perovskite quantum dots solar cell stability high-efficiency photovoltaics

动脉期无明显强化的肝胆期低信号结节是否存在消融或手术后肝细胞癌复发的风险？系统回顾与meta分析

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国际医学放射学杂志 2020年第3期 369-370页

作者： T.h.kim s.Woo s.han c.h.suh D.h.lee j.m.lee 肖依然 Department of Radiology Seoul National University College of Medicine

摘要目的通过系统回顾和meta分析确定接受肝切除术或射频消融(RFA)治疗的肝细胞癌(hcc)病人在钆塞酸增强mRI预处理后,无动脉期强化(APhE)的肝胆期(hBP)

关键词：

search for the doubly charmed baryon ■

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science china(Physics,mechanics & Astronomy) 2020年第2期63卷 8-22页

作者： R.Aaij c.Abellán Beteta T.Ackernley B.Adeva m.Adinolfi h.Afsharnia c.A.Aidala s.Aiola Z.Ajaltouni s.Akar P.Albicocco j.Albrecht F.Alessio m.Alexander A.Alfonso Albero g.Alkhazov P.Alvarez cartelle A.A.Alves jr s.Amato Y.Amhis L.An L.Anderlini g.Andreassi m.Andreotti F.Archilli j.Arnau Romeu A.Artamonov m.Artuso k.Arzymatov E.Aslanides m.Atzeni B.Audurier s.Bachmann j.j.Back s.Baker V.Balagura W.Baldini A.Baranov R.j.Barlow s.Barsuk W.Barter m.Bartolini F.Baryshnikov g.Bassi V.Batozskaya B.Batsukh A.Battig V.Battista A.Bay m.Becker F.Bedeschi I.Bediaga A.Beiter L.j.Bel V.Belavin s.Belin N.Beliy V.Bellee k.Belous I.Belyaev g.Bencivenni E.Ben-haim s.Benson s.Beranek A.Berezhnoy *** D.Berninghoff h.c.Bernstein E.Bertholet A.Bertolin c.Betancourt F.Betti m.O.Bettler Ia.Bezshyiko s.Bhasin j.Bhom m.s.Bieker s.Bifani P.Billoir A.Birnkraut A.Bizzeti m.Bjφrn m.P.Blago T.Blake F.Blanc s.Blusk D.Bobulska V.Bocci O.Boente garcia T.Boettcher A.Boldyrev A.Bondar N.Bondar s.Borghi m.Borisyak m.Borsato j.T.Borsuk T.j.V.Bowcock c.Bozzi s.Braun A.Brea Rodriguez m.Brodski j.Brodzicka A.Brossa gonzalo D.Brundu E.Buchanan A.Buonaura c.Burr A.Bursche j.s.Butter j.Buytaert W.Byczynski s.cadeddu h.cai R.calabrese s.cali R.calladine m.calvi m.calvo gomez A.camboni P.campana D.h.campora Perez L.capriotti A.carbone g.carboni R.cardinale A.cardini P.carniti k.carvalho Akiba A.casais Vidal g.casse m.cattaneo g.cavallero R.cenci j.cerasoli m.g.chapman m.charles Ph.charpentier g.chatzikonstantinidis m.chefdeville V.chekalina c.chen s.chen A.chernov s.-g.chitic V.chobanova m.chrzaszcz A.chubykin P.ciambrone m.F.cicala X.cid Vidal g.ciezarek F.cindolo P.E.L.clarke m.clemencic h.V.cliff j.closier j.L.cobbledick V.coco j.A.B.coelho j.cogan E.cogneras L.cojocariu P.collins T.colombo A.comerma-montells A.contu N.cooke g.coombs s.coquereau g.corti c.m.costa sobral B.couturier D.c.craik j.crkovska A.crocombe m.cruz Torres R.currie c.L.Da silva E.Dall'Occo j.Dalseno c.D'Ambrosio A.Danilina P.d'Argent A.Davis O.De Aguiar Francisco k.De Bruyn s.De capua m centro Brasileiro de Pesquisas Fisicas(cBPF) Rio de JaneiroBrazil Universidade Federal do Rio de janeiro(UFRj) Rio de JaneiroBrazil center for high Energy Physics Tsinghua UniversityBeijingChina school of Physics state key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University of chinese Academy of sciences BeijingChina Institute Of high Energy Physics(IhEP) BeijingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Univ.grenoble Alpes Univ.Savoie Mont BlancCNRSIN2P3-LAPPAnnecyFrance Universite clermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix marseille Univ CNRS/IN2P3CPPMMarseilleFrance LAL Univ.Paris-SudCNRS/IN2P3Universite Paris-SaclayOrsayFrance LPNhE Sorbonne Universite Paris Diderot Sorbonne Paris Cite CNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany max-Planck-Institut für kernphysik(mPIk) HeidelbergGermany Physikalisches Institut Ruprecht-Karls-Universitat HeidelbergHeidelbergGermany school of Physics University College DublinDublinIreland INFN sezione di Bari BariItaly INFN sezione di Bologna BolognaItaly INFN sezione di Ferrara FerraraItaly INFN sezione di Firenze FirenzeItaly INFN Laboratori Nazionali di Frascati FrascatiItaly INFN sezione di genova GenovaItaly INFN sezione di milano-Bicocca MilanoItaly INFN sezione di milano MilanoItaly INFN sezione di cagliari MonserratoItaly INFN sezione di Padova PadovaItaly INFN sezione di Pisa PisaItaly INFN sezione di Roma Tor Vergata RomaItaly INFN sezione di Roma La sapienza RomaItaly Nikhef National Institute for subatomic Physics AmsterdamNetherlands Nikhef National Institute for subatomic Physics and VU University Amsterdam AmsterdamNetherlands henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of sciences KrakowPoland Agh-University of science and Technology Faculty of Physics and Applied Computer ScienceKrakowPoland Natio

A search for the doubly charmed baryon ■^+cc is performed through its decay to theΛ^+c k^-π^+ final state,using proton-proton collision data collected with the Lhcb detector at centre-of-mass energies of 7,8 and 13 *** data correspond to a total integrated luminosity of 9 fb^-*** significant signal is observed in the mass range from 3.4 to 3.8 geV/c^*** limits are set at 95%credibility level on the ratio of the ■^+cc production cross-section times the branching fraction to that ofΛ^+c and ■^++cc *** limits are determined as functions of the ■^+cc mass for different lifetime hypotheses,in the rapidity range from 2.0 to 4.5 and the transverse momentum range from 4 to 15 geV/c.

关键词： charmed baryons limits on production of particles charmed quarks experimental tests

Phase stability and mechanical properties of wire+arc additively manufactured h13 tool steel at elevated temperatures

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journal of materials science & Technology 2021年第8期67卷 80-94页

作者： A.N.m.Tanvir md.R.U.A hsan gijeong seo Brian Bates chanho lee Peter k.Liaw mark Noakese Andrzej Nycz changwook ji Duck Bong kim Department of mechanical Engineering Tennessee Technological UniversityCookevilleTN 38505USA Department of manufacturing and Engineering Technology Tennessee Technological UniversityCookevilleTN 38505USA center for manufacturing Research Tennessee Technological UniversityCookevilleTN 38505USA Department of materials science and Engineering University of TennesseeKnoxvilleTN 37996USA manufacturing Demonstration Facility Oak Ridge National LaboratoryOak RidgeTN 37830USA Advanced Forming Process R&D group Korea Institute of Industrial TechnologyUlsan 44413Republic of Korea

Wire+arc additive manufacturing(WAAm)is considered an innovative technology that can change the manufacturing landscape in the near *** offers the benefits of inexpensive initial system setup and a high deposition rate for fabricating medium-and large-sized parts such as die-casting *** this study,AIsI h13 tool steel,a popular die-casting tool metal,is manufactured by cold metal transfer(cmT)-based WAAm and is then comprehensively analyzed for its microstructural and mechanical ***-dependent phase combinations are observed,which could be explained by nonequilibrium thermal cycles that resulted from the layer-by-layer stacking mechanism used in *** addition,remelting and reheating of the layers reduces welding anomalies(e.g.,pores and voids).The metallurgical characteristics of the h13 strongly correlate with the mechanical *** combinations of phases at different locations of the additively manufactured part exhibit a periodic microhardness ***,Retained Austenite,Ferrite,and carbide phases are found in combination at different locations of the part based on the part’s temperature distribution during additive ***,the tensile properties at elevated temperatures(23℃,300℃,and 600℃)are comparable to those from other WAAm and additive manufacturing(Am)*** X-ray diffraction results verify that the microstructural stability of the fabricated parts at high temperatures would allow them to be used in high temperatures.

关键词： Tool steel martensitic steel Wire+arc additive manufacturing(WAAm) high temperature tensile test high temperature XRD

methods for a blind analysis of isobar data collected by the sTAR collaboration

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Nuclear science and Techniques 2021年第5期32卷 43-50页

作者： 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.Nonak christian University AbileneTX 796992 Agh University of science and Technology FPACSCracow 30-059Poland Alikhanov Institute for Theoretical and Experimental Physics NRc"kurchatov Institute" MoscowRussia 117218 Argonne National Laboratory ArgonneIL 60439 American University of cairo New CairoNew Cairo 11835Egypt Brookhaven National Laboratory UptonNY 11973 University of california BerkeleyCA 94720 University of california DavisCA 95616 University of california Los AngelesCA 90095 University of california RiversideCA 92521 central china Normal University Wuhan 430079 University of Illinois at chicago ChicagoIL 60607 creighton University OmahaNE 68178 czech Technical University in Prague FNSPEPrague 11519Czech Republic Technische Universitat Darmstadt Darmstadt 64289Germany ELTE Eotvos Lorand University Budapest 1117Hungary Frankfurt Institute for Advanced studies FIAs Frankfurt 60438Germany Fudan University Shanghai 200433 University of heidelberg 69120 HeidelbergGermany University of houston HoustonTX 77204 huzhou University Huzhou 313000 Indian Institute of science Education and Research(IIsER) Berhampur 760010India Indian Institute of science Education and Research(IIsER)Tirupati Tirupati 517507India Indian Institute Technology PatnaBihar 801106India Indiana University BloomingtonIN 47408 Institute of modern Physics Chinese Academy of SciencesLanzhou 730000 University of jammu Jammu 180001India joint Institute for Nuclear Research DubnaRussia 141980 kent state University KentOH 44242 University of kentucky LexingtonKY 40506-0055 Lawrence Berkeley National Laboratory BerkeleyCA 94720 Lehigh University BethlehemPA 18015 max-Planck-Institut fur Physik 80805 MunichGermany michigan state University East LansingMI 48824 National Research Nuclear University mEPhI MoscowRussia 115409 National Institute of science Education and Research HBNIJatni 752050India National cheng kung University Tainan 70101 Nuclear Physics Institute of the cAs Rez 25068Czech Republic Ohio state University

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 *** isobar collision species alternated frequently between 9644 Ru+^(96)_(44)Ru and^(96)_(40)Zr+^(96)_(40)*** order to conduct blind analyses of studies related to the chiral magnetic effect in these isobar data,sTAR developed a three-step blind analysis *** 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 *** 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 *** this sample,species-specific information is disguised,but individual output files contain data from a single isobar *** run-by-run corrections and code alteration subsequent to these corrections are allowed at this *** these modifications,the"frozen"code is passed over the fully un-blind data,completing the blind *** 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 *** Au+Au data were prepared in the same manner intended for the isobar blind *** details of the blind analysis procedure and results from the mock data challenge are presented.

关键词： Blind analysis chiral magnetic effect heavy-ion collisions

转移灶与卵巢癌标准化摄取比值对晚期浆液性卵巢上皮癌的预后价值

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国际医学放射学杂志 2018年第1期 109-110页

作者： h.h.chung m.lee h.s.kim j.W.kim N.h.park Y.s.song 黄黎香 Department of Obstetrics and gynaecology Cancer Research InstituteSeoul National University College of Medicine

摘要目的评价术前PET/cT经18F-FDg摄取测得的转移灶代谢活性对晚期浆液性卵巢上皮癌(EOc)病人的预后价值。方法评估国际妇产科协会(FIgO)标准的卵巢癌Ⅲ、Ⅳ

关键词：卵巢上皮癌转移灶卵巢癌浆液性预后价值

search for the rare decay B^(0)→j/ψФ

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chinese Physics c 2021年第4期45卷 47-60页

作者： R.Aaij c.Abellin Beteta T.Ackernley B.Adeva m.Adinolfi h.Afsharnial c.A.Aidala s.Aiola Z.Ajaltouni s.Akar j.Albrecht F.Alessio m.Alexander A.Alfonso Albero Z.Aliouche g.Alkhazov P.Alvarez cartelle s.Amato Y.Amhis L.An L.Anderlini A.Andreianov m.Andreotti F.Archilli A.Artamonov m.Artuso k.Arzymatov E.Aslanides m.Atzeni B.Audurier s.Bachmann m.Bachmaver j.j.Back s.Baker P.Baladron Rodriguez V.Balagura W.Baldinit j.Baptista Leite R.j.Barlow s.Barsuk W.Barter m.Bartolini F.Baryshnikov j.m.Basels g.Bassi B.Batsukh A.Battig A.Bay m.Becker F.Bedeschis I.Bediaga A.Beiter V.Belavin s.Belin V.Bellee k.Belous I.Belov I.Belyaev g.Bencivenni E.Ben-haim A.Berezhnoy *** D.Berninghoff h.c.Bernstein c.Bertella E.Bertholet A.Bertolin c.Betancourt F.Betti m.O.Bettler Ia.Bezshyiko s.Bhasin j.Bhom L.Bian m.s.Bieker s.Bifani P.Billoir m.Birch F.c.R.Bishop A.Bizzeti m.Biorn m.P.Blago T.Blake F.Blanc s.Blusk D.Bobulska j.A.Boelhauve O.Boente garcia T.Boettcher A.Boldyrev A.Bondar N.Bondar s.Borghi m.Borisyak m.Borsato j.T.Borsuk s.A.Bouchiba T.j.V.Bowcock A.Boyer c.Bozzi m.j.Bradley s.Braun A.Brea Rodriguezs m.Brodski j.Brodzicka A.Brossa gonzalo D.Brundu A.Buonaura c.Burr A.Burschee A.Butkevich j.s.Butter j.Buytaert W.Byczynski s.cadeddu h.cai R.calabrese L.calefice L.calero Diaz s.cali R.calladine m.calvi m.calvo gomez P.camargo magalhaes A.camboni P.campana D.h.campora Perez A.F.campoverde Quezada s.capelli L.capriotti A.carbonel g.carboni R.cardinale A.cardini I.carli P.carniti L.carus k.carvalho Akiba A.casais Vidal g.casse m.cattaneo g.cavallero s.celani j.cerasoli A.j.chadwick m.g.chapman m.charles Ph.charpentier g.chatzikonstantinidis c.A.chavez Barajas m.chefdeville c.chen s.chen A.chernov s.-g.chitic V.chobanova s.cholak m.chrzaszcz A.chubykin V.chulikov P.ciambrone m.F.cicala X.cid Vidal g.ciezarek P.E.L.clarke m.clemencic h.V.cliff j.closier j.L.cobbledick V.coco j.A.B.coelho j.cogan E.cogneras L.cojocariu P.collins T.colombo L.congedo A.contu N.cooke g.coombs g.corti c.m.costa sobral B.couturier D.c.craik j.crkovska m.cruz centro Brasileiro de Pesquisas Fisicas(cBPF) Riode JaneiroBrazil Universidade Federal do Riode janeiro(UFRj) Riode JaneiroBrazil center for high Energy Physics Tsinghua UniversityBeijingChina school of Physics state key Laboratory of Nuclear Physics and Technology Peking UniversityBeijingChina University of chinese Academy of sciences BeijingChina Institute Of high Energy Physics(IhEP) BejingChina Institute of Particle Physics Central China Normal UniversityWuhanHubeiChina Univ.grenoble Alpes Univ.Savoie Mont BlancCNRSIN2P3-LAPPAnnecyFrance Universite clermont Auvergne CNRS/IN2P3LPCClermont-FerrandFrance Aix marseille Univ CNRS/IN2P3CPPMMarseilleFrance Universitq Paris-saclay CNRS/IN2P3IJCLabOrsayFrance LPNhE Sorbonne UniversiteParis Diderot Sorbonne Paris CiteCNRS/IN2P3ParisFrance I.Physikalisches Institut RWTH Aachen UniversityAachenGermany Fakultat Physik Technische Universitat DortmundDortmundGermany max-Planck-Institut fir kernphysik(mPIk) HeidelbergGermany Physikalisches Institut Ruprecht-Karls-Universitat HeidelbergHeidelbergGermany school of Physics University College DublinDublinIreland INFN sezione di Bari BariItaly INFN sezione di Bologna BolognaItaly INFN sezione di Ferrara FerraraItaly INFN sezione di Firenze FirenzeItaly INFN Laboratori Nazionali di Frascati Frascatiltaly INFN sezione di genova GenovaItaly INFN sezione di milano Bicocca Milanolaly INFN sezione di milano MilanoItaly INFN sezione di cagliari Monserratoltaly Universita degli studi di Padova Universita e INFNPadovaPadovaItaly INFN sezione di Pisa PisaItaly INFN sezione di Roma Tor Vergata RomaItaly INFN sezione di Roma La sapienza RomaItaly Nikhef National Institute for subatomic Physics AmsterdamNetherlands Nikhef National Institute for subatomic Physics and VU University Amsterdam AmsterdamNetherlands henryk Niewodniczanski Institute of Nuclear Physics Polish Academy of sciences KrakowPoland Agh-University of science and Technology Faculty of Physics and Applied Computer Science

A search for the rare decay B^(0)→j/ψФis performed using Pp collision data collected with the Lhcb dete-ctor at centre-of-mass energies of 7,8 and 13 TeV,corresponding to an integrated luminosity of9 *** significant signal of the decay is observed and an upper limitof 1.1x 10^(-7)at 90%confidence level is set on the branching fraction.

关键词： B physics flavour physics rare decay ω-Фmixing branching fraction