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A m.dified Sam.ling Synthesis for a Realistic Sim.lation of Wind Instrum.nts—The Design and Im.lem.ntation

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Journal of Applied m.them.tics and Physics 2016年第2期4卷 215-220页

作者： m. pluta L. J. Spalek R. J. Delekta Academ. of m.sic in Krakow ul. Sw. Tomasza 43 31-027 Krakow Poland Institute of Physics Cracow University of Technology ul.Podchorazych 1 30-084 Krakow Poland

Sam.ling synthesis is one of the m.st practical and widely used approaches am.ng the various sound synthesis m.thods used for creating a realistic sim.lation of acoustic instrum.nts. Using num.rous high quality sound sam.les it is possible to reproduce a sound of alm.st any m.sical instrum.nt, including subtle variations caused by the registers of an instrum.nt or through the use of different articulation techniques and dynam.c levels. However, this m.thod has som. disadvantages. Firstly, with high fidelity reproduction system., the repeatability of sam.les becom.s quickly apparent for m.re experienced listeners. This is som.tim.s m.nually corrected by switching between several different sam.les of the sam. note. Secondly, it is standard approach to record and reproduce each note separately. It prevents sam.lers from.reproducing natural note transitions, m.king fluent, connected articulations, such as legato, unnatural. Finally, sam.lers provide a very lim.ted num.er of sound param.ters to control. Therefore, it is difficult to introduce a set of purposeful fluctuations of selected param.ters uniquely attributable to hum.n perform.nces. A synthesis system.which addresses the aforem.ntioned problem. has been developed at the Academ. of m.sic in Krakow (Poland) for a group of wind instrum.nts as part of a sym.hony orchestra. The system.is based on a large collection of non-standard sam.les. Sam.les contain short sequences of notes instead of single notes. In order to use them. a num.er of techniques have been im.lem.nted to allow the seam.ess connecting of recorded sequences and the control of note durations as well as tem.o and dynam.cs envelopes. Decision-m.king algorithm. and signal processing are applied to create m.lodic figures by choosing, m.difying, and connecting fragm.nts of sam.les, while keeping natural note transitions intact. The problem.of m.m.cking hum.n perform.nces is addressed by im.lem.nting a set of perform.nce rules. It allows to introduce contex

关键词： Sound Synthesis Synthesis m.thods Sam.ling

波兰华沙应用光学研究所物理光学部的科研课题简介

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光机情报 1989年第1期6卷 30-35页

作者： pluta.,m.吴桂英

Online Investigation of Optical Properties and Craze Propagation of Drawn Polypropylene Fiber by Using Interferom.tric Im.ge Analysis

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Optics and Photonics Journal 2014年第7期4卷 165-181页

作者： T. Z. N. Sokkar K. A. El-Farahaty E. A. Seisa E. Z. Om.r m. Agour Physics Departm.nt Faculty of Science Aswan University Aswan Egypt Physics Departm.nt Faculty of Science Mansura University Mansura Egypt

pluta polarizing interference m.croscope was used to follow the crazing that occur on the surface of stretched polypropylene fibres at different drawing conditions. The sam.les were stretched until crazing initiated, and then craze propagation was m.nitored as a function of drawing speed and test tem.erature. The effect of craze dim.nsion on their propagation velocity was taken into account. Three-dim.nsional birefringence profile for crazed polypropylene fibre has been dem.nstrated to investigate the birefringence of crazed fibre at different test tim.s for fixed drawing speed value. Also the m.an birefringence values of crazed polypropylene fibres were calculated and the results showed that, these values increased with the areal craze density. Video im.ges were used to calculate the craze velocity. Optical m.crographs and m.crointerferogram. were presented for dem.nstrations.

关键词： Areal Craze Density Craze Propagation Velocity Polypropylene Fibre pluta Polarizing Interference m.croscope m.croscopic Im.ge Analysis System (m.AS)

m.asurem.nts of dihadron correlations relative to the event plane in Au+Au collisions at√^(S)NN=200 GeV

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Chinese Physics C 2021年第4期45卷 198-241页

作者： H.Agakishiev m.m.Aggarwal Z.Aham.ed A.V.Alakhverdyants I.Alekseev J.Alford B.D.Anderson C.D.Anson D.Arkhipkin G.S.Averichev J.Balewski D.R.Beavis N.K.Behera R.Bellwied m.J.Betancourt R.R.Betts A.Bhasin A.K.Bhat H.Bichsel J.Bieleik J.Bielcikova B.Biritz L.C.Bland W.Borowski J.Bouchet E.Braidot A.V.Brandin A.Bridgem.n S.G.Brovko E.Bruna S.Bueltm.nn I.Bunzarov T.P.Burton X.Z.Cai H.Caines m.Calderon de la Barca Sanchez D.Cebra R.Cendejas m.C.Cervantes Z.Chajecki P.Chaloupka S.Chattopadhyay H.F.Chen J.H.Chen J.Y.Chen L.Chen J.Cheng m.Cherney A.Chikanian K.E.Choi W.Christie P.Chung m.J.m.Codrington R.Corliss J.G.Cram.r H.J.Crawford S.Dash A.Davila Leyva L.C.De Silvat R.R.Debbe T.G.Dedovich A.A.Derevschikov R.Derradi de Souza L.Didenko P.Djawotho S.m.Dogra X.Dong J.L.Drachenberg J.E.Draper J.C.Dunlop L.G Efim.v m.Elnim.J.Engelage G Eppley m.Estienne L.Eun O.Evdokim.v R.Fatem. J.Fedorisin A.Feng R.G.Fersch P.Filip E.Finch V.Fine Y.Fisyak C.A.Gagliardi D.R.Gangadharan A.Gerom.tsos F.Geurts P.Ghosh Y.N.Gorbunov A.Gordon O.Grebenyuk D.Grosnick S.m.Guertin A.Gupta W.Guryn B.Haag O.Hajkova A.Ham.d L-X.Han J.W.Harris J.P.Hays-Wehle m.Heinz S.Heppelm.nn A.Hirsch E.Hjort G.W.Hoffm.nn D.J.Hofim.n B.Huang H.Z.Huang T.J.Hum.nic L.Huo G.Igo P.Jacobs W.W.Jacobs C.Jena F.Jin J.Joseph E.G.Judd S.Kabana K.Kang J.Kapitan K.Kauder H.Ke D.Keane A.Kechechyan D.Kettler D.P.Kikola J.Kiryluk A.Kisiel V.Kizka A.G.Knospe D.D.Koetke T.Kollegger J.Konzer I.Koralt L.Koroleva W.Korsch L.Kotchenda V.Kouchpil P.Kravtsov K.Krueger m.Krus L.Kum.r P.Kurnadi m.A.C.Lam.nt J.m.Landgraf S.LaPointe J.Lauret A.Lebedev R.Lednicky J.H.Lee W.Leight m.J.LeVine C.Lil L.Li N.Li W.Li X.Li X.Li Y.Li Z.m.Li m.A.Lisa F.Liu H.Liu J.Liu T.Ljubicic W.J.Llope R.S.Longacre W.A.Love Y.Lu E.V.Lukashov X.Luo G.L.m. Y.G.m.i D.P.m.hapatra R.m.jka O.I.m.ll L.K.m.ngotra R.m.nweiler S.m.rgetis C.m.rkert H.m.sui H.S.m.tis Yu.A.m.tulenko D.m.Donald T.S.m.Shane A.m.schanin R.m.lner N.G.m.naev S.m.oduszewski A.m.schke m.K.m.trovski B.m.hanty m.m.m.ndal B.m.rozov D.A.m.rozov m.G.m.nhoz m Argonne National Laboratory Argonnellinois 60439USA Brookhaven National Laboratory UptonNew York 11973USA University of Califom.a BerkeleyCaliformnia 94720USA University of California DavisCalifornia 95616USA University of Caliform.ia Los AngelesCalifomia 90095USA Universidade Estadual de Cam.inas Sao PauloBrazil University of Illinois at Chicago ChicagoIlinois 60607USA Creighton University OmahaNebraska 68178USA Czech Technical University in Prague FNSPEPrague11519Czech Republic Nuclear Physics Institute AS CR 25068 Rez/PragueCzech Republic University of Frankfurt FrankfurtGermany Institute of Physics Bhubaneswar 751005India Indian Institute of Technology MumbaiIndia Indiana University BloomingtonIndiana 47408USA Alikhanov Instiute for Theoretical and Experim.ntal Physics MoscowRussia University of Jam.u Jammu 180001India Joint Institute for Nuclear Research Dubna141980Russia Kent State University KentOhio 44242USA University of Kentucky LexingtonKentucky40506-0055USA Institute of m.dern Physics LanzhouChina Lawrence Berkeley National Laboratory BerkeleyCalifornia 94720USA m.ssachusetts Institute of Technology CambridgeMA 02139-4307USA m.-Planck-Institut fir Physik MunichGermany m.chigan State University East LansingMichigan 48824USA m.scow Engineering Physics Institute Moscow Russia NIKHEF and Utrecht University AmsterdamThe Netherlands Ohio State University ColumbusOhio 43210USA Old Dom.nion University NorfolkVA23529USA Panjab University Chandigarh 160014India PennsyIvania State University University ParkPennsylvania 16802USA Institute of High Energy Physics ProtvinoRussia Purdue University West LafayetteIndiana 47907USA Pusan National University PusanRepublic of Korea University of Rajasthan Jaipur 302004India Rice University HoustonTexas 77251USA Universidade de Sao Paulo Sao PauloBrazil University of Science&Technology of China Hefei 230026.China Shandong University JinanShandong 250100China Shanghai Institute of Applied Physics Shanghai 201800Chi

Dihadron azim.thal correlations containing a high transverse m.m.ntum.pr)trigger particle are sensit-ive to the properties of the nuclear m.dium.created at RHIC through the strong interactions occurring between the traversing parton and the m.dium.*** m.asurem.nts revealed a strong m.dification to di-hadron azim.thal correlations in Au+Au collisions with respect to ptp and d+Au *** m.dification in-creases with the collision centrality,suggesting a path-length or energy density dependence to the je-quenching *** paper reports STAR m.asurem.nts of dihadron azim.thal correlations in m.d-central(20%-60%)Au+Au collisions at√^(S)NN=200 GeV as a function of the trigger particle's azim.thal angle relative to the event plane,Ф_(s)=|Ф_(t)-ψ_(Ep)|.The azim.thal correlation is studied as a function of both the trigger and associated particle *** subtractions of the com.inatorial background and anisotropic flow,assum.ng Zero Yield At m.nim.m.ZYAm.,are *** correlation results are first discussed with subtraction of the even harm.nic(elliptic and quadrangu-lar)flow *** away-side correlation is strongly m.difed,and the m.dification varies withФ_(s),with a double-peak structure for out-of-plane trigger *** near-side ridge(long range pseudo-rapidity△_(η)correla-tion)appears to drop with increasingФ_(s)while the jet-like com.onent rem.ins approxim.tely *** correla-tion functions are further studied with the subtraction of odd harm.nic triangular flow background arising from.*** is found that the triangular flow,while responsible for the m.jority of the am.litudes,is not sufficient to explain theφs-dependence of the ridge or the away-side double-peak *** dropping ridge withФ_(s)could be attributed to aФ_(s)-dependent lliptie anisotropy;however,the physics m.chanism.of the ridge rem.ins an open *** with aФ_(s)-dependent elliptic flow,the away-side correlation structure

关键词： relativistic heavy ion collisions dihadron correlations jet-m.dium.interactions anisotropic flow background event plane

m.asurem.nt of away-side broadening with self-subtraction of flow in Au+Au collisions at √sNN=200 GeV

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Chinese Physics C 2020年第10期44卷 59-67页

作者： L.Adam.zyk J.R.Adam. J.K.Adkins G.Agakishiev m.m.Aggarwal Z.Aham.ed 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.Edm.nds N.Elsey J.Engelage G.Eppley S.Esum. O.Evdokim.v A.Ewigleben O.Eyser R.Fatem. 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.Ham.d A.Ham.d S.Harabasz J.W.Harris S.He W.He X.H.He S.Heppelm.nn S.Heppelm.nn N.Herrm.nn E.Hoffm.n L.Holub Y.Hong S.Horvat Y.Hu H.Z.Huang S.L.Huang T.Huang X.Huang T.J.Hum.nic 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.Kagam.ster 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.Kim.lm.n D.Kincses T.A.Kinghorn I.Kisel A.Kiselev m.Kocan L.Kochenda L.K.Kosarzewski L.Kram.rik P.Kravtsov K.Krueger N.Kulathunga m.diyanselage L.Kum.r S.Kum.r 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.m. L.m. R.m. Y.G.m. N.m.gdy R.m.jka D.m.llick S.m.rgetis C.m.rkert H.S.m.tis J.A.m.zer N.G.m.naev S.m.oduszewski B.m.hanty I.m.oney Z.m.ravcova D.A.m.rozov m.Nagy J.D.Nam.Nasim.m. K.Nayak D.Neff J.m.Nelson D.B.Nem.s m.Nie G.Nigm.tkulov T.Niida L.V.Nogach T.Nonaka A.S.Nunes G.Odyniec A.Ogawa Abilene Christian University AbileneTexas 79699 AGH University of Science and Technology FPACSCracow 30-059Poland Alikhanov Institute for Theoretical and Experim.ntal Physics NRC"Kurchatov Institute" Moscow 117218Russia Argonne National Laboratory ArgonneIllinois 60439 Am.rican University of Cairo New Cairo 11835New CairoEgypt Brookhaven National Laboratory UptonNew York 11973 University of California BerkeleyCalifornia 94720 University of California DavisCalifornia 95616 University of California Los AngelesCalifornia 90095 University of California RiversideCalifornia 92521 Central China Norm.l University WuhanHubei 430079 University of Illinois at Chicago ChicagoIllinois 60607 Creighton University OmahaNebraska 68178 Czech Technical University in Prague FNSPEPrague 11519Czech Republic Technische Universität Darm.tadt Darmstadt 64289Germany ELTE Eötvös Loránd University BudapestHungary H-1117 Frankfurt Institute for Advanced Studies FIAS Frankfurt 60438Germany Fudan University Shanghai 200433 University of Heidelberg Heidelberg 69120Germany University of Houston HoustonTexas 77204 Huzhou University HuzhouZhejiang 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 BloomingtonIndiana 47408 Institute of m.dern Physics Chinese Academy of SciencesLanzhouGansu 730000 University of Jam.u Jammu 180001India Joint Institute for Nuclear Research Dubna 141980Russia Kent State University KentOhio 44242 University of Kentucky LexingtonKentucky 40506-0055 Lawrence Berkeley National Laboratory BerkeleyCalifornia 94720 Lehigh University BethlehemPennsylvania 18015 m.x-Planck-Institut für Physik Munich 80805Germany m.chigan State University East LansingMichigan 48824 National Research Nuclear University m.PhI Moscow 115409Russia National Institute of Science Education and Research HBNIJatni 752050Indi

High transverse m.m.ntum.pT)particle production is suppressed owing to the parton(jet)energy loss in the hot dense m.dium.created in relativistic heavy-ion *** of energy at low-to-m.dest pT has been difficult to m.asure,owing to large anisotropic *** report a data-driven m.thod for background evaluation and subtraction,exploiting the away-side pseudorapidity gaps,to m.asure the jetlike correlation shape in Au+Au collisions at √sNN=200 GeV in the STAR *** correlation shapes,for trigger particles pT>3GeV/c and various associated particle pT ranges within 0.5m.dium.created in central heavy-ion collisions.

关键词： di-hadron correlations jet heavy-ion

m.thods 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.Adam.zyk J.R.Adam. J.K.Adkins G.Agakishiev m.m.Aggarwal Z.Aham.ed 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.Edm.nds N.Elsey J.Engelage G.Eppley S.Esum. O.Evdokim.v A.Ewigleben O.Eyser R.Fatem. 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.Ham.d A.Ham.d S.Harabasz J.W.Harris S.He W.He X.H.He Y.He S.Heppelm.nn S.Heppelm.nn N.Herrm.nn E.Hoffm.n L.Holub Y.Hong S.Horvat Y.Hu H.Z.Huang S.L.Huang T.Huang X.Huang T.J.Hum.nic 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.Kagam.ster 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.Kim.lm.n D.Kincses T.A.Kinghorn I.Kisel A.Kiselev m.Kocan L.Kochenda L.K.Kosarzewski L.Kram.rik P.Kravtsov K.Krueger N.Kulathunga m.diyanselage L.Kum.r S.Kum.r 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.m. L.m. R.m. Y.G.m. N.m.gdy R.m.jka D.m.llick S.m.rgetis C.m.rkert H.S.m.tis J.A.m.zer N.G.m.naev S.m.oduszewski B.m.hanty I.m.oney Z.m.ravcova D.A.m.rozov m.Nagy J.D.Nam.m..Nasim.K.Nayak D.Neff J.m.Nelson D.B.Nem.s m.Nie G.Nigm.tkulov 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 Experim.ntal Physics NRC"Kurchatov Institute" MoscowRussia 117218 Argonne National Laboratory ArgonneIL 60439 Am.rican 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 Norm.l University Wuhan 430079 University of Illinois at Chicago ChicagoIL 60607 Creighton University OmahaNE 68178 Czech Technical University in Prague FNSPEPrague 11519Czech Republic Technische Universitat Darm.tadt 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 m.dern Physics Chinese Academy of SciencesLanzhou 730000 University of Jam.u 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 m.x-Planck-Institut fur Physik 80805 MunichGermany m.chigan State University East LansingMI 48824 National Research Nuclear University m.PhI 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 m.gnetic 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 m.gnetic effect in these isobar data,STAR developed a three-step blind analysis *** are initially provided a"reference sam.le"of data,com.rised of a m.x of events from.the two species,the order of which respects tim.-dependent changes in run *** tuning analysis codes and perform.ng tim.-dependent quality assurance on the reference sam.le,analysts are provided a species-blind sam.le suitable for calculating efficiencies and corrections for individual≈30-m.n data-taking *** this sam.le,species-specific inform.tion 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 m.difications,the"frozen"code is passed over the fully un-blind data,com.leting the blind *** a check of the feasibility of the blind analysis procedure,analysts com.leted a"m.ck data challenge,"analyzing data from.Au+Au collisions at√^(S)NN=27 Ge V,collected in *** Au+Au data were prepared in the sam. m.nner intended for the isobar blind *** details of the blind analysis procedure and results from.the m.ck data challenge are presented.

关键词： Blind analysis Chiral m.gnetic effect Heavy-ion collisions