Dielectron Mass Spectra From Au Plus Au Collisions At Root S(Nn)=200 Ge V

L Adamczyk,X Zhu,H M Spinka,M J Levine,M J Skoby,J M Landgraf,S Heppelmann,J Seger,G Van Nieuwenhuizen, A Bhasin, S Ramachandran, Jiangsha Zhao,Z P Zhang,John T Novak,T P Burton,R A Kycia,J H Lee,B A Trzeciak,H Masui,S Y Noh,Yu Zhang,L C De Silva,R Lednicky,K Kang,P Kravtsov,Abhimanyu Sarkar,W B Schmidke, S Mioduszewski,P Chaloupka,Daniel Mcdonald,Ik Yoo, K S Engle,Z M Li,R N Singaraju, A K Bhati, Z Ahammed,W Korsch,M Pachr,Y X Pan,T Pawlak,K Xin,N Xu,Wei Yan,A Kechechyan, Fuguang Ding, M G Munhoz,I G Bordyuzhin,D R Gangadharan, R E Tribble,J M Nelson, J L Romero,N R Sahoo,N Poljak, D Cebra,Y Pandit,W Borowski, M A Lisa,Weiyang Li,J Bouchet,Kyuhwan Oh,S Vokal,A V Brandin,Pradip Kumar Sahu,Y F Wu,J K Adkins, Xiangdong Li,A H Tang,J Alford,T Kollegger,C Anson,R Debbe, H F Chen,G W Hoffmann,P Filip,D P Kikola,Zhongsheng Sun,I Kisel,Lin Yi,K D Landry, F J M Geurts,Shuying Zhang,Zhen Ye,Yiqing Guo,E P Sichtermann,J Schambach,D Keane, S Margetis,S G Brovko,R Derradi De Souza, M C Cervantes, J H Chen, Jiao Deng,Fanhung Liu,S Das, M Strikhanov,Q H Xu,Lalit Kumar,Guodong Wang,J R Stevens,A Quintero, J B Roberts,J Turnau,A Szanto De Toledo,B Haag,S Bultmann, N Smirnov,O Evdokimov,L C Bland, M Cherney,M Planinic, C Markert,M K Mustafa,Mingwang Shao,D D Koetke,I Koralt, S Gliske,H Pei,T D S Stanislaus, D G Underwood,J Takahashi,W W Jacobs,L G Efimov,A Aparin,D Tlusty,P Tribedy, J Lauret,J C Dunlop, J Bielcik,Y Sun,B Pawlik,T G Dedovich,A N Vasiliev, X L Wang, M Przybycien,X M Sun,O Hajkova,J Konzer, A Hirsch, S Kabana,S Chattopadhyay,D A Morozov,O V Rogachevskiy,Zhe Xu,S W Wissink,T S Mcshane,A A Derevschikov,X Huang, L M Lima,P R Pujahari,A Schmah,B Stringfellow, B Mohanty,Mario Fusco Girard, Xiquan Cui, H Bichsel,I Sakrejda,B Surrow, A Kisiel,L Didenko,H S Matis,D J Hofman,M Calderon De La Barca Sanchez,D Solanki,R Stock,P Yepes,J Porter,P Djawotho, Zhen Xiao,J Engelage,Md Nasim, B Srivastava,Y Fisyak,H Wieman, I Kulakov,H Jang,Z Barnovska, W Peryt,C Li, J W Harris,K Kauder,Han Xu,Z H Khan,J Fedorisin, J L Zhang,V Okorokov,W Guryn,F Videbaek,A Gibson,H Zbroszczyk,A Ohlson,I Alekseev,Han Wang, M M Aggarwal,Peter M Huck, T J Humanic, S Salur, F Wang, J G Cramer,L Kotchenda,J H Thomas,C M Du, Changsheng Yang, T K Nayak,C Perkins,Wei Xie,Zongxi Tang,J Rusnak,Y Zoulkarneeva,R S Longacre, M Sumbera,D Grosnick,B Di Ruzza,J S Wang, J Cheng,Litao Ruan,Y Zawisza,Reina Haque,D Arkhipkin,G Van Buren,T Ullrich,A Davila Leyva, X Dong,A R Timmins, E C Aschenauer, R Vertesi,K Yip,D S Smirnov, H Caines,Nirav R Shah,J Chwastowski,S Raniwala, A Chikanian,Z Chang,A Sandacz,P Sorensen,N K Pruthi,A Vossen,P V Shanmuganathan,G Agakishiev, B D Sharma,Yan Xu, S Gupta,D M M D Madagodagettige Don,C Dilks, A Gupta,S Horvat,L Eun,E Finch,G S Averichev,S Dhamija,Y Panebratsev,A Kesich,D Plyku,S Trentalange,H J Crawford,M M Mondal,O D Tsai,P Bhattarai,E G Judd,J C Webb, A Lebedev,M J M Codrington,Lx Han,K Krueger,J A Vanfossen,Q Y Shou,R Fatemi,C K Riley,N Schmitz, Yuguang Wang,D P Mahapatra,D R Beavis,X Luo,B S Page,E Sangaline,J E Draper,E W Oldag,E Shahaliev,C E Flores,Li Chen,T J M Symons,Yang Yang,L V Nogach,Akira Ogawa,R A N Oliveira,Feng Zhao,B Huang,S S Shi,M Tokarev,G D Westfall,Y H Zhu,R Varma,Y G Ma,J M Butterworth,H W Ke, B K Nandi, J Bielcikova,Geoffrey I Webb,J Pluta,M Zyzak,T Ljubicic,S Fazio, R Bellwied,M A C Lamont, C A Gagliardi,W Q Shen,A Hamed,I Bunzarov,Y P Viyogi,N G Minaev,G Odyniec,Yangguang Li,John Ross,P Pile,R Cendejas,W J Llope, R P Scharenberg,G Eppley,Chong Zhong,D N Svirida,Amitava Banerjee,G Igo,L E Dunkelberger, R Majka,Sankar K Pal,D Kalinkin,X P Zhang,H Z Huang,J L Drachenberg,P Seyboth,A M Poskanzer,H Qiu, R L Ray, R Raniwala,T Tarnowsky, S B Nurushev,Weibin Zha,G M S Vasconcelos,J Sandweiss,W Christie,U G Desouza,Masahisa Wada,A A P Suaide,G L Ma,D Garand,H G Ritter,Abhishek Roy,R Witt

PHYSICAL REVIEW LETTERS(2014)

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摘要
We report the STAR measurements of dielectron (e(+)e(-)) production at midrapidity (vertical bar y(ee)vertical bar < 1) in Au + Au collisions at root s(NN) = 200 GeV. The measurements are evaluated in different invariant mass regions with a focus on 0.30-0.76 (rho-like), 0.76-0.80 (omega-like), and 0.98-1.05 (phi-like) GeV/c(2). The spectrum in the omega-like and phi-like regions can be well described by the hadronic cocktail simulation. In the rho-like region, however, the vacuum rho spectral function cannot describe the shape of the dielectron excess. In this range, an enhancement of 1.77 +/- 0.11(stat) +/- 0.24(syst) +/- 0.33(cocktail) is determined with respect to the hadronic cocktail simulation that excludes the rho meson. The excess yield in the rho-like region increases with the number of collision participants faster than the omega and phi yields. Theoretical models with broadened rho contributions through interactions with constituents in the hot QCD medium provide a consistent description of the dilepton mass spectra for the measurement presented here and the earlier data at the Super Proton Synchrotron energies.
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