Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV
The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found...
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Veröffentlicht in: | Physical review letters 2013-12, Vol.111 (23), p.232302-232302 |
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creator | Abelev, B Adam, J Adamová, D Adare, A M Aggarwal, M M Aglieri Rinella, G Agnello, M Agocs, A G Agostinelli, A Ahammed, Z Ahmad, N Ahmad Masoodi, A Ahmed, I Ahn, S A Ahn, S U Aimo, I Ajaz, M Akindinov, A Aleksandrov, D Alessandro, B Alexandre, D Alici, A Alkin, A Alme, J Alt, T Altini, V Altinpinar, S Altsybeev, I Andrei, C Andronic, A Anguelov, V Anielski, J Anson, C Antičić, T Antinori, F Antonioli, P Aphecetche, L Appelshäuser, H Arbor, N Arcelli, S Arend, A Armesto, N Arnaldi, R Aronsson, T Arsene, I C Arslandok, M Asryan, A Augustinus, A Averbeck, R Awes, T C Äystö, J Azmi, M D Bach, M Badalà, A Baek, Y W Bailhache, R Bala, R Baldisseri, A Baltasar Dos Santos Pedrosa, F Bán, J Baral, R C Barbera, R Barile, F Barnaföldi, G G Barnby, L S Barret, V Bartke, J Basile, M Bastid, N Basu, S Bathen, B Batigne, G Batyunya, B Batzing, P C Baumann, C Bearden, I G Beck, H Behera, N K Belikov, I Bellini, F Bellwied, R Belmont-Moreno, E Bencedi, G Beole, S Berceanu, I Bercuci, A Berdnikov, Y Berenyi, D Bergognon, A A E Bertens, R A Berzano, D Betev, L Bhasin, A Bhati, A K Bhom, J Bianchi, L Bianchi, N Bianchin, C Bielčík, J Bielčíková, J |
description | The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7 GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. These observations open new possibilities for investigation of the initial conditions in heavy-ion collisions with spectator nucleons. |
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A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7 GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. 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C</creatorcontrib><creatorcontrib>Baumann, C</creatorcontrib><creatorcontrib>Bearden, I G</creatorcontrib><creatorcontrib>Beck, H</creatorcontrib><creatorcontrib>Behera, N K</creatorcontrib><creatorcontrib>Belikov, I</creatorcontrib><creatorcontrib>Bellini, F</creatorcontrib><creatorcontrib>Bellwied, R</creatorcontrib><creatorcontrib>Belmont-Moreno, E</creatorcontrib><creatorcontrib>Bencedi, G</creatorcontrib><creatorcontrib>Beole, S</creatorcontrib><creatorcontrib>Berceanu, I</creatorcontrib><creatorcontrib>Bercuci, A</creatorcontrib><creatorcontrib>Berdnikov, Y</creatorcontrib><creatorcontrib>Berenyi, D</creatorcontrib><creatorcontrib>Bergognon, A A E</creatorcontrib><creatorcontrib>Bertens, R A</creatorcontrib><creatorcontrib>Berzano, D</creatorcontrib><creatorcontrib>Betev, L</creatorcontrib><creatorcontrib>Bhasin, A</creatorcontrib><creatorcontrib>Bhati, A K</creatorcontrib><creatorcontrib>Bhom, J</creatorcontrib><creatorcontrib>Bianchi, L</creatorcontrib><creatorcontrib>Bianchi, N</creatorcontrib><creatorcontrib>Bianchin, C</creatorcontrib><creatorcontrib>Bielčík, J</creatorcontrib><creatorcontrib>Bielčíková, J</creatorcontrib><creatorcontrib>ALICE Collaboration</creatorcontrib><title>Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV</title><title>Physical review letters</title><addtitle>Phys Rev Lett</addtitle><description>The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7 GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. These observations open new possibilities for investigation of the initial conditions in heavy-ion collisions with spectator nucleons.</description><issn>1079-7114</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2013</creationdate><recordtype>article</recordtype><recordid>eNo1kE1KAzEAhQdBbK1eQbJsFyPJJJNMFi6k_kKpXQxuh_yNjWSaMUmVggfwDB7PkzhqXT0efHw83kE2RpDxnCFERtlxjM8QQlTQ6igbFYQwWlA4zt6vbDAqGQ1a59-Ab4Fai_A09F6EZJUzEYgEOquD6K22aQeCcSLZVwOSB2ltQOwHgUg-gN6JjQF2A1YyX0mgvHM2Wr_5VXx9fE7jdLmczS6Kc0ZBbR5PssNWuGhO9znJ6pvren6XLx5u7-eXi7wvKcw1FkoZilRVtloVShEJcYVxxREpdFsJoQVhkmolieSSl6bkhGDKqRaScYUn2fRP2wf_sjUxNZ2NyriftX4bG0Q4ZnzwFQN6tke3sjO66YPtRNg1_4fhb4h_ZzI</recordid><startdate>20131206</startdate><enddate>20131206</enddate><creator>Abelev, B</creator><creator>Adam, J</creator><creator>Adamová, D</creator><creator>Adare, A M</creator><creator>Aggarwal, M M</creator><creator>Aglieri Rinella, G</creator><creator>Agnello, M</creator><creator>Agocs, A 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Bearden, I G ; Beck, H ; Behera, N K ; Belikov, I ; Bellini, F ; Bellwied, R ; Belmont-Moreno, E ; Bencedi, G ; Beole, S ; Berceanu, I ; Bercuci, A ; Berdnikov, Y ; Berenyi, D ; Bergognon, A A E ; Bertens, R A ; Berzano, D ; Betev, L ; Bhasin, A ; Bhati, A K ; Bhom, J ; Bianchi, L ; Bianchi, N ; Bianchin, C ; Bielčík, J ; Bielčíková, J</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-p560-d3acce61c85fdc2cc4b0383389142df8aada47b6dcb4b9b95e59443696dab79c3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2013</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Abelev, B</creatorcontrib><creatorcontrib>Adam, J</creatorcontrib><creatorcontrib>Adamová, D</creatorcontrib><creatorcontrib>Adare, A M</creatorcontrib><creatorcontrib>Aggarwal, M M</creatorcontrib><creatorcontrib>Aglieri Rinella, G</creatorcontrib><creatorcontrib>Agnello, 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A</creatorcontrib><creatorcontrib>Anguelov, V</creatorcontrib><creatorcontrib>Anielski, J</creatorcontrib><creatorcontrib>Anson, C</creatorcontrib><creatorcontrib>Antičić, T</creatorcontrib><creatorcontrib>Antinori, F</creatorcontrib><creatorcontrib>Antonioli, P</creatorcontrib><creatorcontrib>Aphecetche, L</creatorcontrib><creatorcontrib>Appelshäuser, H</creatorcontrib><creatorcontrib>Arbor, N</creatorcontrib><creatorcontrib>Arcelli, S</creatorcontrib><creatorcontrib>Arend, A</creatorcontrib><creatorcontrib>Armesto, N</creatorcontrib><creatorcontrib>Arnaldi, R</creatorcontrib><creatorcontrib>Aronsson, T</creatorcontrib><creatorcontrib>Arsene, I C</creatorcontrib><creatorcontrib>Arslandok, M</creatorcontrib><creatorcontrib>Asryan, A</creatorcontrib><creatorcontrib>Augustinus, A</creatorcontrib><creatorcontrib>Averbeck, R</creatorcontrib><creatorcontrib>Awes, T C</creatorcontrib><creatorcontrib>Äystö, J</creatorcontrib><creatorcontrib>Azmi, M D</creatorcontrib><creatorcontrib>Bach, M</creatorcontrib><creatorcontrib>Badalà, A</creatorcontrib><creatorcontrib>Baek, Y W</creatorcontrib><creatorcontrib>Bailhache, R</creatorcontrib><creatorcontrib>Bala, R</creatorcontrib><creatorcontrib>Baldisseri, A</creatorcontrib><creatorcontrib>Baltasar Dos Santos Pedrosa, F</creatorcontrib><creatorcontrib>Bán, J</creatorcontrib><creatorcontrib>Baral, R C</creatorcontrib><creatorcontrib>Barbera, R</creatorcontrib><creatorcontrib>Barile, F</creatorcontrib><creatorcontrib>Barnaföldi, G G</creatorcontrib><creatorcontrib>Barnby, L S</creatorcontrib><creatorcontrib>Barret, V</creatorcontrib><creatorcontrib>Bartke, J</creatorcontrib><creatorcontrib>Basile, M</creatorcontrib><creatorcontrib>Bastid, N</creatorcontrib><creatorcontrib>Basu, S</creatorcontrib><creatorcontrib>Bathen, B</creatorcontrib><creatorcontrib>Batigne, G</creatorcontrib><creatorcontrib>Batyunya, B</creatorcontrib><creatorcontrib>Batzing, P C</creatorcontrib><creatorcontrib>Baumann, C</creatorcontrib><creatorcontrib>Bearden, I G</creatorcontrib><creatorcontrib>Beck, H</creatorcontrib><creatorcontrib>Behera, N K</creatorcontrib><creatorcontrib>Belikov, I</creatorcontrib><creatorcontrib>Bellini, F</creatorcontrib><creatorcontrib>Bellwied, R</creatorcontrib><creatorcontrib>Belmont-Moreno, E</creatorcontrib><creatorcontrib>Bencedi, G</creatorcontrib><creatorcontrib>Beole, S</creatorcontrib><creatorcontrib>Berceanu, I</creatorcontrib><creatorcontrib>Bercuci, A</creatorcontrib><creatorcontrib>Berdnikov, Y</creatorcontrib><creatorcontrib>Berenyi, D</creatorcontrib><creatorcontrib>Bergognon, A A E</creatorcontrib><creatorcontrib>Bertens, R A</creatorcontrib><creatorcontrib>Berzano, D</creatorcontrib><creatorcontrib>Betev, L</creatorcontrib><creatorcontrib>Bhasin, A</creatorcontrib><creatorcontrib>Bhati, A K</creatorcontrib><creatorcontrib>Bhom, J</creatorcontrib><creatorcontrib>Bianchi, L</creatorcontrib><creatorcontrib>Bianchi, N</creatorcontrib><creatorcontrib>Bianchin, C</creatorcontrib><creatorcontrib>Bielčík, J</creatorcontrib><creatorcontrib>Bielčíková, J</creatorcontrib><creatorcontrib>ALICE Collaboration</creatorcontrib><collection>PubMed</collection><collection>MEDLINE - Academic</collection><jtitle>Physical review letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Abelev, B</au><au>Adam, J</au><au>Adamová, D</au><au>Adare, A M</au><au>Aggarwal, M M</au><au>Aglieri Rinella, G</au><au>Agnello, M</au><au>Agocs, A G</au><au>Agostinelli, A</au><au>Ahammed, Z</au><au>Ahmad, N</au><au>Ahmad Masoodi, A</au><au>Ahmed, I</au><au>Ahn, S A</au><au>Ahn, S U</au><au>Aimo, I</au><au>Ajaz, M</au><au>Akindinov, A</au><au>Aleksandrov, D</au><au>Alessandro, B</au><au>Alexandre, D</au><au>Alici, A</au><au>Alkin, A</au><au>Alme, J</au><au>Alt, T</au><au>Altini, V</au><au>Altinpinar, S</au><au>Altsybeev, I</au><au>Andrei, C</au><au>Andronic, A</au><au>Anguelov, V</au><au>Anielski, J</au><au>Anson, C</au><au>Antičić, T</au><au>Antinori, F</au><au>Antonioli, P</au><au>Aphecetche, L</au><au>Appelshäuser, H</au><au>Arbor, N</au><au>Arcelli, S</au><au>Arend, A</au><au>Armesto, N</au><au>Arnaldi, R</au><au>Aronsson, T</au><au>Arsene, I C</au><au>Arslandok, M</au><au>Asryan, A</au><au>Augustinus, A</au><au>Averbeck, R</au><au>Awes, T C</au><au>Äystö, J</au><au>Azmi, M D</au><au>Bach, M</au><au>Badalà, A</au><au>Baek, Y W</au><au>Bailhache, R</au><au>Bala, R</au><au>Baldisseri, A</au><au>Baltasar Dos Santos Pedrosa, F</au><au>Bán, J</au><au>Baral, R C</au><au>Barbera, R</au><au>Barile, F</au><au>Barnaföldi, G G</au><au>Barnby, L S</au><au>Barret, V</au><au>Bartke, J</au><au>Basile, M</au><au>Bastid, N</au><au>Basu, S</au><au>Bathen, B</au><au>Batigne, G</au><au>Batyunya, B</au><au>Batzing, P C</au><au>Baumann, C</au><au>Bearden, I G</au><au>Beck, H</au><au>Behera, N K</au><au>Belikov, I</au><au>Bellini, F</au><au>Bellwied, R</au><au>Belmont-Moreno, E</au><au>Bencedi, G</au><au>Beole, S</au><au>Berceanu, I</au><au>Bercuci, A</au><au>Berdnikov, Y</au><au>Berenyi, D</au><au>Bergognon, A A E</au><au>Bertens, R A</au><au>Berzano, D</au><au>Betev, L</au><au>Bhasin, A</au><au>Bhati, A K</au><au>Bhom, J</au><au>Bianchi, L</au><au>Bianchi, N</au><au>Bianchin, C</au><au>Bielčík, J</au><au>Bielčíková, J</au><aucorp>ALICE Collaboration</aucorp><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV</atitle><jtitle>Physical review letters</jtitle><addtitle>Phys Rev Lett</addtitle><date>2013-12-06</date><risdate>2013</risdate><volume>111</volume><issue>23</issue><spage>232302</spage><epage>232302</epage><pages>232302-232302</pages><eissn>1079-7114</eissn><abstract>The directed flow of charged particles at midrapidity is measured in Pb-Pb collisions at √(s(NN))=2.76 TeV relative to the collision symmetry plane defined by the spectator nucleons. A negative slope of the rapidity-odd directed flow component with approximately 3 times smaller magnitude than found at the highest RHIC energy is observed. This suggests a smaller longitudinal tilt of the initial system and disfavors the strong fireball rotation predicted for the LHC energies. The rapidity-even directed flow component is measured for the first time with spectators and found to be independent of pseudorapidity with a sign change at transverse momenta p(T) between 1.2 and 1.7 GeV/c. Combined with the observation of a vanishing rapidity-even p(T) shift along the spectator deflection this is strong evidence for dipolelike initial density fluctuations in the overlap zone of the nuclei. Similar trends in the rapidity-even directed flow and the estimate from two-particle correlations at midrapidity, which is larger by about a factor of 40, indicate a weak correlation between fluctuating participant and spectator symmetry planes. These observations open new possibilities for investigation of the initial conditions in heavy-ion collisions with spectator nucleons.</abstract><cop>United States</cop><pmid>24476260</pmid><tpages>1</tpages></addata></record> |
fulltext | fulltext |
identifier | EISSN: 1079-7114 |
ispartof | Physical review letters, 2013-12, Vol.111 (23), p.232302-232302 |
issn | 1079-7114 |
language | eng |
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source | American Physical Society Journals |
title | Directed flow of charged particles at midrapidity relative to the spectator plane in Pb-Pb collisions at √(s(NN))=2.76 TeV |
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