Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC
We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimu...
Ausführliche Beschreibung
Autor*in: |
Adamczyk, L [verfasserIn] |
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Englisch |
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2016 |
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Übergeordnetes Werk: |
Enthalten in: Physical review letters - Ridge, NY : American Physical Society, 1958, 116(2016), 11 |
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Übergeordnetes Werk: |
volume:116 ; year:2016 ; number:11 |
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OLC1972542869 |
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520 | |a We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. | ||
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PQ20160430 (DE-627)OLC1972542869 (DE-599)GBVOLC1972542869 (PRQ)pubmed_primary_270352950 (KEY)0009201020160000116001100000beamenergydependenceofthethirdharmonicofazimuthalc DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Adamczyk, L verfasserin aut Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. Adkins, J K oth Agakishiev, G oth Aggarwal, M M oth Ahammed, Z oth Alekseev, I oth Aparin, A oth Arkhipkin, D oth Aschenauer, E C oth Attri, A oth Averichev, G S oth Bai, X oth Bairathi, V oth Bellwied, R oth Bhasin, A oth Bhati, A K oth Bhattarai, P oth Bielcik, J oth Bielcikova, J oth Bland, L C oth Bordyuzhin, I G oth Bouchet, J oth Brandenburg, J D oth Brandin, A V oth Bunzarov, I oth Butterworth, J oth Caines, H oth Calderón de la Barca Sánchez, M oth Campbell, J M oth Cebra, D oth Chakaberia, I oth Chaloupka, P oth Chang, Z oth Chatterjee, A oth Chattopadhyay, S oth Chen, J H oth Chen, X oth Cheng, J oth Cherney, M oth Christie, W oth Contin, G oth Crawford, H J oth Das, S oth De Silva, L C oth Debbe, R R oth Dedovich, T G oth Deng, J oth Derevschikov, A A oth di Ruzza, B oth Didenko, L oth Dilks, C oth Dong, X oth Drachenberg, J L oth Draper, J E oth Du, C M oth Dunkelberger, L E oth Dunlop, J C oth Efimov, L G oth Engelage, J oth Eppley, G oth Esha, R oth Evdokimov, O oth Eyser, O oth Fatemi, R oth Fazio, S oth Federic, P oth Fedorisin, J oth Feng, Z oth Filip, P oth Fisyak, Y oth Flores, C E oth Fulek, L oth Gagliardi, C A oth Garand, D oth Geurts, F oth Gibson, A oth Girard, M oth Greiner, L oth Grosnick, D oth Gunarathne, D S oth Guo, Y oth Gupta, S oth Gupta, A oth Guryn, W oth Hamad, A I oth Hamed, A oth Haque, R oth Harris, J W oth He, L oth Heppelmann, S oth Heppelmann, S oth Hirsch, A oth Hoffmann, G W oth Horvat, S oth Huang, T oth Huang, X oth Huang, B oth Huang, H Z oth Huck, P oth Humanic, T J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 116(2016), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:116 year:2016 number:11 http://www.ncbi.nlm.nih.gov/pubmed/27035295 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 116 2016 11 |
spelling |
PQ20160430 (DE-627)OLC1972542869 (DE-599)GBVOLC1972542869 (PRQ)pubmed_primary_270352950 (KEY)0009201020160000116001100000beamenergydependenceofthethirdharmonicofazimuthalc DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Adamczyk, L verfasserin aut Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. Adkins, J K oth Agakishiev, G oth Aggarwal, M M oth Ahammed, Z oth Alekseev, I oth Aparin, A oth Arkhipkin, D oth Aschenauer, E C oth Attri, A oth Averichev, G S oth Bai, X oth Bairathi, V oth Bellwied, R oth Bhasin, A oth Bhati, A K oth Bhattarai, P oth Bielcik, J oth Bielcikova, J oth Bland, L C oth Bordyuzhin, I G oth Bouchet, J oth Brandenburg, J D oth Brandin, A V oth Bunzarov, I oth Butterworth, J oth Caines, H oth Calderón de la Barca Sánchez, M oth Campbell, J M oth Cebra, D oth Chakaberia, I oth Chaloupka, P oth Chang, Z oth Chatterjee, A oth Chattopadhyay, S oth Chen, J H oth Chen, X oth Cheng, J oth Cherney, M oth Christie, W oth Contin, G oth Crawford, H J oth Das, S oth De Silva, L C oth Debbe, R R oth Dedovich, T G oth Deng, J oth Derevschikov, A A oth di Ruzza, B oth Didenko, L oth Dilks, C oth Dong, X oth Drachenberg, J L oth Draper, J E oth Du, C M oth Dunkelberger, L E oth Dunlop, J C oth Efimov, L G oth Engelage, J oth Eppley, G oth Esha, R oth Evdokimov, O oth Eyser, O oth Fatemi, R oth Fazio, S oth Federic, P oth Fedorisin, J oth Feng, Z oth Filip, P oth Fisyak, Y oth Flores, C E oth Fulek, L oth Gagliardi, C A oth Garand, D oth Geurts, F oth Gibson, A oth Girard, M oth Greiner, L oth Grosnick, D oth Gunarathne, D S oth Guo, Y oth Gupta, S oth Gupta, A oth Guryn, W oth Hamad, A I oth Hamed, A oth Haque, R oth Harris, J W oth He, L oth Heppelmann, S oth Heppelmann, S oth Hirsch, A oth Hoffmann, G W oth Horvat, S oth Huang, T oth Huang, X oth Huang, B oth Huang, H Z oth Huck, P oth Humanic, T J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 116(2016), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:116 year:2016 number:11 http://www.ncbi.nlm.nih.gov/pubmed/27035295 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 116 2016 11 |
allfields_unstemmed |
PQ20160430 (DE-627)OLC1972542869 (DE-599)GBVOLC1972542869 (PRQ)pubmed_primary_270352950 (KEY)0009201020160000116001100000beamenergydependenceofthethirdharmonicofazimuthalc DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Adamczyk, L verfasserin aut Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. Adkins, J K oth Agakishiev, G oth Aggarwal, M M oth Ahammed, Z oth Alekseev, I oth Aparin, A oth Arkhipkin, D oth Aschenauer, E C oth Attri, A oth Averichev, G S oth Bai, X oth Bairathi, V oth Bellwied, R oth Bhasin, A oth Bhati, A K oth Bhattarai, P oth Bielcik, J oth Bielcikova, J oth Bland, L C oth Bordyuzhin, I G oth Bouchet, J oth Brandenburg, J D oth Brandin, A V oth Bunzarov, I oth Butterworth, J oth Caines, H oth Calderón de la Barca Sánchez, M oth Campbell, J M oth Cebra, D oth Chakaberia, I oth Chaloupka, P oth Chang, Z oth Chatterjee, A oth Chattopadhyay, S oth Chen, J H oth Chen, X oth Cheng, J oth Cherney, M oth Christie, W oth Contin, G oth Crawford, H J oth Das, S oth De Silva, L C oth Debbe, R R oth Dedovich, T G oth Deng, J oth Derevschikov, A A oth di Ruzza, B oth Didenko, L oth Dilks, C oth Dong, X oth Drachenberg, J L oth Draper, J E oth Du, C M oth Dunkelberger, L E oth Dunlop, J C oth Efimov, L G oth Engelage, J oth Eppley, G oth Esha, R oth Evdokimov, O oth Eyser, O oth Fatemi, R oth Fazio, S oth Federic, P oth Fedorisin, J oth Feng, Z oth Filip, P oth Fisyak, Y oth Flores, C E oth Fulek, L oth Gagliardi, C A oth Garand, D oth Geurts, F oth Gibson, A oth Girard, M oth Greiner, L oth Grosnick, D oth Gunarathne, D S oth Guo, Y oth Gupta, S oth Gupta, A oth Guryn, W oth Hamad, A I oth Hamed, A oth Haque, R oth Harris, J W oth He, L oth Heppelmann, S oth Heppelmann, S oth Hirsch, A oth Hoffmann, G W oth Horvat, S oth Huang, T oth Huang, X oth Huang, B oth Huang, H Z oth Huck, P oth Humanic, T J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 116(2016), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:116 year:2016 number:11 http://www.ncbi.nlm.nih.gov/pubmed/27035295 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 116 2016 11 |
allfieldsGer |
PQ20160430 (DE-627)OLC1972542869 (DE-599)GBVOLC1972542869 (PRQ)pubmed_primary_270352950 (KEY)0009201020160000116001100000beamenergydependenceofthethirdharmonicofazimuthalc DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Adamczyk, L verfasserin aut Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. Adkins, J K oth Agakishiev, G oth Aggarwal, M M oth Ahammed, Z oth Alekseev, I oth Aparin, A oth Arkhipkin, D oth Aschenauer, E C oth Attri, A oth Averichev, G S oth Bai, X oth Bairathi, V oth Bellwied, R oth Bhasin, A oth Bhati, A K oth Bhattarai, P oth Bielcik, J oth Bielcikova, J oth Bland, L C oth Bordyuzhin, I G oth Bouchet, J oth Brandenburg, J D oth Brandin, A V oth Bunzarov, I oth Butterworth, J oth Caines, H oth Calderón de la Barca Sánchez, M oth Campbell, J M oth Cebra, D oth Chakaberia, I oth Chaloupka, P oth Chang, Z oth Chatterjee, A oth Chattopadhyay, S oth Chen, J H oth Chen, X oth Cheng, J oth Cherney, M oth Christie, W oth Contin, G oth Crawford, H J oth Das, S oth De Silva, L C oth Debbe, R R oth Dedovich, T G oth Deng, J oth Derevschikov, A A oth di Ruzza, B oth Didenko, L oth Dilks, C oth Dong, X oth Drachenberg, J L oth Draper, J E oth Du, C M oth Dunkelberger, L E oth Dunlop, J C oth Efimov, L G oth Engelage, J oth Eppley, G oth Esha, R oth Evdokimov, O oth Eyser, O oth Fatemi, R oth Fazio, S oth Federic, P oth Fedorisin, J oth Feng, Z oth Filip, P oth Fisyak, Y oth Flores, C E oth Fulek, L oth Gagliardi, C A oth Garand, D oth Geurts, F oth Gibson, A oth Girard, M oth Greiner, L oth Grosnick, D oth Gunarathne, D S oth Guo, Y oth Gupta, S oth Gupta, A oth Guryn, W oth Hamad, A I oth Hamed, A oth Haque, R oth Harris, J W oth He, L oth Heppelmann, S oth Heppelmann, S oth Hirsch, A oth Hoffmann, G W oth Horvat, S oth Huang, T oth Huang, X oth Huang, B oth Huang, H Z oth Huck, P oth Humanic, T J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 116(2016), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:116 year:2016 number:11 http://www.ncbi.nlm.nih.gov/pubmed/27035295 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 116 2016 11 |
allfieldsSound |
PQ20160430 (DE-627)OLC1972542869 (DE-599)GBVOLC1972542869 (PRQ)pubmed_primary_270352950 (KEY)0009201020160000116001100000beamenergydependenceofthethirdharmonicofazimuthalc DE-627 ger DE-627 rakwb eng 550 DNB UA 1000 AVZ rvk Adamczyk, L verfasserin aut Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC 2016 Text txt rdacontent ohne Hilfsmittel zu benutzen n rdamedia Band nc rdacarrier We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. Adkins, J K oth Agakishiev, G oth Aggarwal, M M oth Ahammed, Z oth Alekseev, I oth Aparin, A oth Arkhipkin, D oth Aschenauer, E C oth Attri, A oth Averichev, G S oth Bai, X oth Bairathi, V oth Bellwied, R oth Bhasin, A oth Bhati, A K oth Bhattarai, P oth Bielcik, J oth Bielcikova, J oth Bland, L C oth Bordyuzhin, I G oth Bouchet, J oth Brandenburg, J D oth Brandin, A V oth Bunzarov, I oth Butterworth, J oth Caines, H oth Calderón de la Barca Sánchez, M oth Campbell, J M oth Cebra, D oth Chakaberia, I oth Chaloupka, P oth Chang, Z oth Chatterjee, A oth Chattopadhyay, S oth Chen, J H oth Chen, X oth Cheng, J oth Cherney, M oth Christie, W oth Contin, G oth Crawford, H J oth Das, S oth De Silva, L C oth Debbe, R R oth Dedovich, T G oth Deng, J oth Derevschikov, A A oth di Ruzza, B oth Didenko, L oth Dilks, C oth Dong, X oth Drachenberg, J L oth Draper, J E oth Du, C M oth Dunkelberger, L E oth Dunlop, J C oth Efimov, L G oth Engelage, J oth Eppley, G oth Esha, R oth Evdokimov, O oth Eyser, O oth Fatemi, R oth Fazio, S oth Federic, P oth Fedorisin, J oth Feng, Z oth Filip, P oth Fisyak, Y oth Flores, C E oth Fulek, L oth Gagliardi, C A oth Garand, D oth Geurts, F oth Gibson, A oth Girard, M oth Greiner, L oth Grosnick, D oth Gunarathne, D S oth Guo, Y oth Gupta, S oth Gupta, A oth Guryn, W oth Hamad, A I oth Hamed, A oth Haque, R oth Harris, J W oth He, L oth Heppelmann, S oth Heppelmann, S oth Hirsch, A oth Hoffmann, G W oth Horvat, S oth Huang, T oth Huang, X oth Huang, B oth Huang, H Z oth Huck, P oth Humanic, T J oth ... oth Enthalten in Physical review letters Ridge, NY : American Physical Society, 1958 116(2016), 11 (DE-627)129503959 (DE-600)208853-8 (DE-576)014907267 0031-9007 nnns volume:116 year:2016 number:11 http://www.ncbi.nlm.nih.gov/pubmed/27035295 GBV_USEFLAG_A SYSFLAG_A GBV_OLC SSG-OLC-PHY GBV_ILN_21 GBV_ILN_22 GBV_ILN_40 GBV_ILN_47 GBV_ILN_55 GBV_ILN_59 GBV_ILN_60 GBV_ILN_70 GBV_ILN_130 GBV_ILN_2004 GBV_ILN_2016 GBV_ILN_2095 GBV_ILN_2192 GBV_ILN_2279 GBV_ILN_2286 UA 1000 AR 116 2016 11 |
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Adamczyk, L @@aut@@ Adkins, J K @@oth@@ Agakishiev, G @@oth@@ Aggarwal, M M @@oth@@ Ahammed, Z @@oth@@ Alekseev, I @@oth@@ Aparin, A @@oth@@ Arkhipkin, D @@oth@@ Aschenauer, E C @@oth@@ Attri, A @@oth@@ Averichev, G S @@oth@@ Bai, X @@oth@@ Bairathi, V @@oth@@ Bellwied, R @@oth@@ Bhasin, A @@oth@@ Bhati, A K @@oth@@ Bhattarai, P @@oth@@ Bielcik, J @@oth@@ Bielcikova, J @@oth@@ Bland, L C @@oth@@ Bordyuzhin, I G @@oth@@ Bouchet, J @@oth@@ Brandenburg, J D @@oth@@ Brandin, A V @@oth@@ Bunzarov, I @@oth@@ Butterworth, J @@oth@@ Caines, H @@oth@@ Calderón de la Barca Sánchez, M @@oth@@ Campbell, J M @@oth@@ Cebra, D @@oth@@ Chakaberia, I @@oth@@ Chaloupka, P @@oth@@ Chang, Z @@oth@@ Chatterjee, A @@oth@@ Chattopadhyay, S @@oth@@ Chen, J H @@oth@@ Chen, X @@oth@@ Cheng, J @@oth@@ Cherney, M @@oth@@ Christie, W @@oth@@ Contin, G @@oth@@ Crawford, H J @@oth@@ Das, S @@oth@@ De Silva, L C @@oth@@ Debbe, R R @@oth@@ Dedovich, T G @@oth@@ Deng, J @@oth@@ Derevschikov, A A @@oth@@ di Ruzza, B @@oth@@ Didenko, L @@oth@@ Dilks, C @@oth@@ Dong, X @@oth@@ Drachenberg, J L @@oth@@ Draper, J E @@oth@@ Du, C M @@oth@@ Dunkelberger, L E @@oth@@ Dunlop, J C @@oth@@ Efimov, L G @@oth@@ Engelage, J @@oth@@ Eppley, G @@oth@@ Esha, R @@oth@@ Evdokimov, O @@oth@@ Eyser, O @@oth@@ Fatemi, R @@oth@@ Fazio, S @@oth@@ Federic, P @@oth@@ Fedorisin, J @@oth@@ Feng, Z @@oth@@ Filip, P @@oth@@ Fisyak, Y @@oth@@ Flores, C E @@oth@@ Fulek, L @@oth@@ Gagliardi, C A @@oth@@ Garand, D @@oth@@ Geurts, F @@oth@@ Gibson, A @@oth@@ Girard, M @@oth@@ Greiner, L @@oth@@ Grosnick, D @@oth@@ Gunarathne, D S @@oth@@ Guo, Y @@oth@@ Gupta, S @@oth@@ Gupta, A @@oth@@ Guryn, W @@oth@@ Hamad, A I @@oth@@ Hamed, A @@oth@@ Haque, R @@oth@@ Harris, J W @@oth@@ He, L @@oth@@ Heppelmann, S @@oth@@ Hirsch, A @@oth@@ Hoffmann, G W @@oth@@ Horvat, S @@oth@@ Huang, T @@oth@@ Huang, X @@oth@@ Huang, B @@oth@@ Huang, H Z @@oth@@ Huck, P @@oth@@ Humanic, T J @@oth@@ ... @@oth@@ |
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Adamczyk, L ddc 550 rvk UA 1000 Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC |
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Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC |
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Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC |
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beam energy dependence of the third harmonic of azimuthal correlations in au+au collisions at rhic |
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Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC |
abstract |
We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. |
abstractGer |
We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. |
abstract_unstemmed |
We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. When scaled by the pseudorapidity density of charged-particle multiplicity per participating nucleon pair, v_{3}^{2}{2} for central collisions shows a minimum near sqrt[s_{NN}]=20 GeV. |
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11 |
title_short |
Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC |
url |
http://www.ncbi.nlm.nih.gov/pubmed/27035295 |
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Adkins, J K Agakishiev, G Aggarwal, M M Ahammed, Z Alekseev, I Aparin, A Arkhipkin, D Aschenauer, E C Attri, A Averichev, G S Bai, X Bairathi, V Bellwied, R Bhasin, A Bhati, A K Bhattarai, P Bielcik, J Bielcikova, J Bland, L C Bordyuzhin, I G Bouchet, J Brandenburg, J D Brandin, A V Bunzarov, I Butterworth, J Caines, H Calderón de la Barca Sánchez, M Campbell, J M Cebra, D Chakaberia, I Chaloupka, P Chang, Z Chatterjee, A Chattopadhyay, S Chen, J H Chen, X Cheng, J Cherney, M Christie, W Contin, G Crawford, H J Das, S De Silva, L C Debbe, R R Dedovich, T G Deng, J Derevschikov, A A di Ruzza, B Didenko, L Dilks, C Dong, X Drachenberg, J L Draper, J E Du, C M Dunkelberger, L E Dunlop, J C Efimov, L G Engelage, J Eppley, G Esha, R Evdokimov, O Eyser, O Fatemi, R Fazio, S Federic, P Fedorisin, J Feng, Z Filip, P Fisyak, Y Flores, C E Fulek, L Gagliardi, C A Garand, D Geurts, F Gibson, A Girard, M Greiner, L Grosnick, D Gunarathne, D S Guo, Y Gupta, S Gupta, A Guryn, W Hamad, A I Hamed, A Haque, R Harris, J W He, L Heppelmann, S Hirsch, A Hoffmann, G W Horvat, S Huang, T Huang, X Huang, B Huang, H Z Huck, P Humanic, T J . |
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Adkins, J K Agakishiev, G Aggarwal, M M Ahammed, Z Alekseev, I Aparin, A Arkhipkin, D Aschenauer, E C Attri, A Averichev, G S Bai, X Bairathi, V Bellwied, R Bhasin, A Bhati, A K Bhattarai, P Bielcik, J Bielcikova, J Bland, L C Bordyuzhin, I G Bouchet, J Brandenburg, J D Brandin, A V Bunzarov, I Butterworth, J Caines, H Calderón de la Barca Sánchez, M Campbell, J M Cebra, D Chakaberia, I Chaloupka, P Chang, Z Chatterjee, A Chattopadhyay, S Chen, J H Chen, X Cheng, J Cherney, M Christie, W Contin, G Crawford, H J Das, S De Silva, L C Debbe, R R Dedovich, T G Deng, J Derevschikov, A A di Ruzza, B Didenko, L Dilks, C Dong, X Drachenberg, J L Draper, J E Du, C M Dunkelberger, L E Dunlop, J C Efimov, L G Engelage, J Eppley, G Esha, R Evdokimov, O Eyser, O Fatemi, R Fazio, S Federic, P Fedorisin, J Feng, Z Filip, P Fisyak, Y Flores, C E Fulek, L Gagliardi, C A Garand, D Geurts, F Gibson, A Girard, M Greiner, L Grosnick, D Gunarathne, D S Guo, Y Gupta, S Gupta, A Guryn, W Hamad, A I Hamed, A Haque, R Harris, J W He, L Heppelmann, S Hirsch, A Hoffmann, G W Horvat, S Huang, T Huang, X Huang, B Huang, H Z Huck, P Humanic, T J . |
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<?xml version="1.0" encoding="UTF-8"?><collection xmlns="http://www.loc.gov/MARC21/slim"><record><leader>01000caa a2200265 4500</leader><controlfield tag="001">OLC1972542869</controlfield><controlfield tag="003">DE-627</controlfield><controlfield tag="005">20220224042750.0</controlfield><controlfield tag="007">tu</controlfield><controlfield tag="008">160427s2016 xx ||||| 00| ||eng c</controlfield><datafield tag="028" ind1="5" ind2="2"><subfield code="a">PQ20160430</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-627)OLC1972542869</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(DE-599)GBVOLC1972542869</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(PRQ)pubmed_primary_270352950</subfield></datafield><datafield tag="035" ind1=" " ind2=" "><subfield code="a">(KEY)0009201020160000116001100000beamenergydependenceofthethirdharmonicofazimuthalc</subfield></datafield><datafield tag="040" ind1=" " ind2=" "><subfield code="a">DE-627</subfield><subfield code="b">ger</subfield><subfield code="c">DE-627</subfield><subfield code="e">rakwb</subfield></datafield><datafield tag="041" ind1=" " ind2=" "><subfield code="a">eng</subfield></datafield><datafield tag="082" ind1="0" ind2="4"><subfield code="a">550</subfield><subfield code="q">DNB</subfield></datafield><datafield tag="084" ind1=" " ind2=" "><subfield code="a">UA 1000</subfield><subfield code="q">AVZ</subfield><subfield code="2">rvk</subfield></datafield><datafield tag="100" ind1="1" ind2=" "><subfield code="a">Adamczyk, L</subfield><subfield code="e">verfasserin</subfield><subfield code="4">aut</subfield></datafield><datafield tag="245" ind1="1" ind2="0"><subfield code="a">Beam Energy Dependence of the Third Harmonic of Azimuthal Correlations in Au+Au Collisions at RHIC</subfield></datafield><datafield tag="264" ind1=" " ind2="1"><subfield code="c">2016</subfield></datafield><datafield tag="336" ind1=" " ind2=" "><subfield code="a">Text</subfield><subfield code="b">txt</subfield><subfield code="2">rdacontent</subfield></datafield><datafield tag="337" ind1=" " ind2=" "><subfield code="a">ohne Hilfsmittel zu benutzen</subfield><subfield code="b">n</subfield><subfield code="2">rdamedia</subfield></datafield><datafield tag="338" ind1=" " ind2=" "><subfield code="a">Band</subfield><subfield code="b">nc</subfield><subfield code="2">rdacarrier</subfield></datafield><datafield tag="520" ind1=" " ind2=" "><subfield code="a">We present results from a harmonic decomposition of two-particle azimuthal correlations measured with the STAR detector in Au+Au collisions for energies ranging from sqrt[s_{NN}]=7.7 to 200 GeV. The third harmonic v_{3}^{2}{2}=⟨cos3(ϕ_{1}-ϕ_{2})⟩, where ϕ_{1}-ϕ_{2} is the angular difference in azimuth, is studied as a function of the pseudorapidity difference between particle pairs Δη=η_{1}-η_{2}. Nonzero v_{3}^{2}{2} is directly related to the previously observed large-Δη narrow-Δϕ ridge correlations and has been shown in models to be sensitive to the existence of a low viscosity quark gluon plasma phase. For sufficiently central collisions, v_{3}^{2}{2} persist down to an energy of 7.7 GeV, suggesting that quark gluon plasma may be created even in these low energy collisions. In peripheral collisions at these low energies, however, v_{3}^{2}{2} is consistent with zero. 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