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High Transverse Momentum Triggered Correlations over a Large Pseudorapidity Acceptance in<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:mi>Au</mml:mi><mml:mo>+</mml:mo><mml:mi>Au</mml:mi></mml:math>Collisions at<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML" display="inline"><mml:msqrt><mml:msub><mml:mi>s</mml:mi><mml:mrow><mml:mi>N</mml:mi><mml:mi>N</mml:mi></mml:mrow></mml:msub></mml:msqrt><mml:mo>=</mml:mo><mml:mn>200</mml:mn><mml:mtext> </mml:mtext><mml:mtext> </mml:mtext><mml:mi>GeV</mml:mi></mml:math>

B. AlverMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAB. B. BackArgonne National Laboratory, Argonne, Illinois 60439-4843, USAM. D. BakerBrookhaven National Laboratory, Upton, New York 11973-5000, USAM. BallintijnMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAD. S. BartonBrookhaven National Laboratory, Upton, New York 11973-5000, USAR. R. BettsUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAA. A. BickleyUniversity of Maryland, College Park, Maryland 20742, USAR. BindelUniversity of Maryland, College Park, Maryland 20742, USAW. BuszaMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAA. CarrollBrookhaven National Laboratory, Upton, New York 11973-5000, USAZ. ChaiBrookhaven National Laboratory, Upton, New York 11973-5000, USAV. ChetluruUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAM. P. DecowskiMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAE. Garcı́aUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAT. GburekInstitute of Nuclear Physics PAN, Kraków, PolandN. GeorgeBrookhaven National Laboratory, Upton, New York 11973-5000, USAK. GulbrandsenMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAC. HalliwellUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAJ. HamblenUniversity of Rochester, Rochester, New York 14627, USAM. HauerBrookhaven National Laboratory, Upton, New York 11973-5000, USAC. HendersonMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAD. J. HofmanUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAR. S. HollisUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAR. HołyńskiInstitute of Nuclear Physics PAN, Kraków, PolandB. HolzmanBrookhaven National Laboratory, Upton, New York 11973-5000, USAA. IordanovaUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAE. JohnsonUniversity of Rochester, Rochester, New York 14627, USAJ. L. KaneMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAN. KhanUniversity of Rochester, Rochester, New York 14627, USAP. KulinichMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAC. M. KuoNational Central University, Chung-Li, TaiwanW. LiMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAW.T. LinNational Central University, Chung-Li, TaiwanC. LoizidesMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAS. ManlyUniversity of Rochester, Rochester, New York 14627, USAA. C. MignereyUniversity of Maryland, College Park, Maryland 20742, USAR. NouicerBrookhaven National Laboratory, Upton, New York 11973-5000, USAA. OlszewskiInstitute of Nuclear Physics PAN, Kraków, PolandR. PakBrookhaven National Laboratory, Upton, New York 11973-5000, USAC. ReedMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAC. RolandMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAG. RolandMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAJ. SagererUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAH. SealsBrookhaven National Laboratory, Upton, New York 11973-5000, USAI. SedykhBrookhaven National Laboratory, Upton, New York 11973-5000, USAChristopher SmithUniversity of Illinois at Chicago, Chicago, Illinois 60607-7059, USAM. A. StankiewiczBrookhaven National Laboratory, Upton, New York 11973-5000, USAP. SteinbergBrookhaven National Laboratory, Upton, New York 11973-5000, USAG. S. F. StephansMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAA. SukhanovBrookhaven National Laboratory, Upton, New York 11973-5000, USAM. B. TonjesUniversity of Maryland, College Park, Maryland 20742, USAA. TrzupekInstitute of Nuclear Physics PAN, Kraków, PolandC. ValeMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAG. J. van NieuwenhuizenMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAS. S. VaurynovichMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAR. VerdierMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAG. I. VeresMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAPeter WaltersUniversity of Rochester, Rochester, New York 14627, USAE. A. WengerMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USAF. L. H. WolfsUniversity of Rochester, Rochester, New York 14627, USAB. K. WosiekInstitute of Nuclear Physics PAN, Kraków, PolandK. W. WoźniakInstitute of Nuclear Physics PAN, Kraków, PolandB. WysłouchMassachusetts Institute of Technology, Cambridge, Massachusetts 02139-4307, USA
2010lv
ABI

Annotatsiya

A measurement of two-particle correlations with a high transverse momentum trigger particle (${p}_{T}^{\mathrm{trig}}&gt;2.5\text{ }\text{ }\mathrm{GeV}/c$) is presented for $\mathrm{Au}+\mathrm{Au}$ collisions at $\sqrt{{s}_{NN}}=200\text{ }\text{ }\mathrm{GeV}$ over the uniquely broad longitudinal acceptance of the PHOBOS detector ($\ensuremath{-}4&lt;\ensuremath{\Delta}\ensuremath{\eta}&lt;2$). A broadening of the away-side azimuthal correlation compared to elementary collisions is observed at all $\ensuremath{\Delta}\ensuremath{\eta}$. As in $p+p$ collisions, the near side is characterized by a peak of correlated partners at small angle relative to the trigger particle. However, in central $\mathrm{Au}+\mathrm{Au}$ collisions an additional correlation extended in $\ensuremath{\Delta}\ensuremath{\eta}$ and known as the ``ridge'' is found to reach at least $|\ensuremath{\Delta}\ensuremath{\eta}|\ensuremath{\approx}4$. The ridge yield is largely independent of $\ensuremath{\Delta}\ensuremath{\eta}$ over the measured range, and it decreases towards more peripheral collisions. For the chosen ${p}_{T}^{\mathrm{trig}}$ cut, the ridge yield is consistent with zero for events with less than roughly 100 participating nucleons.

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