000061875 001__ 61875
000061875 005__ 20140130013205.0
000061875 035__ $$9INSPIRETeX$$aAdare:2013xlp
000061875 035__ $$9arXiv$$aoai:arXiv.org:1311.1427
000061875 037__ $$9arXiv$$aarXiv:1311.1427$$cnucl-ex
000061875 100__ $$aAdare, A.$$uColorado U.
000061875 245__ $$9arXiv$$aHeavy-flavor electron-muon correlations in $p$$+$$p$ and $d$+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV
000061875 246__ $$9arXiv$$aHeavy-flavor electron-muon correlations in $p$$+$$p$ and $d$+Au collisions at $\sqrt{s_{_{NN}}}$ = 200 GeV
000061875 269__ $$c2013-11-06
000061875 300__ $$a14
000061875 500__ $$a*Brief entry*
000061875 500__ $$9arXiv$$a449 authors, 14 pages, 11 figures, 2 tables. Submitted to Phys. Rev. C. Plain text data tables for the points plotted in figures for this and previous PHENIX publications are (or will be) publicly available at http://www.phenix.bnl.gov/papers.html
000061875 500__ $$a*Temporary entry*
000061875 520__ $$9arXiv$$aWe report $e^\pm-\mu^\mp$ pair yield from charm decay measured between midrapidity electrons ($|\eta|<0.35$ and $p_T>0.5$ GeV/$c$) and forward rapidity muons ($1.4<\eta<2.1$ and $p_T>1.0$ GeV/$c$) as a function of $\Delta\phi$ in both $p$$+$$p$ and in $d$+Au collisions at $\sqrt{s_{_{NN}}}=200$ GeV. Comparing the $p$$+$$p$ results with several different models, we find the results are consistent with a total charm cross section $\sigma_{c\bar{c}} =$ 538 $\pm$ 46 (stat) $\pm$ 197 (data syst) $\pm$ 174 (model syst) $\mu$b. These generators also indicate that the back-to-back peak at $\Delta\phi = \pi$ is dominantly from the leading order contributions (gluon fusion), while higher order processes (flavor excitation and gluon splitting) contribute to the yield at all $\Delta\phi$. We observe a suppression in the pair yield per collision in $d$+Au. We find the pair yield suppression factor for $2.7<\Delta\phi<3.2$ rad is $J_{dA}$ = 0.433 $\pm$ 0.087 (stat) $\pm$ 0.135 (syst), indicating cold nuclear matter modification of $c\bar{c}$ pairs.
000061875 540__ $$ahttp://arxiv.org/licenses/nonexclusive-distrib/1.0/$$barXiv
000061875 541__ $$aarxiv$$cOAI
000061875 65017 $$2arXiv$$anucl-ex
000061875 65017 $$2INSPIRE$$aExperiment-Nucl
000061875 693__ $$eBNL-RHIC-PHENIX
000061875 695__ $$2INSPIRE$$a* Automatic Keywords *
000061875 695__ $$2INSPIRE$$ahigher-order: 0
000061875 695__ $$2INSPIRE$$aelectron muon: correlation
000061875 695__ $$2INSPIRE$$agluon: splitting
000061875 695__ $$2INSPIRE$$amuon: rapidity
000061875 695__ $$2INSPIRE$$agluon: fusion
000061875 695__ $$2INSPIRE$$acharm: decay
000061875 695__ $$2INSPIRE$$asuppression
000061875 695__ $$2INSPIRE$$anuclear matter
000061875 695__ $$2INSPIRE$$aexcited state
000061875 695__ $$2INSPIRE$$aheavy quark
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000061875 700__ $$aPark, S.K.$$uKorea U.
000061875 700__ $$aPark, W.J.$$uKorea U.
000061875 700__ $$aPate, S.F.$$uNew Mexico State U.
000061875 700__ $$aPei, H.$$uIowa State U.
000061875 700__ $$aPeng, J.C.$$uIllinois U., Urbana
000061875 700__ $$aPereira, H.$$uDAPNIA, Saclay
000061875 700__ $$aPeresedov, V.$$uDubna, JINR
000061875 700__ $$aPeressounko, D.Yu.$$uKurchatov Inst., Moscow
000061875 700__ $$aPetti, R.$$uSUNY, Stony Brook
000061875 700__ $$aPinkenburg, C.$$uBrookhaven
000061875 700__ $$aPisani, R.P.$$uBrookhaven
000061875 700__ $$aProissl, M.$$uSUNY, Stony Brook
000061875 700__ $$aPurschke, M.L.$$uBrookhaven
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000061875 700__ $$aQu, H.$$uGeorgia State U.
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000061875 700__ $$aRakotozafindrabe, A.$$uEcole Polytechnique
000061875 700__ $$aRavinovich, I.$$uWeizmann Inst.
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000061875 700__ $$aRembeczki, S.$$uFlorida Inst. Tech.
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000061875 700__ $$aRiabov, V.$$uSt. Petersburg, INP
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000061875 700__ $$aRoche, G.$$uClermont-Ferrand U.
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000061875 700__ $$aSemenov, A.Yu.$$uIowa State U.
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000061875 700__ $$aZaudtke, O.$$uMunster U.
000061875 700__ $$aZhang, C.$$uOak Ridge
000061875 700__ $$aZhou, S.$$uBeijing, Inst. Atomic Energy
000061875 700__ $$aZolin, L.$$uDubna, JINR
000061875 710__ $$gPHENIX Collaboration
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/DecayCorrelation_Run6pp_North.png$$y00006 The fully-corrected like-sign-subtracted and near-far vertex-subtracted (see text) muon-decay $\Delta\phi$ pair yield in (a) \pp and (b) \dAu collisions. Both are consistent with no residual correlation after like-sign subtraction. The solid lines and shaded bands indicate the flat line fits and their uncertainty with $\chi^2$/NDF of 27.1/24 and 18.0/24 in \pp and~\dAu, respectively.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/DecayCorrelation_Run8dAu_North.png$$y00007 The fully-corrected like-sign-subtracted and near-far vertex-subtracted (see text) muon-decay $\Delta\phi$ pair yield in (a) \pp and (b) \dAu collisions. Both are consistent with no residual correlation after like-sign subtraction. The solid lines and shaded bands indicate the flat line fits and their uncertainty with $\chi^2$/NDF of 27.1/24 and 18.0/24 in \pp and~\dAu, respectively.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/FinalPP.png$$y00010 (Color Online) The fully-corrected like-sign-subtracted heavy flavor $e$--$\mu$ pair yield in \pp. The error bars are statistical only. The boxes show the type B systematic uncertainty from the punch-through hadron and light hadron decay muon background subtraction. The 16.1\% type C systematic uncertainty is not shown.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/FinaldAu.png$$y00012 (Color Online) The fully corrected like-sign-subtracted heavy flavor $e$--$\mu$ pair yield in \dAu. The error bars are statistical only. The boxes show the type B systematic uncertainty from the punch-through hadron and light hadron decay muon background subtraction. The 13.4\% type C systematic uncertainty is not shown.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/JdAuVsDphi_all.png$$y00014 $J_{dA}$ is plotted as a function of $\Delta\phi$. The vertical bars are statistical uncertainties, the black boxes are the type B systematic uncertainties, and the gray band around 1.0 on the left is the type C systematic uncertainty. The type B systematics are symmetric around the central value but in some cases are outside the range of the plot. (b) alternative rebinning of the data in (a).
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/JdAuVsDphi_rebinned.png$$y00015 $J_{dA}$ is plotted as a function of $\Delta\phi$. The vertical bars are statistical uncertainties, the black boxes are the type B systematic uncertainties, and the gray band around 1.0 on the left is the type C systematic uncertainty. The type B systematics are symmetric around the central value but in some cases are outside the range of the plot. (b) alternative rebinning of the data in (a).
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/Overlay_pp_dAu.png$$y00013 (Color online) The fully-corrected like-sign-subtracted heavy flavor $e$--$\mu$ pair yield in ([red] circles) $\langle N_{\rm coll}\rangle$-scaled \pp ([blue] boxes) \dAu, shifted in $\Delta\phi$ for clarity. The bars are statistical uncertainty. The boxes are the type B systematic uncertainty from the decay and punch-through background subtraction. The overall normalization uncertainties of 16.1\% and 13.4\% in \pp and \dAu, respectively, and 5.7\% uncertainty from $N_{\rm coll}$ are not included.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/Phenix_2008.png$$y00000 (Color online) A schematic view of the PHENIX detector during the 2008 \dAu data taking. (a) beam view of the central spectrometer arms. (b) longitudinal view including the global event and triggering detectors, as well as the muon spectrometer arms. The configurations of the central spectrometer and muon arms were the same for the 2006 \pp data taking.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/PhotonicCorrelations_Run6pp.png$$y00008 The fully-corrected like-sign-subtracted photonic electron-muon $\Delta\phi$ pair yield in (a) \pp and (b) \dAu collisions. Both are consistent with no residual correlation after like-sign subtraction. The solid lines and shaded bands indicate the flat line fits and their uncertainties with $\chi^2$/NDF of 33.2/24 and 20.2/24 in \pp and~\dAu, respectively.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/PhotonicCorrelations_Run8dAu.png$$y00009 The fully-corrected like-sign-subtracted photonic electron-muon $\Delta\phi$ pair yield in (a) \pp and (b) \dAu collisions. Both are consistent with no residual correlation after like-sign subtraction. The solid lines and shaded bands indicate the flat line fits and their uncertainties with $\chi^2$/NDF of 33.2/24 and 20.2/24 in \pp and~\dAu, respectively.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/PunchthroughCorrelation_Run6pp_North.png$$y00004 The fully-corrected like-sign-subtracted electron plus punch-through hadron pair yield in (a) \pp and (b) \dAu collisions. The line indicates the fitted yield that is removed from the inclusive electron-muon pair correlation. The shaded band indicates the fit uncertainty that is propagated as a systematic uncertainty in the final pair yield. In \pp the fit is is a flat line with $\chi^2$/NDF = 22.7/24. In \dAu it is a flat line and a Gaussian centered at $\pi$ with $\chi^2$/NDF = 26.3/22.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/PunchthroughCorrelation_Run8dAu_North.png$$y00005 The fully-corrected like-sign-subtracted electron plus punch-through hadron pair yield in (a) \pp and (b) \dAu collisions. The line indicates the fitted yield that is removed from the inclusive electron-muon pair correlation. The shaded band indicates the fit uncertainty that is propagated as a systematic uncertainty in the final pair yield. In \pp the fit is is a flat line with $\chi^2$/NDF = 22.7/24. In \dAu it is a flat line and a Gaussian centered at $\pi$ with $\chi^2$/NDF = 26.3/22.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/PunchthroughPzDist.png$$y00003 The distribution of $p_z$ for tracks that stop in the next-to-last MuID gap (4th gap). The peak at lower $p_z$ is due to muons, while the broad distribution is from hadrons that punch through the absorber to the 4th gap. The solid line is a two-Gaussian fit to this distribution with the solid line indicating the hadronic background in the muon peak region.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/PythiaPowhegComparison.png$$y00011 (Color online) Comparison of the measured \pp pair yield ([red] points) with heavy flavor production in {\sc powheg} ([blue] dashed line), {\sc pythia} ([black] solid line) and MC@NLO ([green] long dashed line). The $e$--$\mu$ pair yield from the subset of {\sc pythia} events, when the $c\bar{c}$ is not produced at the event vertex is plotted as the dotted [black] line. Each Monte Carlo curve was scaled by a single parameter to match the observed yield. The resulting cross sections are consistent with the previously measured PHENIX results (see Table~\ref{tab:xsect}).
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/dAuLikeUnlikeSB.png$$y00002 (Color online) The fully-corrected inclusive like-sign ($e^{\pm}-\mu^{\pm}$) and unlike-sign ($e^{\pm}-\mu^{\mp}$) distributions for (a) \pp and (b) \dAu, as a function of $\Delta\phi$. The inset shows the unlike-like difference divided by the like-sign distribution, which is the heavy flavor signal-to-background in the inclusive unlike-sign distribution.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/ppLikeUnlikeSB.png$$y00001 (Color online) The fully-corrected inclusive like-sign ($e^{\pm}-\mu^{\pm}$) and unlike-sign ($e^{\pm}-\mu^{\mp}$) distributions for (a) \pp and (b) \dAu, as a function of $\Delta\phi$. The inset shows the unlike-like difference divided by the like-sign distribution, which is the heavy flavor signal-to-background in the inclusive unlike-sign distribution.
000061875 8564_ $$uhttp://inspirehep.net/record/1263517/files/arXiv:1311.1427.pdf
000061875 909CO $$ooai:inspirehep.net:1263517$$pINSPIRE:HEP
000061875 980__ $$aarXiv
000061875 980__ $$aCiteable
000061875 980__ $$aHEP
000061875 980__ $$aCORE
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