Elsevier : Predictions for Cold Nuclear Matter Effects in $p+$Pb Collisions at $\sqrt{s_{_{NN}}} = 8.16$ TeV

Albacete, Javier L.; Zhang, Ben-Wei; Arleo, François; Sapeta, Sebastian; Wang, Xin-Nian; Lappi, Tuomas; Harangozó, Szilvester Miklós; Zhang, Wei-Ning; Eskola, Kari J.; Papp, Gábor; Ru, Peng; Helenius, Ilkka; Vogt, Ramona; Barnaföldi, Gergely G.; Vitev, Ivan; Kotko, Piotr; Ma, Guoyang; Kang, Zhong-Bo; Venugopalan, Raju; Lansberg, Jean Philippe; Schlichting, Sören; Petti, Roberto; Ma, Yan-Qing; Rezaeian, Amir H.; Bíró, Gábor; Zhang, Hong-Fei; d'Enterria, David; Lévai, Péter; Xu, Rong; Schenke, Björn; Mäntysaari, Heikki; Gyulassy, Miklos; Xing, Hongxi; Ferreiro, Elena G.; Paukkunen, Hannu; Kutak, Krzysztof; Lin, Zi-Wei; Shao, Hua-Sheng; Ducloué, Bertrand; Kulagin, Sergey A.; Wang, Enke; Tribedy, Prithwish
doi:10.1016/j.nuclphysa.2017.11.015
002276639 001__ 2276639
002276639 005__ 20240508045845.0
002276639 0248_ $$aoai:cds.cern.ch:2276639$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002276639 0247_ $$2DOI$$9bibmatch$$a10.1016/j.nuclphysa.2017.11.015
002276639 037__ $$9arXiv$$aarXiv:1707.09973$$chep-ph
002276639 035__ $$9arXiv$$aoai:arXiv.org:1707.09973
002276639 035__ $$9Inspire$$aoai:inspirehep.net:1613697$$d2024-05-07T11:27:49Z$$h2024-05-08T02:00:10Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002276639 035__ $$9Inspire$$a1613697
002276639 041__ $$aeng
002276639 100__ $$aAlbacete, Javier L.$$uCAFPE, Granada$$uGranada U., Theor. Phys. Astrophys.$$vCAFPE and Departamento de Física Teórica y del Cosmos, Universidad de Granada E-18071 Campus de Fuentenueva, Granada, Spain
002276639 245__ $$9Elsevier$$aPredictions for Cold Nuclear Matter Effects in $p+$Pb Collisions at $\sqrt{s_{_{NN}}} = 8.16$ TeV
002276639 246__ $$9arXiv$$aPredictions for $p+$Pb Collisions at $\sqrt{s_{_{NN}}} = 8.16$ TeV
002276639 269__ $$c2017-07-31
002276639 260__ $$c2018-04
002276639 300__ $$a68 p
002276639 500__ $$9arXiv$$a84 pages, 44 figures, version accepted for publication in Nuclear Physics A
002276639 520__ $$9Elsevier$$aPredictions for cold nuclear matter effects on charged hadrons, identified light hadrons, quarkonium and heavy flavor hadrons, Drell–Yan dileptons, jets, photons, gauge bosons and top quark pairs produced in p +Pb collisions at sNN=8.16 TeV are compiled and, where possible, compared to each other. Predictions of the normalized ratios of p +Pb to p+p cross sections are also presented for most of the observables, providing new insights into the expected role of cold nuclear matter effects. In particular, the role of nuclear parton distribution functions on particle production can now be probed over a wider range of phase space than ever before.
002276639 520__ $$9arXiv$$aPredictions for cold nuclear matter effects on charged hadrons, identified light hadrons, quarkonium and heavy flavor hadrons, Drell-Yan dileptons, jets, photons, gauge bosons and top quarks produced in $p+$Pb collisions at $\sqrt{s_{_{NN}}} = 8.16$ TeV are compiled and, where possible, compared to each other. Predictions of the normalized ratios of $p+$Pb to $p+p$ cross sections are also presented for most of the observables, providing new insights into the expected role of cold nuclear matter effects. In particular, the role of nuclear parton distribution functions on particle production can now be probed over a wider range of phase space than ever before.
002276639 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002276639 542__ $$fElsevier B.V.
002276639 65017 $$2arXiv$$ahep-ph
002276639 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
002276639 690C_ $$aCERN
002276639 690C_ $$aARTICLE
002276639 700__ $$aArleo, François$$uEcole Polytechnique$$vLaboratoire Leprince-Ringuet, École Polytechnique, CNRS/IN2P3, Université Paris-Saclay, 91128, Palaiseau, France
002276639 700__ $$aBarnaföldi, Gergely G.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, 29-33 Konkoly-Thege Miklós Str, H-1121 Budapest, Hungary
002276639 700__ $$aBíró, Gábor$$uWigner RCP, Budapest$$uEotvos U.$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, 29-33 Konkoly-Thege Miklós Str, H-1121 Budapest, Hungary$$vEötvös Loránd University, 1/A Pázmány P. Sétány, H-1117, Budapest, Hungary
002276639 700__ $$ad'Enterria, David$$uCERN$$vCERN, EP Department, 1211 Geneva, Switzerland
002276639 700__ $$aDucloué, Bertrand$$uJyvaskyla U.$$vDepartment of Physics, University of Jyväskylä, University of Jyväskylä, P.O. Box 35, 40014, Finland$$vHelsinki Institute of Physics, University of Helsinki, P.O. Box 64, 00014, Finland
002276639 700__ $$aEskola, Kari J.$$uJyvaskyla U.$$uHelsinki Inst. of Phys.$$vUniversity of Jyväskyl\"{a$$vHelsinki Institute of Physics, P. O. Box 64, FIN-00014 University of Helsinki, Finland
002276639 700__ $$aFerreiro, Elena G.$$uSantiago de Compostela U., IGFAE$$vDepartamento de Física de Partí
002276639 700__ $$aGyulassy, Miklos$$uWigner RCP, Budapest$$uColumbia U.$$uLBNL, NSD$$uCCNU, Wuhan, Inst. Part. Phys.$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, 29-33 Konkoly-Thege Miklós Str, H-1121 Budapest, Hungary$$vPupin Lab MS-5202, Department of Physics, Columbia University, New York, NY 10027, USA$$vNuclear Science Division, MS 70R0319, Lawrence Berkeley National Laboratory, Berkeley, California 94720 USA$$vInstitute of Particle Physics, Central China Normal University, Wuhan 430079, China
002276639 700__ $$aHarangozó, Szilvester Miklós$$uWigner RCP, Budapest$$uEotvos U.$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, 29-33 Konkoly-Thege Miklós Str, H-1121 Budapest, Hungary$$vEötvös Loránd University, 1/A Pázmány P. Sétány, H-1117, Budapest, Hungary
002276639 700__ $$aHelenius, Ilkka$$uTubingen U.$$vInstitute for Theoretical Physics, Tübingen University, Auf der Morgenstelle 14, 72076 Tübingen, Germany
002276639 700__ $$aKang, Zhong-Bo$$uUCLA$$uLos Alamos Natl. Lab., Theor. Div.$$vDepartment of Physics and Astronomy, University of California, Los Angeles, CA 90095, USA$$vMani L. Bhaumik Institute for Theoretical Physics, University of California, Los Angeles, CA 90095, USA$$vTheoretical Division, MS B283, Los Alamos National Laboratory, Los Alamos, NM 87545, USA
002276639 700__ $$aKotko, Piotr$$uPenn State U.$$vDepartment of Physics, Penn State University, University Park, PA 16803, USA
002276639 700__ $$aKulagin, Sergey A.$$uMoscow, INR$$vInstitute for Nuclear Research of the Russian Academy of Sciences, Moscow 117312, Russia
002276639 700__ $$aKutak, Krzysztof$$uCracow, INP$$vThe H. \ Niewodniczański Institute of Nuclear Physics PAN, Radzikowskiego 152, 31-342 Kraków, Poland
002276639 700__ $$aLansberg, Jean Philippe$$uOrsay, IPN$$vIPNO, Université Paris-Sud, CNRS/IN2P3, Université Paris-Saclay, 91406 Orsay Cedex, France
002276639 700__ $$aLappi, Tuomas$$uJyvaskyla U.$$uHelsinki Inst. of Phys.$$vDepartment of Physics, University of Jyväskylä, University of Jyväskylä, P.O. Box 35, 40014, Finland$$vHelsinki Institute of Physics, University of Helsinki, P.O. Box 64, 00014, Finland
002276639 700__ $$aLévai, Péter$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, 29-33 Konkoly-Thege Miklós Str, H-1121 Budapest, Hungary
002276639 700__ $$aLin, Zi-Wei$$uEast Carolina U.$$vDepartment of Physics, East Carolina University, Greenville, NC 27858, USA
002276639 700__ $$aMa, Guoyang$$uCCNU, Wuhan, Inst. Part. Phys.$$vInstitute of Particle Physics, Central China Normal University, Wuhan 430079, China
002276639 700__ $$aMa, Yan-Qing$$uPeking U., SKLNPT$$uPeking U., CHEP$$vSchool of Physics and State Key Laboratory of Nuclear Physics and Technology, Peking University, Beijing 100871, China$$vCenter for High Energy Physics, Peking University, Beijing 100871, China
002276639 700__ $$aMäntysaari, Heikki$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton, NY 11973, USA
002276639 700__ $$aPaukkunen, Hannu$$uJyvaskyla U.$$uHelsinki Inst. of Phys.$$vUniversity of Jyväskyl\"{a$$vHelsinki Institute of Physics, P. O. Box 64, FIN-00014 University of Helsinki, Finland
002276639 700__ $$aPapp, Gábor$$uEotvos U.$$vEötvös Loránd University, 1/A Pázmány P. Sétány, H-1117, Budapest, Hungary
002276639 700__ $$aPetti, Roberto$$uSouth Carolina U.$$vDepartment of Physics and Astronomy, University of South Carolina, Columbia SC 29208, USA
002276639 700__ $$aRezaeian, Amir H.$$uSanta Maria U., Valparaiso$$uCCTVal, Valparaiso$$vDepartamento de Física, Universidad Técnica Federico Santa María, Avda. España 1680, Casilla 110-V, Valparaíso, Chile$$vCentro Científico Tecnológico de Valparaíso (CCTVal), Universidad Técnica Federico Santa María, Casilla 110-V, Valparaíso, Chile
002276639 700__ $$aRu, Peng$$uDalian U. Tech.$$uCCNU, Wuhan, Inst. Part. Phys.$$vSchool of Physics & Optoelectronic Technology, DalianUniversity of Technology, Dalian, 116024 China$$vInstitute of Particle Physics, Central China Normal University, Wuhan, 430079 China
002276639 700__ $$aSapeta, Sebastian$$uCracow, INP$$vThe H. \ Niewodniczański Institute of Nuclear Physics PAN, Radzikowskiego 152, 31-342 Kraków, Poland
002276639 700__ $$aSchenke, Björn$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton, New York 11973-5000, USA
002276639 700__ $$aSchlichting, Sören$$uWashington U., Seattle$$vDepartment of Physics, University of Washington, Seattle, WA98195-1560, USA
002276639 700__ $$aShao, Hua-Sheng$$uParis, LPTHE$$vSorbonne Universités, UPMC Univ. Paris 06, UMR 7589, LPTHE, F-75005 Paris, France$$vCNRS, UMR 7589, LPTHE, F-75005 Paris, France
002276639 700__ $$aTribedy, Prithwish$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton, New York 11973-5000, USA
002276639 700__ $$aVenugopalan, Raju$$uBrookhaven$$vPhysics Department, Brookhaven National Laboratory, Upton, New York 11973-5000, USA
002276639 700__ $$aVitev, Ivan$$uLos Alamos Natl. Lab., Theor. Div.$$vTheoretical Division, MS B283, Los Alamos National Laboratory, Los Alamos, NM 87545, USA
002276639 700__ $$aVogt, [email protected]$$uLLNL, Livermore$$uUC, Davis$$vPhysics Division, Lawrence Livermore National Laboratory, Livermore, CA 94551, USA
002276639 700__ $$aWang, Enke$$uHua-Zhong Normal U., LQLP$$uCCNU, Wuhan, Inst. Part. Phys.$$vKey Laboratory of Quarks and Lepton Physics (MOE), Institute of Particle Physics, Central China Normal University, Wuhan, 430079, China
002276639 700__ $$aWang, Xin-Nian$$uLBNL, NSD$$uCCNU, Wuhan, Inst. Part. Phys.$$vNuclear Science Division, MS 70R0319, Lawrence Berkeley National Laboratory, Berkeley, California 94720 USA$$vInstitute of Particle Physics, Central China Normal University, Wuhan 430079, China
002276639 700__ $$aXing, Hongxi$$uNorthwestern U.$$uArgonne$$vDepartment of Physics and Astronomy, Northwestern University, Evanston, IL 60208, USA$$vHigh Energy Physics Division, Argonne National Laboratory, Argonne, IL 60439, USA
002276639 700__ $$aXu, Rong$$uCCNU, Wuhan, Inst. Part. Phys.$$uHua-Zhong Normal U., LQLP$$vKey Laboratory of Quark and Lepton Physics (MOE) and Institute of Particle Physics, Central China Normal University, Wuhan 430079, China
002276639 700__ $$aZhang, Ben-Wei$$uCCNU, Wuhan, Inst. Part. Phys.$$uHua-Zhong Normal U., LQLP$$vKey Laboratory of Quarks and Lepton Physics (MOE), Institute of Particle Physics, Central China Normal University, Wuhan, 430079, China
002276639 700__ $$aZhang, Hong-Fei$$uCUPT, Chongqing$$vSchool of Science, Chongqing University of Posts and Telecommunications, Chongqing 400065, China
002276639 700__ $$aZhang, Wei-Ning$$uHarbin Inst. Tech.$$vPhysics Department, HarbinInstitute of Technology, Harbin 150006, China
002276639 773__ $$c18-85$$pNucl. Phys. A$$v972$$y2018
002276639 8564_ $$82226800$$s16916$$uhttp://cds.cern.ch/record/2276639/files/v2pt8_Ziwei.png$$y00023 (Color online) The $v_2\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from $\mathtt{AMPT-SM}$ at 5~TeV (a) and 8~TeV (b). The 5~TeV results in the (0-5)\% centrality range from $\mathtt{AMPT-SM}$ versions 2.26t7 (solid blue) and 2.26t1 (dashed magenta) are compared to each other and to the CMS 5~TeV $p+$Pb data \protect\cite{Chatrchyan:2013nka} in (a). In (b), the $\mathtt{AMPT-SM}$ version 2.26t7 calculations at 8~TeV for (0-5)\% (solid red) and (0-20)\% (dashed black) are shown.
002276639 8564_ $$82226801$$s12132$$uhttp://cds.cern.ch/record/2276639/files/cRpPb_EPPS16_CT14_y_top.png$$y00065 (Color online) Nuclear modification factors as a function of transverse momentum (left) and rapidity (right) for $t \overline t$ production in the $\ell$+jets channel at $\sqrt{s_{_{NN}}} = 8.16$~TeV for: the produced top quarks, (a) and (b), their isolated decay leptons, (c) and (d), and their $b$-jet decays, (e) and (f), obtained at NLO accuracy with the central sets of CT14+EPPS16 (dashed curves) and CT10+EPS09 (solid curves).
002276639 8564_ $$82226802$$s25587$$uhttp://cds.cern.ch/record/2276639/files/v2pt_Ziwei.png$$y00021 (Color online) $v_2\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from string melting $\mathtt{AMPT}$.
002276639 8564_ $$82226803$$s32835$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-pPb.png$$y00003 (Color online) The IP-Glasma prediction for the charged hadron multiplicity distribution in $p+p$ collisions at 7 TeV (a) and $p+$Pb collisions at 5.02 and 8~TeV (b) are shown. The ALICE data for $|\eta| &lt; 1$ in 7 TeV $p+p$ collisions \protect\cite{Aamodt:2010pp} and the CMS data for $|\eta|&lt;2.4$ in 5.02 TeV $p+$Pb collisions \protect\cite{CMS:2012qk} are shown in red. The corresponding IP-Glasma calculations are shown in black while the 8 TeV $p+$Pb predictions are given in blue.
002276639 8564_ $$82226804$$s1755798$$uhttp://cds.cern.ch/record/2276639/files/arXiv:1707.09973.pdf
002276639 8564_ $$82226805$$s11454$$uhttp://cds.cern.ch/record/2276639/files/cRpPb_EPPS16_CT14_pT_bjet.png$$y00068 (Color online) Nuclear modification factors as a function of transverse momentum (left) and rapidity (right) for $t \overline t$ production in the $\ell$+jets channel at $\sqrt{s_{_{NN}}} = 8.16$~TeV for: the produced top quarks, (a) and (b), their isolated decay leptons, (c) and (d), and their $b$-jet decays, (e) and (f), obtained at NLO accuracy with the central sets of CT14+EPPS16 (dashed curves) and CT10+EPS09 (solid curves).
002276639 8564_ $$82226806$$s105013$$uhttp://cds.cern.ch/record/2276639/files/dy_ppb_8160_npdf_nlo.png$$y00051 (Color online) The Drell-Yan nuclear suppression factor in $p+$Pb collisions at $\sqrt{s_{_{NN}}}=8.16$~TeV for the DSSZ (magenta), EPS09 (blue), nCTEQ15 (red) and isospin only (black line) \protect\cite{Arleo:2015qiv}.
002276639 8564_ $$82226807$$s18733$$uhttp://cds.cern.ch/record/2276639/files/ups_all_midY_pT.png$$y00039 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $\Upsilon$ at midrapidity as a function of transverse momentum at 8~TeV. The EPS09 NLO results of Vogt (dot-dot-dash-dashed red curve) and Lansberg and Shao (solid cyan) are shown with their results for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) at midrapidity.
002276639 8564_ $$82226808$$s19668$$uhttp://cds.cern.ch/record/2276639/files/v2pt5_Ziwei.png$$y00022 (Color online) The $v_2\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from $\mathtt{AMPT-SM}$ at 5~TeV (a) and 8~TeV (b). The 5~TeV results in the (0-5)\% centrality range from $\mathtt{AMPT-SM}$ versions 2.26t7 (solid blue) and 2.26t1 (dashed magenta) are compared to each other and to the CMS 5~TeV $p+$Pb data \protect\cite{Chatrchyan:2013nka} in (a). In (b), the $\mathtt{AMPT-SM}$ version 2.26t7 calculations at 8~TeV for (0-5)\% (solid red) and (0-20)\% (dashed black) are shown.
002276639 8564_ $$82226809$$s14042$$uhttp://cds.cern.ch/record/2276639/files/v4pt8_Ziwei.png$$y00027 (Color online) The $v_4\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from $\mathtt{AMPT-SM}$ at 5~TeV (a) and 8~TeV (b). The 5~TeV results in the (0-5)\% centrality range from $\mathtt{AMPT-SM}$ versions 2.26t7 (solid blue) and 2.26t1 (dashed magenta) are compared in (a). In (b), the $\mathtt{AMPT-SM}$ version 2.26t7 calculations at 8~TeV for (0-5)\% (solid red) and (0-20)\% (dashed black) are shown.
002276639 8564_ $$82226810$$s6660$$uhttp://cds.cern.ch/record/2276639/files/RpA-ptmax8TeV.png$$y00053 (Color online) The blue lines correspond to predictions obtained with the KS gluon density~\protect\cite{Kutak:2012rf} while the red lines are predictions using a hard-scale-dependent gluon density \protect\cite{Kutak:2014wga} at 8~TeV. In both cases, the renormalization and factorization scales are set to $\mu= (p_{T,1}+p_{T,2})/2$. The light red bands illustrate the scale variation by factors of 0.5 and 2 for the ``KS nonlinear + hard scale'' result. The analogous variation for the pure KS gluon gives a negligible effect. The suppression factor for the hardest jet is shown in (a) while that for the subleading jet is shown in (b). The nuclear modification factor as a function of azimuthal angle between jets is given in (c).
002276639 8564_ $$82226811$$s10458$$uhttp://cds.cern.ch/record/2276639/files/plot_nPDFs_highx_nice.png$$y00063 (Color online) Ratio of the lead-to-proton gluon densities in the antishadowing ($x \approx 0.05-0.1$) and EMC ($x\approx 0.1-0.6$) regions probed by $t \overline t$ production at virtualities $Q^2= m_t^2\approx 3\times 10^{4}$~GeV$^2$ in $p+$Pb collisions at the LHC, for three different NLO nuclear PDF sets: EPS09~\cite{Eskola:2009uj} (red), DSSZ~\cite{deFlorian:2011fp} (yellow), and FGS10~\cite{Frankfurt:2011cs} (blue).
002276639 8564_ $$82226812$$s20001$$uhttp://cds.cern.ch/record/2276639/files/psi_all_midY_pT_c.png$$y00034 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of transverse momentum at 8~TeV. The EPS09 NLO results of Vogt (dot-dot-dash-dashed red curve) and Lansberg and Shao (solid cyan) are shown with their results for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) at backward (a), forward (b), and mid (c) rapidity. The ALICE data \protect\cite{Enrico} at backward and forward rapidity are shown in black in (a) and (b) while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226813$$s20486$$uhttp://cds.cern.ch/record/2276639/files/Bp_ydist.png$$y00048 (Color online) Prediction for $B$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions as a function of rapidity at 8~TeV. The data-driven shadowing results of Lansberg and Shao are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram). The $\mathtt{HIJING++}$ calculations are the red points.
002276639 8564_ $$82226814$$s11526$$uhttp://cds.cern.ch/record/2276639/files/cRpPb_EPPS16_CT14_pT_top.png$$y00064 (Color online) Nuclear modification factors as a function of transverse momentum (left) and rapidity (right) for $t \overline t$ production in the $\ell$+jets channel at $\sqrt{s_{_{NN}}} = 8.16$~TeV for: the produced top quarks, (a) and (b), their isolated decay leptons, (c) and (d), and their $b$-jet decays, (e) and (f), obtained at NLO accuracy with the central sets of CT14+EPPS16 (dashed curves) and CT10+EPS09 (solid curves).
002276639 8564_ $$82226815$$s21976$$uhttp://cds.cern.ch/record/2276639/files/dndpt-K-HIJING++_a.png$$y00013 (Color online) The $p_T$ spectra of charged kaons (a) and protons (b) in 8~TeV $p+p$ and $p+$Pb collisions. In both cases the solid curves are the $p+$Pb results while the $p+p$ results for $\mathtt{HIJING++}$ and $\mathtt{PYTHIA8}$ are given by the dashed and dot-dashed curves respectively.
002276639 8564_ $$82226816$$s8540$$uhttp://cds.cern.ch/record/2276639/files/photons_highpT_b.png$$y00057 (Color online) Prediction for direct photon $R_{p{\rm Pb}}$ in $p+$Pb collisions at midrapidity for $p_T &lt; 30$~GeV (a) and $p_T &gt; 50$~GeV (b) in 8~TeV collisions. Results with Cronin broadening alone (solid) and with energy loss: full Cronin and moderate energy loss (dashed) and reduced Cronin but stronger energy loss (dot-dashed), are shown.
002276639 8564_ $$82226817$$s18119$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-MB_lab_a.png$$y00000 (Color online) The charged particle multiplicity distribution $dN_{\rm ch}/d\eta$ at $\sqrt{s_{NN}} = 8$~TeV from $\mathtt{AMPT}$ (solid blue), rcBK from Albacete and Dumitru (black dot dashed), bCGC from Rezaeian (blue dashed), and $\mathtt{HIJING++}$ (dashed red) in the laboratory (a) and center-of-mass (b) frames. The $\mathtt{AMPT}$ result is in the lab frame while the $\mathtt{HIJING++}$ calculation and the rcBK result from Albacete and Dumitru are given in both frames.
002276639 8564_ $$82226818$$s5976$$uhttp://cds.cern.ch/record/2276639/files/RpA-ptmin8TeV.png$$y00054 (Color online) The blue lines correspond to predictions obtained with the KS gluon density~\protect\cite{Kutak:2012rf} while the red lines are predictions using a hard-scale-dependent gluon density \protect\cite{Kutak:2014wga} at 8~TeV. In both cases, the renormalization and factorization scales are set to $\mu= (p_{T,1}+p_{T,2})/2$. The light red bands illustrate the scale variation by factors of 0.5 and 2 for the ``KS nonlinear + hard scale'' result. The analogous variation for the pure KS gluon gives a negligible effect. The suppression factor for the hardest jet is shown in (a) while that for the subleading jet is shown in (b). The nuclear modification factor as a function of azimuthal angle between jets is given in (c).
002276639 8564_ $$82226819$$s8687$$uhttp://cds.cern.ch/record/2276639/files/ups_eps09nlo_y_a.png$$y00037 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $\Upsilon$ as a function of rapidity at 8~TeV. (a) The EPS09 NLO result is compared between the NLO CEM calculation of Vogt (dot-dot-dash-dashed red curve) and the data-driven result of Lansberg and Shao (solid cyan). (b) The data-driven calculation of Lansberg and Shao for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) is compared to the energy loss only calculation of Arleo (dot-dashed red curve).
002276639 8564_ $$82226820$$s29897$$uhttp://cds.cern.ch/record/2276639/files/dndpt-p-HIJING++_b.png$$y00014 (Color online) The $p_T$ spectra of charged kaons (a) and protons (b) in 8~TeV $p+p$ and $p+$Pb collisions. In both cases the solid curves are the $p+$Pb results while the $p+p$ results for $\mathtt{HIJING++}$ and $\mathtt{PYTHIA8}$ are given by the dashed and dot-dashed curves respectively.
002276639 8564_ $$82226821$$s17980$$uhttp://cds.cern.ch/record/2276639/files/psi_forY_pT_8vs5_b.png$$y00036 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of $p_T$ at 5 TeV (blue points and solid blue curves) and 8 TeV (red points and dashes red curves) calculated with EPS09 NLO are compared. The data from ALICE at 5 TeV \protect\cite{ALICE_psi_pT} and 8 TeV \protect\cite{Enrico} are also shown at backward rapidity (a) and forward rapidity (b).
002276639 8564_ $$82226822$$s19902$$uhttp://cds.cern.ch/record/2276639/files/psi_y_8vs5_eloss_b.png$$y00031 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of rapidity at 5 TeV (blue points and solid blue curves) and 8 TeV (red points and dashed red curves) are compared. The data from ALICE at 5 TeV \protect\cite{ALICE_psiy5} and 8 TeV \protect\cite{Enrico} are also shown. (a) The EPS09 NLO CEM result. (b) The energy loss calculation by Arleo.
002276639 8564_ $$82226823$$s27132$$uhttp://cds.cern.ch/record/2276639/files/psi_other_y_data_b.png$$y00029 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of rapidity at 8~TeV. (a) The EPS09 NLO result is compared between the NLO CEM calculation of Vogt (dot-dot-dash-dashed red curve) and the data-driven result of Lansberg and Shao (solid cyan). (b) The data-driven calculation of Lansberg and Shao for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) is compared to the energy loss only calculation of Arleo (dot-dashed red curve). The $\mathtt{HIJING++}$ calculations are shown by the red points. The ALICE data \protect\cite{Enrico} are shown in black while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226824$$s19476$$uhttp://cds.cern.ch/record/2276639/files/psi_y_8vs5_a.png$$y00030 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of rapidity at 5 TeV (blue points and solid blue curves) and 8 TeV (red points and dashed red curves) are compared. The data from ALICE at 5 TeV \protect\cite{ALICE_psiy5} and 8 TeV \protect\cite{Enrico} are also shown. (a) The EPS09 NLO CEM result. (b) The energy loss calculation by Arleo.
002276639 8564_ $$82226825$$s20318$$uhttp://cds.cern.ch/record/2276639/files/psi_eps09nlo_y_data_a.png$$y00028 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of rapidity at 8~TeV. (a) The EPS09 NLO result is compared between the NLO CEM calculation of Vogt (dot-dot-dash-dashed red curve) and the data-driven result of Lansberg and Shao (solid cyan). (b) The data-driven calculation of Lansberg and Shao for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) is compared to the energy loss only calculation of Arleo (dot-dashed red curve). The $\mathtt{HIJING++}$ calculations are shown by the red points. The ALICE data \protect\cite{Enrico} are shown in black while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226826$$s42758$$uhttp://cds.cern.ch/record/2276639/files/wcms8etaKPr.png$$y00058 (Color online) The differential cross section as a function of the charged lepton pseudorapidity for $W^+$~(a) and $W^-$~(b) production in $p+$Pb collisions at 8~TeV for EPS09 (red circles), nCTEQ (green squares) and KP (blue stars). The corresponding $R_{p{\rm Pb}}$ calculations are shown in (c) and (d) respectively, along with the nuclear modification factor due to isospin alone, with CT10 (red dashes) and ABMP15 (blue dot-dashed). The range of the charged-lepton transverse momentum is $p_T^l&gt;25$~GeV~\protect\cite{Khachatryan:2015hha}.
002276639 8564_ $$82226827$$s27731$$uhttp://cds.cern.ch/record/2276639/files/dndpt_pPb_kTpQCD_HIJING_b.png$$y00012 (Color online) The $p_T$ spectra of charged pions from $\mathtt{kTpQCD}$ and $\mathtt{HIJING++}$ in $p+p$ (a) and $p+$Pb (b) collisions, both at 8~TeV. The $p+p$ results from $\mathtt{HIJING++}$, $\mathtt{PYTHIA8}$ and $\mathtt{kTpQCD}$ are given by the red dashed, red dot-dashed and blue dot-dashed curves respectively in (a). The $p+$Pb results from $\mathtt{HIJING++}$ and $\mathtt{kTpQCD}$ are given by the red solid and blue dashed curves respectively. The $\mathtt{AMPT-SM}$ non-diffractive $p+$Pb result for charged hadrons at 8 TeV is given by the black dashed curve in (b).
002276639 8564_ $$82226828$$s9440$$uhttp://cds.cern.ch/record/2276639/files/rpPb_ch_mid_CGC.png$$y00016 (Color online) Charged hadron $R_{p {\rm Pb}}$ as a function of $p_T$ at midrapidity in 8~TeV collisions. The central EPS09 NLO result from Fig.~\protect\ref{fig:RpPbEPS09} is shown in the solid blue curve. The dashed blue curves show the uncertainty in the low $p_T$ region. The midrapidity CGC calculation by Lappi and M\"antysaari is given in the dot-dashed red curve. The results by Rezaeian are given in the dot-dot-dot-dashed black curves.
002276639 8564_ $$82226829$$s22085$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-MB_cm_b.png$$y00001 (Color online) The charged particle multiplicity distribution $dN_{\rm ch}/d\eta$ at $\sqrt{s_{NN}} = 8$~TeV from $\mathtt{AMPT}$ (solid blue), rcBK from Albacete and Dumitru (black dot dashed), bCGC from Rezaeian (blue dashed), and $\mathtt{HIJING++}$ (dashed red) in the laboratory (a) and center-of-mass (b) frames. The $\mathtt{AMPT}$ result is in the lab frame while the $\mathtt{HIJING++}$ calculation and the rcBK result from Albacete and Dumitru are given in both frames.
002276639 8564_ $$82226830$$s22913$$uhttp://cds.cern.ch/record/2276639/files/rpPb_ch_mid2.png$$y00018 (Color online) Charged hadron $R_{p {\rm Pb}}$ as a function of $p_T$ at midrapidity in 8~TeV collisions are shown for $\mathtt{HIJING++}$ (black dashed histogram) and two parameterizations in $\mathtt{kTpQCD\_v21}$ (EPS09, magenta curve, and the $\mathtt{HIJING}$ shadowing parameterization, red curve). Estimated uncertainties are also shown for the last two calculations. The central EPS09 NLO calculation by Eskola (solid blue curve) is also shown.
002276639 8564_ $$82226831$$s44078$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-5TeV-AMPT-ATLAS.png$$y00006 (Color online) The new $\mathtt{AMPT-SM}$ charged hadron multiplicity distribution, $dN_{\rm ch}/d\eta$, at 5 TeV (in blue) is compared to the ATLAS data (black points) \protect\cite{Aad:2015zza} in the same centrality bins: (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\% and (60-90)\%.
002276639 8564_ $$82226832$$s29745$$uhttp://cds.cern.ch/record/2276639/files/dndpt-ch-HIJING++_b.png$$y00010 (Color online) The $p_T$ spectra of charged pions at 8~TeV from $\mathtt{kTpQCD}$ is given in (a) with the $p+$Pb results with EPS09 NLO and the HIJING shadowing parameterization given by the solid and dashed curves respectively while the $p+p$ result is shown in the dot-dashed curve. The $\mathtt{HIJING++}$ 8~TeV results are given in (b) for $p+$Pb (solid curve) and $p+p$ (dashed curve) while the $\mathtt{PYTHIA8}$ result is shown in the dot-dashed curve.
002276639 8564_ $$82226833$$s24578$$uhttp://cds.cern.ch/record/2276639/files/Bp_forwardy_b.png$$y00050 (Color online) Prediction for $B$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions at midrapidity (a) and forward rapidity (b) at 8~TeV. The data-driven shadowing results of Lansberg and Shao are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram). Results with Cronin broadening alone (solid red) and with energy loss (full Cronin and moderate energy loss, red dashed, reduced Cronin and stronger energy loss, red dot dashed) are also shown.
002276639 8564_ $$82226834$$s20179$$uhttp://cds.cern.ch/record/2276639/files/jets_midy.png$$y00052 (Color online) Prediction for single jet $R_{p{\rm Pb}}$ in $p+$Pb collisions at mid ($y=0$) and forward ($y=4$) rapidity at 8~TeV. Results with Cronin broadening alone (solid) and with energy loss (full Cronin and moderate energy loss, dashed, and reduced Cronin and stronger energy loss, dot dashed) are shown. The midrapidity ratios are given in red and the $y = 4$ results for $p_T &gt; 20$ GeV are shown in blue.
002276639 8564_ $$82226835$$s14305$$uhttp://cds.cern.ch/record/2276639/files/z0cms8ppbfbasy.png$$y00061 (Color online) The forward-backward asymmetry for $Z^0$ production at 8~TeV. The nPDF esults are shown for EPS09 (red circles), nCTEQ (yellow squares) and KP (blue stars) while calculations with isospin alone are shown for CT10 (red dashes) and ABMP15 (blue dot-dashed).
002276639 8564_ $$82226836$$s22285$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-5TeV-AMPT.png$$y00005 (Color online) The charged hadron multiplicity distribution, $dN_{\rm ch}/d\eta$, in 5 TeV $p+$Pb collisions at different centralities from $\mathtt{AMPT-SM}$ are shown in the laboratory frame. The previous prediction for minimum-bias events at 5 TeV (cyan points and line) is shown for comparison. The blue lines, from top to bottom are for centralities of (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\%, (60-90)\% and (90-100)\%. The red points and line shows the previous $\mathtt{AMPT}$ result for the 5 TeV non-diffractive multiplicity. The red and cyan curves are somewhat different in shape but similar in magnitude.
002276639 8564_ $$82226837$$s28878$$uhttp://cds.cern.ch/record/2276639/files/dndpt-ch-AMPT.png$$y00008 (Color online) The $p_T$ spectra of charged hadrons per collision in $p+$Pb collisions at both 5 and 8~TeV from $\mathtt{AMPT-SM}$. The previous 5~TeV result is given by the magenta dot-dash-dash-dashed curve while the current 5~TeV non-diffractive result is given by the solid blue curve. The non-diffractive and (0-5)\% most central results at 8~TeV are given by the black dashed and red dot-dashed curves respectively.
002276639 8564_ $$82226838$$s19471$$uhttp://cds.cern.ch/record/2276639/files/rpPb_ch_Ivan.png$$y00021 (Color online) Charged hadron $R_{pA}$ as a function of $p_T$ at mid ($y=0$, blue) and forward rapidity ($y=4$, red) in 8~TeV collisions. The calculations by Vitev {\it et al.}\ are shown for Cronin only (solid), with moderate energy loss (dashed) and moderate Cronin with full energy loss (dot-dashed).
002276639 8564_ $$82226839$$s10900$$uhttp://cds.cern.ch/record/2276639/files/rpPb_ch_for.png$$y00020 (Color online) Charged hadron $R_{pA}$ as a function of $p_T$ at forward rapidity in 8~TeV collisions. The rcBK results are shown in magenta for $y = 3$ (solid), 4 (dashed) and 5 (dot-dashed). The calculations by Vitev {\it et al.}\ at $y = 4$ are shown in red for Cronin only (solid), with moderate energy loss (dashed) and moderate Cronin with full energy loss (dot-dashed).
002276639 8564_ $$82226840$$s18174$$uhttp://cds.cern.ch/record/2276639/files/D0_ydist.png$$y00044 (Color online) Prediction for $D$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions at 8~TeV as a function of rapidity. The data-driven shadowing results of Lansberg and Shao are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram). The $\mathtt{HIJING++}$ calculations are the red points.
002276639 8564_ $$82226841$$s44797$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-5TeV-AMPT-ATLAScent.png$$y00007 (Color online) The new $\mathtt{AMPT-SM}$ charged hadron multiplicity distribution, $dN_{\rm ch}/d\eta$, at 5 TeV (in blue) is compared to the ATLAS data (black points) \protect\cite{Aad:2015zza} in the same centrality bins: (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\% and (60-90)\%.
002276639 8564_ $$82226842$$s25400$$uhttp://cds.cern.ch/record/2276639/files/psi_all_forY_pT_data_b.png$$y00033 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of transverse momentum at 8~TeV. The EPS09 NLO results of Vogt (dot-dot-dash-dashed red curve) and Lansberg and Shao (solid cyan) are shown with their results for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) at backward (a), forward (b), and mid (c) rapidity. The ALICE data \protect\cite{Enrico} at backward and forward rapidity are shown in black in (a) and (b) while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226843$$s26144$$uhttp://cds.cern.ch/record/2276639/files/psi_all_bckY_pT_data_a.png$$y00032 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of transverse momentum at 8~TeV. The EPS09 NLO results of Vogt (dot-dot-dash-dashed red curve) and Lansberg and Shao (solid cyan) are shown with their results for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) at backward (a), forward (b), and mid (c) rapidity. The ALICE data \protect\cite{Enrico} at backward and forward rapidity are shown in black in (a) and (b) while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226844$$s16865$$uhttp://cds.cern.ch/record/2276639/files/psi_cgc_y_data_a.png$$y00042 (Color online) Nuclear suppression factor for $J/\psi$ production at 8~TeV by Douclou\'e {\it et al.} \protect\cite{Ducloue:2016pqr} (red dashed curves) and by Ma {\it et al.} \protect\cite{Ma:2015sia} (solid blue curves). (a) The rapidity dependence. (b) The transverse momentum dependence. The ALICE data \protect\cite{Enrico} are shown in black while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226845$$s17145$$uhttp://cds.cern.ch/record/2276639/files/v3pt5_Ziwei.png$$y00024 (Color online) The $v_3\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from $\mathtt{AMPT-SM}$ at 5~TeV (a) and 8~TeV (b). The 5~TeV results in the (0-5)\% centrality range from $\mathtt{AMPT-SM}$ versions 2.26t7 (solid blue) and 2.26t1 (dashed magenta) are compared to each other and to the CMS 5~TeV $p+$Pb data \protect\cite{Chatrchyan:2013nka} in (a). In (b), the $\mathtt{AMPT-SM}$ version 2.26t7 calculations at 8~TeV for (0-5)\% (solid red) and (0-20)\% (dashed black) are shown.
002276639 8564_ $$82226846$$s11806$$uhttp://cds.cern.ch/record/2276639/files/cRpPb_EPPS16_CT14_y_lept.png$$y00067 (Color online) Nuclear modification factors as a function of transverse momentum (left) and rapidity (right) for $t \overline t$ production in the $\ell$+jets channel at $\sqrt{s_{_{NN}}} = 8.16$~TeV for: the produced top quarks, (a) and (b), their isolated decay leptons, (c) and (d), and their $b$-jet decays, (e) and (f), obtained at NLO accuracy with the central sets of CT14+EPPS16 (dashed curves) and CT10+EPS09 (solid curves).
002276639 8564_ $$82226847$$s25525$$uhttp://cds.cern.ch/record/2276639/files/dndpt-ch-kTpQCD_a.png$$y00009 (Color online) The $p_T$ spectra of charged pions at 8~TeV from $\mathtt{kTpQCD}$ is given in (a) with the $p+$Pb results with EPS09 NLO and the HIJING shadowing parameterization given by the solid and dashed curves respectively while the $p+p$ result is shown in the dot-dashed curve. The $\mathtt{HIJING++}$ 8~TeV results are given in (b) for $p+$Pb (solid curve) and $p+p$ (dashed curve) while the $\mathtt{PYTHIA8}$ result is shown in the dot-dashed curve.
002276639 8564_ $$82226848$$s15145$$uhttp://cds.cern.ch/record/2276639/files/RpA-dphi8TeV.png$$y00055 (Color online) The blue lines correspond to predictions obtained with the KS gluon density~\protect\cite{Kutak:2012rf} while the red lines are predictions using a hard-scale-dependent gluon density \protect\cite{Kutak:2014wga} at 8~TeV. In both cases, the renormalization and factorization scales are set to $\mu= (p_{T,1}+p_{T,2})/2$. The light red bands illustrate the scale variation by factors of 0.5 and 2 for the ``KS nonlinear + hard scale'' result. The analogous variation for the pure KS gluon gives a negligible effect. The suppression factor for the hardest jet is shown in (a) while that for the subleading jet is shown in (b). The nuclear modification factor as a function of azimuthal angle between jets is given in (c).
002276639 8564_ $$82226849$$s27431$$uhttp://cds.cern.ch/record/2276639/files/dndpt_kTpQCD_HIJING_a.png$$y00011 (Color online) The $p_T$ spectra of charged pions from $\mathtt{kTpQCD}$ and $\mathtt{HIJING++}$ in $p+p$ (a) and $p+$Pb (b) collisions, both at 8~TeV. The $p+p$ results from $\mathtt{HIJING++}$, $\mathtt{PYTHIA8}$ and $\mathtt{kTpQCD}$ are given by the red dashed, red dot-dashed and blue dot-dashed curves respectively in (a). The $p+$Pb results from $\mathtt{HIJING++}$ and $\mathtt{kTpQCD}$ are given by the red solid and blue dashed curves respectively. The $\mathtt{AMPT-SM}$ non-diffractive $p+$Pb result for charged hadrons at 8 TeV is given by the black dashed curve in (b).
002276639 8564_ $$82226850$$s37507$$uhttp://cds.cern.ch/record/2276639/files/wcms8eta.png$$y00054 (Color online) The differential cross section as a function of the charged lepton pseudorapidity for $W^+$~(a) and $W^-$~(b) production. The ratios of each result to the corresponding baseline calculation are shown in (c) and (d) respectively. The range of the charged-lepton transverse momentum is $p_T^l&gt;25$~GeV~\protect\cite{Khachatryan:2015hha}.
002276639 8564_ $$82226851$$s22207$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-pp.png$$y00002 (Color online) The IP-Glasma prediction for the charged hadron multiplicity distribution in $p+p$ collisions at 7 TeV (a) and $p+$Pb collisions at 5.02 and 8~TeV (b) are shown. The ALICE data for $|\eta| &lt; 1$ in 7 TeV $p+p$ collisions \protect\cite{Aamodt:2010pp} and the CMS data for $|\eta|&lt;2.4$ in 5.02 TeV $p+$Pb collisions \protect\cite{CMS:2012qk} are shown in red. The corresponding IP-Glasma calculations are shown in black while the 8 TeV $p+$Pb predictions are given in blue.
002276639 8564_ $$82226852$$s25634$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-8TeV-AMPT-ATLAScent.png$$y00004 (Color online) The charged hadron multiplicity, $dN_{\rm ch}/d\eta$, in 8 TeV $p+$Pb collisions at different centralities calculated with $\mathtt{AMPT-SM}$ are shown. The result for all non-diffractive events at 5 TeV (red points and line) is also shown for comparison. The blue lines, from top to bottom are for centralities of (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\%, (60-90)\% and (90-100)\%. The blue points and line shows the 8 TeV non-diffractive multiplicity. The 8~TeV non-diffractive multiplicity is very similar to the calculation in the (40-60)\% centrality bin. The results in (a) are for the ATLAS centrality definition, $\langle E_T \rangle(-4.9 &lt; \eta_{\rm lab} &lt; -3.1)$ \protect\cite{Aad:2015zza}, while the results in (b) use the centrality definition based on charged particle multiplicity in the central region $\langle N_{\rm ch} \rangle(|\eta_{\rm lab}|&lt;2.4)$.
002276639 8564_ $$82226853$$s18044$$uhttp://cds.cern.ch/record/2276639/files/rpPb_PID_mid.png$$y00019 (Color online) Charged hadron $R_{pA}$ as a function of $p_T$ at midrapidity in 8~TeV collisions are shown for $\mathtt{HIJING++}$ calculations of charged pions (solid red histogram), charged kaons (dashed black histogram) and protons/antiprotons (dot-dashed blue histogram).
002276639 8564_ $$82226854$$s6054$$uhttp://cds.cern.ch/record/2276639/files/RpPbvsy8TeV.png$$y00040 (Color online) The $J/\psi$ (blue lines) and $\psi(2{\rm S})$ (red lines) nuclear modification factor $R_{p{\rm Pb}}$ as a function of rapidity at 5.02~TeV (dashed lines) and 8.16~TeV (solid lines).
002276639 8564_ $$82226855$$s11916$$uhttp://cds.cern.ch/record/2276639/files/cRpPb_EPPS16_CT14_pT_lept.png$$y00066 (Color online) Nuclear modification factors as a function of transverse momentum (left) and rapidity (right) for $t \overline t$ production in the $\ell$+jets channel at $\sqrt{s_{_{NN}}} = 8.16$~TeV for: the produced top quarks, (a) and (b), their isolated decay leptons, (c) and (d), and their $b$-jet decays, (e) and (f), obtained at NLO accuracy with the central sets of CT14+EPPS16 (dashed curves) and CT10+EPS09 (solid curves).
002276639 8564_ $$82226856$$s22865$$uhttp://cds.cern.ch/record/2276639/files/z0cms8ppbnlopt.png$$y00058 (Color online) (a) The differential cross section as a function of $Z^0$ transverse momentum. (b) The ratios of each result and the corresponding baseline. The $Z^0$ mass window $60&lt;m_Z&lt;120$~GeV and rapidity interval $-2.5&lt;y^Z_{\rm cm}&lt;1.5$~\cite{CMS:2014sca} are used in the calculations.
002276639 8564_ $$82226857$$s16639$$uhttp://cds.cern.ch/record/2276639/files/v4pt5_Ziwei.png$$y00026 (Color online) The $v_4\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from $\mathtt{AMPT-SM}$ at 5~TeV (a) and 8~TeV (b). The 5~TeV results in the (0-5)\% centrality range from $\mathtt{AMPT-SM}$ versions 2.26t7 (solid blue) and 2.26t1 (dashed magenta) are compared in (a). In (b), the $\mathtt{AMPT-SM}$ version 2.26t7 calculations at 8~TeV for (0-5)\% (solid red) and (0-20)\% (dashed black) are shown.
002276639 8564_ $$82226858$$s22817$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-5TeV-AMPT-cent.png$$y00006 (Color online) The charged hadron multiplicity distribution, $dN_{\rm ch}/d\eta$, in 5 TeV $p+$Pb collisions at different centralities from $\mathtt{AMPT-SM}$ are shown in the laboratory frame. The previous prediction for minimum-bias events at 5 TeV (cyan points and line) is shown for comparison. The blue lines, from top to bottom are for centralities of (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\%, (60-90)\% and (90-100)\%. The red points and line shows the previous $\mathtt{AMPT}$ result for the 5 TeV non-diffractive multiplicity. The red and cyan curves are somewhat different in shape but similar in magnitude. The results in are for the ATLAS centrality definition, $\langle E_T \rangle(-4.9 &lt; \eta_{\rm lab} &lt; -3.1)$ \cite{Aad:2015zza}.
002276639 8564_ $$82226859$$s11578$$uhttp://cds.cern.ch/record/2276639/files/cRpPb_EPPS16_CT14_y_bjet.png$$y00069 (Color online) Nuclear modification factors as a function of transverse momentum (left) and rapidity (right) for $t \overline t$ production in the $\ell$+jets channel at $\sqrt{s_{_{NN}}} = 8.16$~TeV for: the produced top quarks, (a) and (b), their isolated decay leptons, (c) and (d), and their $b$-jet decays, (e) and (f), obtained at NLO accuracy with the central sets of CT14+EPPS16 (dashed curves) and CT10+EPS09 (solid curves).
002276639 8564_ $$82226860$$s7876$$uhttp://cds.cern.ch/record/2276639/files/v3pt8_Ziwei.png$$y00025 (Color online) The $v_3\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from $\mathtt{AMPT-SM}$ at 5~TeV (a) and 8~TeV (b). The 5~TeV results in the (0-5)\% centrality range from $\mathtt{AMPT-SM}$ versions 2.26t7 (solid blue) and 2.26t1 (dashed magenta) are compared to each other and to the CMS 5~TeV $p+$Pb data \protect\cite{Chatrchyan:2013nka} in (a). In (b), the $\mathtt{AMPT-SM}$ version 2.26t7 calculations at 8~TeV for (0-5)\% (solid red) and (0-20)\% (dashed black) are shown.
002276639 8564_ $$82226861$$s17812$$uhttp://cds.cern.ch/record/2276639/files/ups_other_y_b.png$$y00038 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $\Upsilon$ as a function of rapidity at 8~TeV. (a) The EPS09 NLO result is compared between the NLO CEM calculation of Vogt (dot-dot-dash-dashed red curve) and the data-driven result of Lansberg and Shao (solid cyan). (b) The data-driven calculation of Lansberg and Shao for EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram) is compared to the energy loss only calculation of Arleo (dot-dashed red curve).
002276639 8564_ $$82226862$$s22738$$uhttp://cds.cern.ch/record/2276639/files/z0cms8ppbnloy.png$$y00056 (Color online) (a) The differential cross section as a function of $Z^0$ rapidity. (b) The ratios of each result and the corresponding baseline. The $Z^0$ mass window used in the calculation is $60&lt;m_Z&lt;120$~GeV~\cite{CMS:2014sca}.
002276639 8564_ $$82226863$$s26148$$uhttp://cds.cern.ch/record/2276639/files/D0_forwardy_b.png$$y00047 (Color online) Prediction for $D$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions at midrapidity (a) and forward rapidity (b) at 8~TeV. The data-driven shadowing results of Lansberg and Shao are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram). Results with Cronin broadening alone (solid red) and with energy loss (full Cronin and moderate energy loss, red dashed, reduced Cronin and stronger energy loss, red dot dashed) are also shown.
002276639 8564_ $$82226864$$s22139$$uhttp://cds.cern.ch/record/2276639/files/v3pt_Ziwei.png$$y00022 (Color online) $v_3\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from string melting $\mathtt{AMPT}$.
002276639 8564_ $$82226865$$s18199$$uhttp://cds.cern.ch/record/2276639/files/psi_bckY_pT_8vs5_a.png$$y00035 (Color online) The ratio $R_{\rm p{\rm Pb}}$ for $J/\psi$ as a function of $p_T$ at 5 TeV (blue points and solid blue curves) and 8 TeV (red points and dashes red curves) calculated with EPS09 NLO are compared. The data from ALICE at 5 TeV \protect\cite{ALICE_psi_pT} and 8 TeV \protect\cite{Enrico} are also shown at backward rapidity (a) and forward rapidity (b).
002276639 8564_ $$82226866$$s25219$$uhttp://cds.cern.ch/record/2276639/files/D0_midy_a.png$$y00046 (Color online) Prediction for $D$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions at midrapidity (a) and forward rapidity (b) at 8~TeV. The data-driven shadowing results of Lansberg and Shao are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram). Results with Cronin broadening alone (solid red) and with energy loss (full Cronin and moderate energy loss, red dashed, reduced Cronin and stronger energy loss, red dot dashed) are also shown.
002276639 8564_ $$82226867$$s26722$$uhttp://cds.cern.ch/record/2276639/files/wcms8ppbcas.png$$y00059 (Color online) (a) The $W^+/W^-$ charge asymmetry as a function of the charged lepton pseudorapidity in $p+$Pb collisions at 8~TeV. (b) The differences between each result and its corresponding baseline as a function of charged lepton pseudorapidity. In both (a) and (b), the calculations with CT10+EPS09 are shown by red circles, CT10+nCTEQ by green squares and ABMP15+KP by blue stars. (c) The differences between nCTEQ and KP shadowing and EPS09 NLO are shown by the green squares and blue stars respectively.
002276639 8564_ $$82226868$$s25054$$uhttp://cds.cern.ch/record/2276639/files/Bp_midy_a.png$$y00049 (Color online) Prediction for $B$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions at midrapidity (a) and forward rapidity (b) at 8~TeV. The data-driven shadowing results of Lansberg and Shao are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram). Results with Cronin broadening alone (solid red) and with energy loss (full Cronin and moderate energy loss, red dashed, reduced Cronin and stronger energy loss, red dot dashed) are also shown.
002276639 8564_ $$82226869$$s8704$$uhttp://cds.cern.ch/record/2276639/files/photons_lowpT_a.png$$y00056 (Color online) Prediction for direct photon $R_{p{\rm Pb}}$ in $p+$Pb collisions at midrapidity for $p_T &lt; 30$~GeV (a) and $p_T &gt; 50$~GeV (b) in 8~TeV collisions. Results with Cronin broadening alone (solid) and with energy loss: full Cronin and moderate energy loss (dashed) and reduced Cronin but stronger energy loss (dot-dashed), are shown.
002276639 8564_ $$82226870$$s1411$$uhttp://cds.cern.ch/record/2276639/files/plot_R_pPb_ch_y0_8TeV_updated.png$$y00015 (Color online) Charged-hadron nuclear modification factor for $p$+Pb collisions at $\sqrt{s_{_{NN}}} = 8.0$~TeV and $|\eta| &lt; 1.0$. The NLO predictions are computed using the CT10 free proton PDFs with EPS09 nuclear modifications and three fragmentation functions: Kretzer (blue, long-dashed), KKP (red, dot-dashed) and DSS (green, dashed). The uncertainty band is derived from the EPS09 error sets using the DSS fragmentation function. The dotted line with an arrow shows the $p_T$ region where this calculation is expected to be relevant.
002276639 8564_ $$82226871$$s7131$$uhttp://cds.cern.ch/record/2276639/files/DoubleRpPbvy8TeV_5TeV.png$$y00041 (Color online) The ratio of nuclear modification factors $R_{p{\rm Pb}}(y)$ for $\psi(2{\rm S})$ relative to $\psi(1{\rm S})$ are compared at 8.16~TeV (solid) and 5.02~TeV (dashed).
002276639 8564_ $$82226872$$s27721$$uhttp://cds.cern.ch/record/2276639/files/z0cms8ppbnloptKPr.png$$y00062 (Color online) (a) The differential cross section as a function of $Z^0$ transverse momentum in $p+$Pb collisions at 8~TeV for EPS09 (red circles), nCTEQ (yellow squares) and KP (blue stars). The corresponding $R_{p{\rm Pb}}$ calculations are shown for the nPDF effects in (b) while the nuclear modification factor due to isospin alone is shown in (c) for CT10 (open red circles) and ABMP15 (blue triangles).
002276639 8564_ $$82226873$$s25682$$uhttp://cds.cern.ch/record/2276639/files/dndeta-ch-8TeV-AMPT.png$$y00005 (Color online) The charged hadron multiplicity, $dN_{\rm ch}/d\eta$, in 8 TeV $p+$Pb collisions at different centralities calculated with $\mathtt{AMPT-SM}$ are shown. The result for all non-diffractive events at 5 TeV (red points and line) is also shown for comparison. The blue lines, from top to bottom are for centralities of (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\%, (60-90)\% and (90-100)\%. The blue points and line shows the 8 TeV non-diffractive multiplicity. The 8~TeV non-diffractive multiplicity is very similar to the calculation in the (40-60)\% centrality bin. The results in (a) are for the ATLAS centrality definition, $\langle E_T \rangle(-4.9 &lt; \eta_{\rm lab} &lt; -3.1)$ \protect\cite{Aad:2015zza}, while the results in (b) use the centrality definition based on charged particle multiplicity in the central region $\langle N_{\rm ch} \rangle(|\eta_{\rm lab}|&lt;2.4)$.
002276639 8564_ $$82226874$$s22873$$uhttp://cds.cern.ch/record/2276639/files/v4pt_Ziwei.png$$y00023 (Color online) $v_4\{2,|\Delta \eta|&gt;2\}(p_T)$ for $p+$Pb collisions from string melting $\mathtt{AMPT}$.
002276639 8564_ $$82226875$$s20379$$uhttp://cds.cern.ch/record/2276639/files/psi_cgc_pt_data_b.png$$y00043 (Color online) Nuclear suppression factor for $J/\psi$ production at 8~TeV by Douclou\'e {\it et al.} \protect\cite{Ducloue:2016pqr} (red dashed curves) and by Ma {\it et al.} \protect\cite{Ma:2015sia} (solid blue curves). (a) The rapidity dependence. (b) The transverse momentum dependence. The ALICE data \protect\cite{Enrico} are shown in black while the LHCb data \protect\cite{Aaij:2017cqq} are shown in blue.
002276639 8564_ $$82226876$$s8542$$uhttp://cds.cern.ch/record/2276639/files/rpPb_ch_mid.png$$y00017 (Color online) Charged hadron $R_{p {\rm Pb}}$ as a function of $p_T$ at midrapidity in 8~TeV collisions. The results by Vitev {\it et al.}\ with Cronin broadening alone (solid red) and with energy loss (full Cronin and moderate energy loss, red dashed, reduced Cronin and stronger energy loss, red dot dashed) are shown.
002276639 8564_ $$82226877$$s24772$$uhttp://cds.cern.ch/record/2276639/files/z0cms8ppbnloyKPr.png$$y00060 (Color online) (a) The differential cross section as a function of $Z^0$ rapidity in $p+$Pb collisions at 8~TeV for EPS09 (red circles), nCTEQ (green squares) and KP (blue stars). The corresponding $R_{p{\rm Pb}}$ calculations are shown in (b), along with the nuclear modification factor due to isospin alone, with CT10 (red dashed) and ABMP15 (blue dot-dashed). The $Z^0$ mass window used in the calculation is $60&lt;m_Z&lt;120$~GeV~\cite{CMS:2014sca}.
002276639 8564_ $$82226878$$s18577$$uhttp://cds.cern.ch/record/2276639/files/D0_backwardy.png$$y00045 (Color online) Prediction for $D$-meson $R_{p{\rm Pb}}$ in $p+$Pb collisions at $\sqrt{s_{_{NN}}}=8$ TeV with $-4 &lt; y &lt; -2.96$. The red band corresponds to $0.09 \leq \xi^2 \leq 0.12$~GeV$^2$. The data-driven shadowing results of Lansberg and Shao at 8 TeV and $-4.46 &lt; y &lt; -2.96$ are shown for EPS09 NLO (dashed blue histogram), EPS09 LO (solid blue histogram) and nCTEQ (dotted magenta histogram).
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