002157402 001__ 2157402
002157402 003__ SzGeCERN
002157402 005__ 20211012041502.0
002157402 0247_ $$2DOI$$a10.1142/S0218301316300058
002157402 0248_ $$aoai:cds.cern.ch:2157402$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002157402 035__ $$9arXiv$$aoai:arXiv.org:1605.09479
002157402 035__ $$9Inspire$$a1466449
002157402 037__ $$9arXiv$$aarXiv:1605.09479$$chep-ph
002157402 041__ $$aeng
002157402 084__ $$2PACS$$a12.38.Bx
002157402 084__ $$2PACS$$a25.75.Bh
002157402 084__ $$2PACS$$a25.75.Cj
002157402 084__ $$2PACS$$a13.87.−a
002157402 100__ $$aAlbacete, Javier L.$$uOrsay, IPN
002157402 245__ $$aPredictions for $p+$Pb Collisions at $\sqrt{s_{NN}} = 5$ TeV: Comparison with Data
002157402 246__ $$9arXiv$$aPredictions for $p+$Pb Collisions at $\sqrt{s_{NN}} = 5$ TeV: Comparison with Data
002157402 269__ $$c30 May 2016
002157402 260__ $$c2016-09-20
002157402 300__ $$a53 p
002157402 500__ $$9arXiv$$a55 pages 35 figures
002157402 520__ $$aPredictions made in Albacete {\it et al} prior to the LHC $p+$Pb run at $\sqrt{s_{NN}} = 5$ TeV are compared to currently available data. Some predictions shown here have been updated by including the same experimental cuts as the data. Some additional predictions are also presented, especially for quarkonia, that were provided to the experiments before the data were made public but were too late for the original publication are also shown here.
002157402 520__ $$9World Scientific$$aPredictions made in Albacete et al. [Int. J. Mod. Phys. E 22 (2013) 1330007] prior to the LHC p+Pb run at sNN = 5 TeV are compared to currently available data. Some predictions shown here have been updated by including the same experimental cuts as the data. Some additional predictions are also presented, especially for quarkonia, that were provided to the experiments before the data were made public but were too late for the original publication.
002157402 520__ $$9arXiv$$aPredictions made in Albacete {\it et al} prior to the LHC $p+$Pb run at $\sqrt{s_{NN}} = 5$ TeV are compared to currently available data. Some predictions shown here have been updated by including the same experimental cuts as the data. Some additional predictions are also presented, especially for quarkonia, that were provided to the experiments before the data were made public but were too late for the original publication are also shown here.
002157402 540__ $$aarXiv nonexclusive-distrib. 1.0$$barXiv$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002157402 542__ $$3Publication$$dWorld Scientific Publishing Company$$g2016
002157402 595__ $$aLANL EDS
002157402 65017 $$2arXiv$$aParticle Physics - Phenomenology
002157402 65027 $$2arXiv$$aNuclear Physics - Theory
002157402 65027 $$2arXiv$$bNuclear Physics - Experiment
002157402 695__ $$9LANL EDS$$ahep-ph
002157402 695__ $$9LANL EDS$$anucl-ex
002157402 695__ $$9LANL EDS$$anucl-th
002157402 690C_ $$aARTICLE
002157402 690C_ $$aCERN
002157402 700__ $$aArleo, François$$uAnnecy, LAPTH$$uEcole Polytechnique
002157402 700__ $$aBarnaföldi, Gergely G.$$uWigner RCP, Budapest
002157402 700__ $$aBarrette, Jean$$uSaclay
002157402 700__ $$aDeng, Wei-Tian$$uFrankfurt U., FIAS$$uShandong U.
002157402 700__ $$aDumitru, Adrian$$uBaruch Coll.
002157402 700__ $$aEskola, Kari J.$$uHelsinki Inst. of Phys.$$uJyvaskyla U.
002157402 700__ $$aFerreiro, Elena G.$$uSantiago de Compostela U.
002157402 700__ $$aFleuret, Frederic$$uParis U., VI-VII
002157402 700__ $$aFujii, Hirotsugu$$uKEK, Tsukuba
002157402 700__ $$aGyulassy, Miklos$$uColumbia U.
002157402 700__ $$aHarangozó, Szilveszter Miklós$$uBudapest, RMKI$$uEotvos Lorand U., Budapest, Inst. Theor. Phys.
002157402 700__ $$aHelenius, Ilkka$$uHelsinki Inst. of Phys.$$uJyvaskyla U.
002157402 700__ $$aKang, Zhong-Bo$$uLos Alamos
002157402 700__ $$aKotko, Piotr$$uPenn State U.
002157402 700__ $$aKutak, Krzysztof$$uCracow, INP
002157402 700__ $$aLansberg, Jean-Philippe$$uOrsay, IPN
002157402 700__ $$aLevai, Peter$$uBudapest, RMKI
002157402 700__ $$aLin, Zi-Wei$$uEast Carolina U.
002157402 700__ $$aNara, Yasushi$$uAkita Intl. U.
002157402 700__ $$aRakotozafindrabe, Andry$$uIRFU, Saclay
002157402 700__ $$aPapp, Gábor$$uEotvos U.
002157402 700__ $$aPaukkunen, Hannu$$uJyvaskyla U.$$uHelsinki Inst. of Phys.
002157402 700__ $$aPeigné, Stéphane$$uSUBATECH, Nantes
002157402 700__ $$aPetrovici, Mihai$$uBucharest, IFIN-HH
002157402 700__ $$aQiu, Jian-Wei$$uIowa State U.
002157402 700__ $$aRezaeian, Amir H.$$uCCTVal, Valparaiso$$uSanta Maria U., Valparaiso
002157402 700__ $$aRu, Peng$$uCCNU, Wuhan, Inst. Part. Phys.
002157402 700__ $$aSapeta, Sebastian$$uCracow, INP$$uCERN
002157402 700__ $$aTopor Pop, Vasile$$uMcGill U.
002157402 700__ $$aVitev, Ivan$$uLos Alamos
002157402 700__ $$aVogt, Ramona$$uUC, Davis$$uLLNL, Livermore
002157402 700__ $$aWang, Enke$$uHua-Zhong Normal U., LQLP$$uHua-Zhong Normal U.
002157402 700__ $$aWang, Xin-Nian$$uDuke U.
002157402 700__ $$aXing, Hongxi$$uLos Alamos
002157402 700__ $$aXu, Rong$$uCCNU, Wuhan, Inst. Part. Phys.
002157402 700__ $$aZhang, Ben-Wei$$uHua-Zhong Normal U.$$uHua-Zhong Normal U., LQLP
002157402 700__ $$aZhang, Wei-Ning$$uDalian U. Tech.$$uHarbin Inst. Tech.
002157402 773__ $$c1630005$$pInt. J. Mod. Phys. E$$v25$$y2016
002157402 8564_ $$uhttp://arxiv.org/pdf/1605.09479.pdf$$yPreprint
002157402 8564_ $$82222940$$s31303$$uhttp://cds.cern.ch/record/2157402/files/W_CMS_5pPb_fbasy.png$$y00044 (Color online) The froward-backward asymmetry as a function of the charged lepton pseudorapidity in the laboratory frame for $W^\pm$ production. The results for $W^+$ are shown on the left-hand side while those for $W^-$ are shown on the right-hand side. The results with the CT10 proton PDFs are shown on top while those with MSTW2008 are shown on the bottom. The calculations are compared to the CMS data~\cite{Khachatryan:2015hha}.
002157402 8564_ $$82222941$$s13240$$uhttp://cds.cern.ch/record/2157402/files/v4pt-compare.png$$y00015 (Color online) The value of $v_4\{2,|\Delta \eta|>2\}(p_T)$ calculated with $\mathtt{AMPT-SM}$ for $p+$Pb collisions.
002157402 8564_ $$82222942$$s27660$$uhttp://cds.cern.ch/record/2157402/files/ups_fb_5dat.png$$y00035 (Color online) (Left) The ratio $R_{p{\rm Pb}}$ for $\Upsilon$ as a function of $y$. The red curves show the EPS09 NLO CEM uncertainties \protect\cite{Vogt:2015uba}. The EPS09 LO CSM calculation \protect\cite{Ferreiro:2013pua} is shown in cyan. The energy loss only calculations \protect\cite{Arleo:2012rs,Arleo:2013zua} are shown in magenta. The upper and lower limits of the CGC calculation \cite{Fujii:2013gxa} are in blue at forward rapidity. (Right) The forward-backward ratio, $R_{FB}$, as a function of rapidity. The same results as on the left-hand side are given, except for the CGC result which is not calculable at backward rapidity. The data from ALICE \protect\cite{Abelev:2014oea} and LHCb \protect\cite{Aaij:2013zxa} are also shown in both panels.
002157402 8564_ $$82222943$$s25538$$uhttp://cds.cern.ch/record/2157402/files/R_cp_pt.png$$y00017 (Color online) Comparison of the calculated $R_{CP}$ with the ATLAS data \protect\cite{ATLAS:2014cpa} (points) as a function of $p_T$. The upper and lower limits of the calculated results are given as red solid curves for (a) $0.3 < y < 0.8$, (b) $0.8 < y < 1.2$, (c) $1.2 < y < 2.1$, (d) $2.1 < y < 2.8$, (e) $2.8 < y < 3.6$, and (f) $3.6 < y < 4.4$.
002157402 8564_ $$82222944$$s1631006$$uhttp://cds.cern.ch/record/2157402/files/arXiv:1605.09479.pdf
002157402 8564_ $$82222945$$s12064$$uhttp://cds.cern.ch/record/2157402/files/RpA_dphi_qm15.png$$y00028 (Color online) Similar to Fig.~\protect\ref{fig:decor-p-Pb} but expanding the low-$p_T$ ($p_T < 25$ GeV) (top) and high $\Delta \phi$ ($\Delta \phi > 2$) (bottom) regions. Calculations using the Sudakov-weighted events \protect\cite{vanHameren:2014ala} are given by the orange band. The statistical errors on the calculations are included in the uncertainty bands.
002157402 8564_ $$82222946$$s17645$$uhttp://cds.cern.ch/record/2157402/files/z0_LHCb_fb.png$$y00043 (Color online) The forward and backward $Z^0$ cross sections are shown on the left-hand side while the forward-backward asymmetry is shown on the right-hand side. The results are compared with the LHCb data~\protect\cite{Aaij:2014pvu}.
002157402 8564_ $$82222947$$s20644$$uhttp://cds.cern.ch/record/2157402/files/dnchdpt_xndata.png$$y00006 (Color online) Charged particle $p_T$ distributions at $\sqrt{s_{_{NN}}} = 5.02$ TeV. The charged hadron $p_T$ distribution in $p+$Pb collisions with different $\mathtt{HIJING2.1}$ options \protect\cite{Xu:2012au} is also compared to data. The data are from the ALICE \protect\cite{ALICE:2012mj} (left) and CMS \protect\cite{CMS:2013cka} (right) Collaborations. All the calculations were presented in Ref.~[\protect\refcite{Albacete:2013ei}].
002157402 8564_ $$82222948$$s10127$$uhttp://cds.cern.ch/record/2157402/files/RpA_dphi_5TeV_sud.png$$y00022 (Color online) (Top left) Comparison of the CMS 7 TeV $p+p$ data \protect\cite{CMS:2014oma} to predictions in the hybrid high energy factorization approach using the KS linear and nonlinear gluon densities. (Top right) The CMS data are compared to the result with the Sudakov-improved KS nonlinear gluon density. (Bottom) The prediction of the nuclear modification factor for inclusive dijet production as well as for the inside-jet tag scenario where there is third jet with $p_{T3}>20$ GeV obeying the constraint $y_1>y_3>y_2$. From Ref.~[\protect\refcite{vanHameren:2014ala}].
002157402 8564_ $$82222949$$s26577$$uhttp://cds.cern.ch/record/2157402/files/upsy_all_nlo_shad_5dat_old.png$$y00034 (Color online) (Left) The ratio $R_{p{\rm Pb}}$ for $\Upsilon$ as a function of $y$. The red curves show the EPS09 NLO CEM uncertainties \protect\cite{Vogt:2015uba}. The EPS09 LO CSM calculation \protect\cite{Ferreiro:2013pua} is shown in cyan. The energy loss only calculations \protect\cite{Arleo:2012rs,Arleo:2013zua} are shown in magenta. The upper and lower limits of the CGC calculation \cite{Fujii:2013gxa} are in blue at forward rapidity. (Right) The forward-backward ratio, $R_{FB}$, as a function of rapidity. The same results as on the left-hand side are given, except for the CGC result which is not calculable at backward rapidity. The data from ALICE \protect\cite{Abelev:2014oea} and LHCb \protect\cite{Aaij:2013zxa} are also shown in both panels.
002157402 8564_ $$82222950$$s25656$$uhttp://cds.cern.ch/record/2157402/files/lhc_jps_ups_ppb.png$$y00029 (Color online) The $\jpsi$ and $\Upsilon$ suppression factor as a function of rapidity in $p+$Pb collisions at $\sqrts=5.02$~TeV for cold matter energy loss alone.
002157402 8564_ $$82222951$$s20130$$uhttp://cds.cern.ch/record/2157402/files/W_CMS_5pPb_asy.png$$y00045 (Color online) The $W^+/W^-$ charge asymmetry as a function of the charged lepton pseudorapidity calculated with the CT10 proton PDFs is shown on the left while results with MSTW2008 are shown on the right. The CMS data are from Ref.~[\protect\refcite{Khachatryan:2015hha}].
002157402 8564_ $$82222952$$s20955$$uhttp://cds.cern.ch/record/2157402/files/dnchdpt_xncms.png$$y00007 (Color online) Charged particle $p_T$ distributions at $\sqrt{s_{_{NN}}} = 5.02$ TeV. The charged hadron $p_T$ distribution in $p+$Pb collisions with different $\mathtt{HIJING2.1}$ options \protect\cite{Xu:2012au} is also compared to data. The data are from the ALICE \protect\cite{ALICE:2012mj} (left) and CMS \protect\cite{CMS:2013cka} (right) Collaborations. All the calculations were presented in Ref.~[\protect\refcite{Albacete:2013ei}].
002157402 8564_ $$82222953$$s1306$$uhttp://cds.cern.ch/record/2157402/files/figpPby4e.png$$y00036 (Color online) The $J/\psi$ (blue line) and $\psi(2S)$ (red line) nuclear modification factors $R_{p {\rm Pb}}$ as a function of rapidity compared to the ALICE data \protect\cite{Abelev:2014zpa}. The suppression due to the shadowing corrections (dashed line) is also shown.
002157402 8564_ $$82222954$$s26649$$uhttp://cds.cern.ch/record/2157402/files/yasym_CMS.png$$y00012 (Color online) Predictions for the forward-backward asymmetry, $Y_{\rm asym}^{h}(p_T)$, from Refs.~\protect\cite{Levai:2011qm,Barnafoldi:2008ec}. Centrality-independent results are shown for the HKN \protect\cite{Hirai:2001np}, EKS98 \protect\cite{Eskola:1998df} and EPS08 \protect\cite{Eskola:2008ca} parameterizations. Minimum bias results obtained by integrating over centrality are also shown for $\mathtt{HIJINGB\overline{B}}$ and $\mathtt{HIJING2.0}$ with and without multiple scattering. The blue points are the $\mathtt{AMPT-def}$ results. The CMS data \protect\cite{CMS:2013cka,Khachatryan:2015xaa} are shown in black.
002157402 8564_ $$82222955$$s1631$$uhttp://cds.cern.ch/record/2157402/files/forRamonapPbvsncoll1.png$$y00037 (Color online) The nuclear modification factor $R_{p{\rm Pb}}$ as a function of the number of binary nucleon-nucleon collisions, $N_{\rm coll}$, in the backward $-4.46<y<-2.96$ rapidity interval for the $J/\psi$ (blue line) and the $\psi(2S)$ (red line). The modification due to the shadowing corrections alone (dotted line) is also shown.
002157402 8564_ $$82222956$$s1630$$uhttp://cds.cern.ch/record/2157402/files/forRamonapPbvsncoll2.png$$y00038 (Color online) The nuclear modification factor $R_{p{\rm Pb}}$ as a function of the number of binary nucleon-nucleon collisions, $N_{\rm coll}$, in the forward $2.03<y<3.53$ rapidity interval for the $J/\psi$ (blue line) and the $\psi(2S)$ (red line). The modification due to the shadowing corrections alone (dotted line) is also shown.
002157402 8564_ $$82222957$$s20895$$uhttp://cds.cern.ch/record/2157402/files/psipt_fb_nlo_5dat_new.png$$y00033 (Color online) The ratio $R_{FB}$ for $J/\psi$ as a function of $y$ (left) and $p_T$ (right). The red curves show the EPS09 NLO uncertainties \protect\cite{Vogt:2015uba}. The result with energy loss alone \protect\cite{Arleo:2012rs,Arleo:2013zua} are shown in magenta. The EPS09 LO CSM results \protect\cite{Ferreiro:2013pua} are given by the cyan curves for the rapidity dependence only. The ALICE \protect\cite{Abelev:2013yxa,Abelev:2014oea} and LHCb \protect\cite{Aaij:2013zxa,Aaij:2014mza} data are also shown.
002157402 8564_ $$82222958$$s26555$$uhttp://cds.cern.ch/record/2157402/files/dnchdpt_cms.png$$y00005 (Color online) Charged particle $p_T$ distributions at $\sqrt{s_{_{NN}}} = 5.02$ TeV. The solid and dashed cyan curves outline the rcBK band \protect\cite{Albacete:2012xq}. The magenta curves, calculated with $\mathtt{HIJINGB\overline{B}2.0}$ are presented without (dot-dashed) and with (dotted) shadowing. The $\mathtt{AMPT}$ results are given by the dot-dash-dash-dashed (default) and dot-dot-dot-dashed (SM) blue curves. The data are from the ALICE \protect\cite{ALICE:2012mj} (left) and CMS \protect\cite{CMS:2013cka} (right) Collaborations. All the calculations were presented in Ref.~[\protect\refcite{Albacete:2013ei}].
002157402 8564_ $$82222959$$s5976$$uhttp://cds.cern.ch/record/2157402/files/RpA-ptmin.png$$y00024 (Color online) The nuclear modification factor, $R_{pA}$, as functions of the $p_T$ of the harder jet (top left), the $p_T$ of the subleading jet (top right), and the azimuthal angle between the jets (bottom). The blue lines correspond to predictions obtained using the KS gluon density alone \protect\cite{Kutak:2012rf} while the red lines are predictions including a gluon density that also depends on the hard scale \protect\cite{Kutak:2014wga}. In both cases, the renormalization and factorization scales are $\mu= (p_{T1}+p_{T2})/2$. The light red bands show the effect of varying the scales in the KS nonlinear + hard scale result from $0.5 \leq \mu \leq 2$. The analogous variation for the pure KS nonlinear gluon gives virtually no effect and is therefore not shown.
002157402 8564_ $$82222960$$s42025$$uhttp://cds.cern.ch/record/2157402/files/R_cp_ptcoshy_for.png$$y00018 (Color online) Comparison of the calculated $R_{CP}$ with the ATLAS data \protect\cite{ATLAS:2014cpa} as a function of $p_T \cosh y$. In (a), the results at forward rapidities ($0.8 < y < 1.2$ (blue diamonds), $1.2 < y < 2.1$ (maroon upward-pointing triangles), $2.1 < y < 2.8$ (green left-pointing triangles), $2.8 < y < 3.6$ (magenta downward-pointing triangles), and $3.6 < y < 4.4$ (orange right-pointing triangles) are shown. In (b), results near midrapidity are shown ($-0.3 < y < 0.3$ (black circles) and $0.3 < y < 0.8$ (red squares)). The upper and lower limits of the calculation for each rapidity region overlap each other.
002157402 8564_ $$82222961$$s22213$$uhttp://cds.cern.ch/record/2157402/files/ATLAS-Z.png$$y00046 (Color online) The $Z^0$ transverse momentum spectra in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$~TeV with the low $p_T$ region emphasized. The results for ATLAS~\protect\cite{ZpPbATLAS} and CMS~\protect\cite{CMS:2014sca} are shown in the left and right panels, respectively.
002157402 8564_ $$82222962$$s30797$$uhttp://cds.cern.ch/record/2157402/files/psiy_all_nlo_shad_5dat_new.png$$y00030 (Color online) (Left) The ratio $R_{p{\rm Pb}}$ for $J/\psi$ as a function of $y$. The red curves show the EPS09 NLO CEM uncertainties \protect\cite{Vogt:2015uba}. The EPS09 LO CSM calculation \protect\cite{Ferreiro:2013pua} is shown in cyan. The energy loss only calculations \protect\cite{Arleo:2012rs,Arleo:2013zua} are shown in magenta. The upper and lower limits of the CGC calculation \cite{Fujii:2013gxa} are in blue at forward rapidity. (Right) The EPS09 LO calculations in the CEM (red) and CSM (cyan) are compared with each other and with the EPS09 NLO CEM calculation on the left-hand side. The CEM calculation \protect\cite{Vogt:2015uba} includes the full EPS09 LO uncertainty added in quadrature while the CSM calculation \protect\cite{Ferreiro:2013pua} includes only the minimum and maximum uncertainty sets. The ALICE \protect\cite{Abelev:2013yxa,Abelev:2014oea} and LHCb \protect\cite{Aaij:2013zxa,Aaij:2014mza} data are also shown.
002157402 8564_ $$82222963$$s86547$$uhttp://cds.cern.ch/record/2157402/files/plot_ratio.png$$y00011 (Color online) Ratios between the ALICE \protect\cite{Abelev:2014dsa, Abelev:2013ala} (diamonds) and CMS \protect\cite{Khachatryan:2015xaa, Chatrchyan:2011av, CMS:2012aa} (circles) and the NLO calculations employing the CT10 proton PDFs with EPS09 NLO (in $p+$Pb collisions), and Kretzer FFs. In all panels, the light blue bands quantify the QCD scale uncertainty while the darker blue bands indicate the CT10 error range in $p+p$ collisions and the EPS09 NLO error range in $p+$Pb collisions. The purple and green curves are calculations in the same framework but employing the KKP \protect\cite{Kniehl:2000fe} and DSS \protect\cite{deFlorian:2007hc} FFs respectively, normalized to the calculation with the Kretzer FFs. The $\sqrt{s}=7$~TeV and $\sqrt{s}=2.76$~TeV panels are from Ref.~[\protect\refcite{d'Enterria:2013vba}].
002157402 8564_ $$82222964$$s11925$$uhttp://cds.cern.ch/record/2157402/files/RpA_pT1_qm15.png$$y00026 (Color online) Similar to Fig.~\protect\ref{fig:decor-p-Pb} but expanding the low-$p_T$ ($p_T < 25$ GeV) (top) and high $\Delta \phi$ ($\Delta \phi > 2$) (bottom) regions. Calculations using the Sudakov-weighted events \protect\cite{vanHameren:2014ala} are given by the orange band. The statistical errors on the calculations are included in the uncertainty bands.
002157402 8564_ $$82222965$$s9801$$uhttp://cds.cern.ch/record/2157402/files/z0_CMS_5pPb_fbasy.png$$y00042 (Color online) The forward-backward asymmetry as a function of the absolute value of $Z^0$ rapidity in the center of mass frame. The results with the CT10 proton PDFs are shown on the left and the results with the MSTW2008 PDFs are shown on the right. The CMS data are from Ref.~[\protect\refcite{CMS:2014sca}].
002157402 8564_ $$82222966$$s14757$$uhttp://cds.cern.ch/record/2157402/files/RpA-dphi.png$$y00025 (Color online) The nuclear modification factor, $R_{pA}$, as functions of the $p_T$ of the harder jet (top left), the $p_T$ of the subleading jet (top right), and the azimuthal angle between the jets (bottom). The blue lines correspond to predictions obtained using the KS gluon density alone \protect\cite{Kutak:2012rf} while the red lines are predictions including a gluon density that also depends on the hard scale \protect\cite{Kutak:2014wga}. In both cases, the renormalization and factorization scales are $\mu= (p_{T1}+p_{T2})/2$. The light red bands show the effect of varying the scales in the KS nonlinear + hard scale result from $0.5 \leq \mu \leq 2$. The analogous variation for the pure KS nonlinear gluon gives virtually no effect and is therefore not shown.
002157402 8564_ $$82222967$$s24318$$uhttp://cds.cern.ch/record/2157402/files/R_cp_ptcoshy_mid.png$$y00019 (Color online) Comparison of the calculated $R_{CP}$ with the ATLAS data \protect\cite{ATLAS:2014cpa} as a function of $p_T \cosh y$. In (a), the results at forward rapidities ($0.8 < y < 1.2$ (blue diamonds), $1.2 < y < 2.1$ (maroon upward-pointing triangles), $2.1 < y < 2.8$ (green left-pointing triangles), $2.8 < y < 3.6$ (magenta downward-pointing triangles), and $3.6 < y < 4.4$ (orange right-pointing triangles) are shown. In (b), results near midrapidity are shown ($-0.3 < y < 0.3$ (black circles) and $0.3 < y < 0.8$ (red squares)). The upper and lower limits of the calculation for each rapidity region overlap each other.
002157402 8564_ $$82222968$$s26119$$uhttp://cds.cern.ch/record/2157402/files/dnchdpt_data.png$$y00004 (Color online) Charged particle $p_T$ distributions at $\sqrt{s_{_{NN}}} = 5.02$ TeV. The solid and dashed cyan curves outline the rcBK band \protect\cite{Albacete:2012xq}. The magenta curves, calculated with $\mathtt{HIJINGB\overline{B}2.0}$ are presented without (dot-dashed) and with (dotted) shadowing. The $\mathtt{AMPT}$ results are given by the dot-dash-dash-dashed (default) and dot-dot-dot-dashed (SM) blue curves. The data are from the ALICE \protect\cite{ALICE:2012mj} (left) and CMS \protect\cite{CMS:2013cka} (right) Collaborations. All the calculations were presented in Ref.~[\protect\refcite{Albacete:2013ei}].
002157402 8564_ $$82222969$$s17668$$uhttp://cds.cern.ch/record/2157402/files/plot-aliceff.png$$y00000 (Color online) The ALICE charged particle pseudorapidity distribution in minimum-bias $p+$Pb collisions at $\sqrt{s_{_{NN}}}=5.02$ TeV \protect\cite{ALICE:2012xs}. The b-CGC curves are based on leading log $k_T$-factorization and the b-CGC saturation model. The results are obtained for $m_{\rm jet} =1$, 5, and 10~MeV. The plot is taken from Ref.~[\protect\refcite{Rezaeian:2012ye}].
002157402 8564_ $$82222970$$s20751$$uhttp://cds.cern.ch/record/2157402/files/plot_R_pPb_ch_y0.png$$y00010 (Color online) The charged-hadron nuclear modification factor measured in $p+$Pb collisions by the ALICE \protect\cite{Abelev:2014dsa} (diamonds) and CMS \protect\cite{Khachatryan:2015xaa} (circles) collaborations. The data are compared to NLO calculations \protect\cite{Helenius:2012wd} which use the CT10 free proton PDFs \protect\cite{Lai:2010vv}, EPS09 NLO nuclear modifications \protect\cite{Eskola:2009uj}, and three different set of fragmentation functions (Kretzer \protect\cite{Kretzer:2000yf}, KKP \protect\cite{Kniehl:2000fe} and DSS \protect\cite{deFlorian:2007hc}). The EPS09 uncertainty range is shown as a sky blue band and is calculated using the DSS fragmentation function.
002157402 8564_ $$82222971$$s19113$$uhttp://cds.cern.ch/record/2157402/files/CMS-Z.png$$y00047 (Color online) The $Z^0$ transverse momentum spectra in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$~TeV with the low $p_T$ region emphasized. The results for ATLAS~\protect\cite{ZpPbATLAS} and CMS~\protect\cite{CMS:2014sca} are shown in the left and right panels, respectively.
002157402 8564_ $$82222972$$s28681$$uhttp://cds.cern.ch/record/2157402/files/psiy_fb_5dat_new.png$$y00032 (Color online) The ratio $R_{FB}$ for $J/\psi$ as a function of $y$ (left) and $p_T$ (right). The red curves show the EPS09 NLO uncertainties \protect\cite{Vogt:2015uba}. The result with energy loss alone \protect\cite{Arleo:2012rs,Arleo:2013zua} are shown in magenta. The EPS09 LO CSM results \protect\cite{Ferreiro:2013pua} are given by the cyan curves for the rapidity dependence only. The ALICE \protect\cite{Abelev:2013yxa,Abelev:2014oea} and LHCb \protect\cite{Aaij:2013zxa,Aaij:2014mza} data are also shown.
002157402 8564_ $$82222973$$s6774$$uhttp://cds.cern.ch/record/2157402/files/RpA-ptmax.png$$y00023 (Color online) The nuclear modification factor, $R_{pA}$, as functions of the $p_T$ of the harder jet (top left), the $p_T$ of the subleading jet (top right), and the azimuthal angle between the jets (bottom). The blue lines correspond to predictions obtained using the KS gluon density alone \protect\cite{Kutak:2012rf} while the red lines are predictions including a gluon density that also depends on the hard scale \protect\cite{Kutak:2014wga}. In both cases, the renormalization and factorization scales are $\mu= (p_{T1}+p_{T2})/2$. The light red bands show the effect of varying the scales in the KS nonlinear + hard scale result from $0.5 \leq \mu \leq 2$. The analogous variation for the pure KS nonlinear gluon gives virtually no effect and is therefore not shown.
002157402 8564_ $$82222974$$s16929$$uhttp://cds.cern.ch/record/2157402/files/v2pt-compare.png$$y00013 (Color online) The $v_2\{2,|\Delta \eta|>2\}(p_T)$ calculated for $p+$Pb collisions with $\mathtt{AMPT-SM}$. The data are from Ref.~[\protect\refcite{Chatrchyan:2013nka}]. The uncertainties shown on the data are statistical only.
002157402 8564_ $$82222975$$s44939$$uhttp://cds.cern.ch/record/2157402/files/z0_pPb_pt.png$$y00041 (Color online) The $Z^0$ transverse momentum spectra in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$~TeV. The results for ATLAS~\protect\cite{ZpPbATLAS} and CMS~\protect\cite{CMS:2014sca} are shown in the left and right panels, respectively. The top panels show results with the CT10 proton PDFs while results with the MSTW2008 PDFs are shown in the bottom panels.
002157402 8564_ $$82222976$$s30112$$uhttp://cds.cern.ch/record/2157402/files/psiy_nlo_lo_shad_5dat.png$$y00031 (Color online) (Left) The ratio $R_{p{\rm Pb}}$ for $J/\psi$ as a function of $y$. The red curves show the EPS09 NLO CEM uncertainties \protect\cite{Vogt:2015uba}. The EPS09 LO CSM calculation \protect\cite{Ferreiro:2013pua} is shown in cyan. The energy loss only calculations \protect\cite{Arleo:2012rs,Arleo:2013zua} are shown in magenta. The upper and lower limits of the CGC calculation \cite{Fujii:2013gxa} are in blue at forward rapidity. (Right) The EPS09 LO calculations in the CEM (red) and CSM (cyan) are compared with each other and with the EPS09 NLO CEM calculation on the left-hand side. The CEM calculation \protect\cite{Vogt:2015uba} includes the full EPS09 LO uncertainty added in quadrature while the CSM calculation \protect\cite{Ferreiro:2013pua} includes only the minimum and maximum uncertainty sets. The ALICE \protect\cite{Abelev:2013yxa,Abelev:2014oea} and LHCb \protect\cite{Aaij:2013zxa,Aaij:2014mza} data are also shown.
002157402 8564_ $$82222977$$s1698$$uhttp://cds.cern.ch/record/2157402/files/pPb_eta_AD.png$$y00001 (Color online) Charged particle pseudorapidity distribution at $\sqrt{s_{_{NN}}}= 5.02$ TeV as a function of $\eta$ with and without the adjusted Jacobian, calculated by Albacete and Dumitru.
002157402 8564_ $$82222978$$s43459$$uhttp://cds.cern.ch/record/2157402/files/z0_pPb_y.png$$y00039 (Color online) The $Z^0$ rapidity distribution in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$~TeV. The left panels show the results compared to the ATLAS data~\protect\cite{ZpPbATLAS} while those on the right show comparisons to the CMS data~\protect\cite{CMS:2014sca}. The top panels show calculations with the CT10 PDFs while results with MSTW2008 are shown on the bottom.
002157402 8564_ $$82222979$$s22039$$uhttp://cds.cern.ch/record/2157402/files/plot-5-e0-alicef.png$$y00009 (Color online) The nuclear modification factor $R_{pA}(p_T)$ for inclusive charged hadron production in minimum-bias $p+$Pb collisions at $\sqrt{s_{_{NN}}}=5.02$ TeV and $\eta=0$. The calculations are solutions of the rcBK equation with $Q_{0A}^2=0.168\, N$ GeV$^2$ for $4 < N < 6$ (grey area). The black curve shows $N=5$. The calculations are detailed in Ref.~[\protect\refcite{Rezaeian:2012ye}]. The points are the ALICE data while the dashed red lines delineate the experimental systematic uncertainties \protect\cite{ALICE:2012mj}. (The plot is taken from Ref.~[\protect\refcite{Rezaeian:2012ye}]).
002157402 8564_ $$82222980$$s57528$$uhttp://cds.cern.ch/record/2157402/files/dndeta-ch-cent-ATLAS-final-AR.png$$y00002 (Color online) The charged particle pseudorapidity distributions in the ATLAS centrality bins \protect\cite{Aad:2015zza} compared to calculations based on leading log $k_t$-factorization in the b-CGC saturation model. The central value of the calculation is for $m_{\rm jet} = 5$ MeV. From top down the centrality bins are: (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\%, and (60-90)\%. There is no additional scaling, neither on the data nor the calculations. See Ref.~[\protect\refcite{Rezaeian:2012ye}] for details of the calculation.
002157402 8564_ $$82222981$$s14142$$uhttp://cds.cern.ch/record/2157402/files/v3pt-compare.png$$y00014 (Color online) The calculated $v_3\{2,|\Delta \eta|>2\}(p_T)$ for $p+$Pb collisions with $\mathtt{AMPT-SM}$. The data are from Ref.~[\protect\refcite{Chatrchyan:2013nka}]. The uncertainties shown on the data are statistical only.
002157402 8564_ $$82222982$$s9962$$uhttp://cds.cern.ch/record/2157402/files/pp_dphi_7TeV_lin_vs_nonlin.png$$y00020 (Color online) (Top left) Comparison of the CMS 7 TeV $p+p$ data \protect\cite{CMS:2014oma} to predictions in the hybrid high energy factorization approach using the KS linear and nonlinear gluon densities. (Top right) The CMS data are compared to the result with the Sudakov-improved KS nonlinear gluon density. (Bottom) The prediction of the nuclear modification factor for inclusive dijet production as well as for the inside-jet tag scenario where there is third jet with $p_{T3}>20$ GeV obeying the constraint $y_1>y_3>y_2$. From Ref.~[\protect\refcite{vanHameren:2014ala}].
002157402 8564_ $$82222983$$s60382$$uhttp://cds.cern.ch/record/2157402/files/dijet_nPDF.png$$y00016 (Color online) The CMS dijet measurements \protect\cite{Chatrchyan:2014hqa} are compared to NLO theory calculations \protect\cite{Eskola:2013aya}. The predictions employ the CT10 free proton PDFs \protect\cite{Lai:2010vv} (purple dashed curve) and the CT10 PDFs modified by the EPS09 NLO \protect\cite{Eskola:2009uj} nuclear modifications (blue curve). The upper panel shows the normalized cross section as a function of $\eta_{\rm dijet}$. The lower two panels display the ratio of the data to the CT10+EPS09 and CT10 calculations respectively, including the PDF and nPDF uncertainty bands. The data are given for $p_{T,1} > 120$ GeV, $p_{T,2} > 30$ GeV, and azimuthal separation $\Delta \phi_{1,2} > 2\pi/3$. The pseudorapidity interval is chosen so that there is a gap in psuedorapidity between the dijets and the forward transverse energy deposited in the CMS HF detectors at $4 < |\eta| < 5.2$. See Ref.~[\protect\refcite{Chatrchyan:2014hqa}] for more experimental details.
002157402 8564_ $$82222984$$s9573$$uhttp://cds.cern.ch/record/2157402/files/RpA_pT2_qm15.png$$y00027 (Color online) Similar to Fig.~\protect\ref{fig:decor-p-Pb} but expanding the low-$p_T$ ($p_T < 25$ GeV) (top) and high $\Delta \phi$ ($\Delta \phi > 2$) (bottom) regions. Calculations using the Sudakov-weighted events \protect\cite{vanHameren:2014ala} are given by the orange band. The statistical errors on the calculations are included in the uncertainty bands.
002157402 8564_ $$82222985$$s33635$$uhttp://cds.cern.ch/record/2157402/files/W_CMS_5pPb_eta.png$$y00040 (Color online) The charged lepton pseudorapidity distributions for $W$ boson production in $p+$Pb collisions at $\sqrt{s_{NN}}=5.02$~TeV. The results for $W^+$ are shown on the left-hand side while those for $W^-$ are shown on the right. The results with the CT10~(top panels) and MSTW2008 PDFs~(bottom panels) are compared to the CMS data~\protect\cite{Khachatryan:2015hha}.
002157402 8564_ $$82222986$$s4205$$uhttp://cds.cern.ch/record/2157402/files/pp_dphi_7TeV_KSsud_vsCMS.png$$y00021 (Color online) (Top left) Comparison of the CMS 7 TeV $p+p$ data \protect\cite{CMS:2014oma} to predictions in the hybrid high energy factorization approach using the KS linear and nonlinear gluon densities. (Top right) The CMS data are compared to the result with the Sudakov-improved KS nonlinear gluon density. (Bottom) The prediction of the nuclear modification factor for inclusive dijet production as well as for the inside-jet tag scenario where there is third jet with $p_{T3}>20$ GeV obeying the constraint $y_1>y_3>y_2$. From Ref.~[\protect\refcite{vanHameren:2014ala}].
002157402 8564_ $$82222987$$s44562$$uhttp://cds.cern.ch/record/2157402/files/dndeta-ch-cent-ATLAS-final-AMPT.png$$y00003 (Color online) The charged particle pseudorapidity distributions in the ATLAS centrality bins \protect\cite{Aad:2015zza} compared to $\mathtt{AMPT}$ calculations. From top down the centrality bins are: (0-1)\%, (1-5)\%, (5-10)\%, (10-20)\%, (20-30)\%, (30-40)\%, (40-60)\%, and (60-90)\%. There is no additional scaling, neither on the data nor the calculations.
002157402 8564_ $$82222988$$s31851$$uhttp://cds.cern.ch/record/2157402/files/plot-av-all-largef.png$$y00008 (Color online) The average transverse momentum, $\langle p_T\rangle$, of charged particles in the range $0.15<p_T<10$ GeV as a function of charged particle multiplicity, $N_{\rm ch}$, in $p+p$, $p+$Pb, and Pb+Pb collisions at $\sqrt{s_{_{NN}}} = 7$, 5.02 and 2.76 TeV respectively for $|\eta|<0.3$. The b-CGC band includes the theoretical uncertainties \protect\cite{Rezaeian:2013woa}. The ALICE data \protect\cite{Abelev:2013bla} are also shown. (Taken from Ref.~[\protect\refcite{Rezaeian:2013woa}].)
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