002765256 001__ 2765256
002765256 005__ 20241127052219.0
002765256 0248_ $$aoai:cds.cern.ch:2765256$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
002765256 0247_ $$2DOI$$a10.22323/1.387.0190
002765256 037__ $$9arXiv$$aarXiv:2104.10926$$cnucl-ex
002765256 035__ $$9arXiv$$aoai:arXiv.org:2104.10926
002765256 035__ $$9Inspire$$aoai:inspirehep.net:1859987$$d2024-11-26T15:16:22Z$$h2024-11-27T03:03:33Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002765256 035__ $$9Inspire$$a1859987
002765256 041__ $$aeng
002765256 100__ $$aTrzeciak, [email protected]$$uPrague, Tech. U.$$vFaculty of Nuclear Sciences and Physics Engineering,Czech Technical University in Prague,Brehova 7,115 19 Prague,Czech Republic
002765256 245__ $$9arXiv$$aHeavy-flavour studies with a high-luminosity fixed-target experiment at the LHC
002765256 269__ $$c2021-04-22
002765256 260__ $$c2021-09-01
002765256 300__ $$a6 p
002765256 500__ $$9arXiv$$aHard Probes 2020 proceedings
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. $pp$, pd and $p$A collisions at $\sqrt{s_{\rm{NN}}}$ = 115 GeV and Pb$p$ and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy.
In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 520__ $$9arXiv$$aExtraction of the multi-TeV proton and lead LHC beams with a bent crystal or by using an internal gas target allows one to perform the most energetic fixed-target experiment ever. pp, pd and pA collisions at $\sqrt{s}$ = 115 GeV and Pbp and PbA collisions at $\sqrt{s_{\rm{NN}}}$ = 72 GeV can be studied with high precision and modern detection techniques over a broad rapidity range. Using the LHCb or the ALICE detector in a fixed-target mode offers unprecedented possibilities to access heavy-flavour production in a new energy domain, half way between the SPS and the nominal RHIC energy. In this contribution, a review of projection studies for quarkonium and open charm and beauty production with both detector set-ups used with various nuclear targets and the LHC lead beams is presented.
002765256 540__ $$3preprint$$aarXiv nonexclusive-distrib 1.0$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002765256 540__ $$3publication$$aCC-BY-NC-ND-4.0$$uhttps://creativecommons.org/licenses/by-nc-nd/4.0/
002765256 542__ $$3publication$$dThe author(s)$$g2021
002765256 65017 $$2arXiv$$anucl-ex
002765256 65017 $$2SzGeCERN$$aNuclear Physics - Experiment
002765256 690C_ $$aCERN
002765256 690C_ $$aARTICLE
002765256 700__ $$aBrodsky, S.J.$$uSLAC$$vSLAC National Accelerator Laboratory,Stanford University,Menlo Park,CA 94025,USA
002765256 700__ $$aCavoto, G.$$uRome U.$$uINFN, Rome$$v"Sapienza" Università di Roma,Dipartimento di Fisica & INFN,Sez. di Roma,P.le A. Moro 2,00185 Roma,Italy
002765256 700__ $$aDa Silva, C.$$uLos Alamos$$vP-25,Los Alamos National Laboratory,Los Alamos,NM 87545,USA
002765256 700__ $$aEchevarria, M.G.$$uUCM, Madrid, Dept. Phys.$$vDepartment of Physics and Mathematics,University of Alcalá,28805 Alcalá de Henares (Madrid),Spain
002765256 700__ $$aFerreiro, E.G.$$uSantiago de Compostela U., IGFAE$$uSantiago de Compostela U.$$vDept. de Física de Partículas & IGFAE,Universidade de Santiago de Compostela,15782 Santiago de Compostela,Spain
002765256 700__ $$aHadjidakis, C.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aHaque, R.$$uWarsaw U. of Tech.$$vFaculty of Physics,Warsaw University of Technology,ul. Koszykowa 75,00-662 Warsaw,Poland
002765256 700__ $$aHřivnáčová, I.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aKikoła, D.$$uWarsaw U. of Tech.$$vFaculty of Physics,Warsaw University of Technology,ul. Koszykowa 75,00-662 Warsaw,Poland
002765256 700__ $$aKlein, A.$$uLos Alamos$$vP-25,Los Alamos National Laboratory,Los Alamos,NM 87545,USA
002765256 700__ $$aKurepin, A.$$uMoscow, INR$$vInstitute for Nuclear Research,Moscow,Russia
002765256 700__ $$aKusina, A.$$uCracow, INP$$vInstitute of Nuclear Physics Polish Academy of Sciences,PL-31342 Krakow,Poland
002765256 700__ $$aLansberg, J.P.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aLorcé, C.$$uEcole Polytechnique, CPHT$$vCPHT,CNRS,Ecole Polytechnique,Institut Polytechnique de Paris,91128 Palaiseau,France
002765256 700__ $$aLyonnet, F.$$uSouthern Methodist U.$$vSouthern Methodist University,Dallas,TX 75275,USA
002765256 700__ $$aMakdisi, Y.$$uBNL, C-A Dept.$$vBrookhaven National Laboratory,Collider Accelerator Department
002765256 700__ $$aMassacrier, L.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aPorteboeuf, S.$$uClermont-Ferrand U.$$vUniversité Clermont Auvergne,CNRS/IN2P3,LPC,F-63000 Clermont-Ferrand,France.
002765256 700__ $$aQuintans, C.$$uLIP, Lisbon$$vLIP,Av. Prof. Gama Pinto,2,1649-003 Lisboa,Portugal
002765256 700__ $$aRakotozafindrabe, A.$$uIRFU, Saclay, DPHN$$vIRFU/DPhN,CEA Saclay,91191 Gif-sur-Yvette Cedex,France
002765256 700__ $$aRobbe, P.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aScandale, W.$$uCERN$$vCERN,European Organization for Nuclear Research,1211 Geneva 23,Switzerland
002765256 700__ $$aSchienbein, I.$$uLPSC, Grenoble$$vLaboratoire de Physique Subatomique et de Cosmologie,Université Grenoble Alpes,CNRS/IN2P3,53 Avenue des Martyrs,F-38026 Grenoble,France
002765256 700__ $$aSeixas, J.$$uLisbon, IST$$uLIP, Lisbon$$vDep. Fisica,Instituto Superior Tecnico,Av. Rovisco Pais 1,1049-001 Lisboa,Portugal$$vLIP,Av. Prof. Gama Pinto,2,1649-003 Lisboa,Portugal
002765256 700__ $$aShao, H.S.$$uParis, LPTHE$$vLPTHE,UMR 7589,Sorbonne Universityé et CNRS,4 place Jussieu,75252 Paris Cedex 05,France
002765256 700__ $$aSignori, A.$$uPavia U.$$uJefferson Lab$$vDipartimento di Fisica,Università di Pavia,via Bassi 6,I-27100 Pavia,Italy$$vTheory Center,Thomas Jefferson National Accelerator Facility,12000 Jefferson Avenue,Newport News,VA 23606,USA
002765256 700__ $$aTopilskaya, N.$$uMoscow, INR$$vInstitute for Nuclear Research,Moscow,Russia
002765256 700__ $$aUras, A.$$uLyon, IPN$$vIPNL,Université Claude Bernard Lyon-I and CNRS-IN2P3,Villeurbanne,France
002765256 700__ $$aVan Hulse, C.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aWagner, J.$$uNCBJ, Warsaw$$vNational Centre for Nuclear Research (NCBJ),Hoża 69,00-681,Warsaw,Poland
002765256 700__ $$aYamanaka, N.$$uIJCLab, Orsay$$vUniversité Paris-Saclay,CNRS,IJCLab,91405 Orsay,France
002765256 700__ $$aYang, Z.$$uTsinghua U., Beijing$$vCenter for High Energy Physics,Department of Engineering Physics,Tsinghua University,Beijing,China
002765256 700__ $$aZelenski, A.$$uBNL, C-A Dept.$$vBrookhaven National Laboratory,Collider Accelerator Department
002765256 773__ $$c190$$pPoS$$vHardProbes2020$$wC20-05-31.1$$y2021
002765256 8564_ $$uhttps://pos.sissa.it/387/190/pdf$$yPreprint
002765256 8564_ $$82291060$$s426174$$uhttp://cds.cern.ch/record/2765256/files/2104.10926.pdf$$yFulltext
002765256 8564_ $$82291061$$s50410$$uhttp://cds.cern.ch/record/2765256/files/charm_Rg_MU2GeV_xlin_90CL-crop.png$$y00002 Left: nCTEQ15 gluon nPDFs (ratio of gluon densities in nCTEQ15/CT14 PDFs) before and after the reweighting using fixed-target $D^{0}$ $R_{p\rm{Xe}}$ pseudo-data from LHCb-like simulations at a scale $Q=$~2~GeV. Right: The di-muon invariant mass distribution (the uncorrelated background subtraction) in the $\Upsilon(nS)$ mass range, PbXe collisions at \snn~=~72~GeV with the LHCb-like setup. No nuclear modifications are assumed.
002765256 8564_ $$82291062$$s28434$$uhttp://cds.cern.ch/record/2765256/files/ALICEFTYields_systems_hardQCD_solid_hDmeson_x2_yield.png$$y00001 Left: Typical kinematical reach in $x_{2}$ with bottomonium, charmonium and D, B meson probes and at $m_{T}$ scale of the fixed-target mode with the LHCb-like detector acceptance in $pp$ collisions at \s~=~115~GeV. Right: Expected $D^{0}$ meson yields with the ALICE-like setup as a function of $x_{2}$, with the proton beam on different nuclear targets at \snn~=~115~GeV, for one LHC running year.
002765256 8564_ $$82291063$$s26651$$uhttp://cds.cern.ch/record/2765256/files/ALICEFT_DmesonV2_010.png$$y00005 Statistical projections on $R_{CP}$ (left) and $v_2$ (right) vs $D^{0}$ $p_{T}$ in 0--10\% central $p$A collisions at \snn~=~115~GeV for the ALICE-like detector setup.
002765256 8564_ $$82291064$$s16597$$uhttp://cds.cern.ch/record/2765256/files/UpsilonStates72gev_BkgFit_Xe_UpsilonSignal_pt7y3-5.png$$y00003 Left: nCTEQ15 gluon nPDFs (ratio of gluon densities in nCTEQ15/CT14 PDFs) before and after the reweighting using fixed-target $D^{0}$ $R_{p\rm{Xe}}$ pseudo-data from LHCb-like simulations at a scale $Q=$~2~GeV. Right: The di-muon invariant mass distribution (the uncorrelated background subtraction) in the $\Upsilon(nS)$ mass range, PbXe collisions at \snn~=~72~GeV with the LHCb-like setup. No nuclear modifications are assumed.
002765256 8564_ $$82291065$$s36102$$uhttp://cds.cern.ch/record/2765256/files/LHCxBjorken-pp115GeV_LHCb.png$$y00000 Left: Typical kinematical reach in $x_{2}$ with bottomonium, charmonium and D, B meson probes and at $m_{T}$ scale of the fixed-target mode with the LHCb-like detector acceptance in $pp$ collisions at \s~=~115~GeV. Right: Expected $D^{0}$ meson yields with the ALICE-like setup as a function of $x_{2}$, with the proton beam on different nuclear targets at \snn~=~115~GeV, for one LHC running year.
002765256 8564_ $$82291066$$s27556$$uhttp://cds.cern.ch/record/2765256/files/ALICEFT_DmesonRcp_010.png$$y00004 Statistical projections on $R_{CP}$ (left) and $v_2$ (right) vs $D^{0}$ $p_{T}$ in 0--10\% central $p$A collisions at \snn~=~115~GeV for the ALICE-like detector setup.
002765256 8564_ $$82321495$$s333617$$uhttp://cds.cern.ch/record/2765256/files/document.pdf$$yFulltext
002765256 960__ $$a13
002765256 962__ $$b2740437$$k190$$naustin20200531
002765256 980__ $$aConferencePaper
002765256 980__ $$aARTICLE