CERN Accelerating science

002705729 001__ 2705729
002705729 005__ 20241030072933.0
002705729 0248_ $$aoai:cds.cern.ch:2705729$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002705729 0247_ $$2DOI$$a10.1103/PhysRevC.102.011901
002705729 037__ $$9arXiv$$aarXiv:1912.10871$$chep-ex
002705729 037__ $$aFERMILAB-PUB-19-664-AD-SCD
002705729 035__ $$9arXiv$$aoai:arXiv.org:1912.10871
002705729 035__ $$9Inspire$$aoai:inspirehep.net:1772241$$d2024-10-29T15:43:09Z$$h2024-10-30T03:51:54Z$$mmarcxml$$ttrue$$uhttps://inspirehep.net/api/oai2d
002705729 035__ $$9Inspire$$a1772241
002705729 041__ $$aeng
002705729 100__ $$aAduszkiewicz, A.$$uWarsaw U. (main)$$vUniversity of Warsaw, Warsaw, Poland
002705729 245__ $$9arXiv$$aProton-proton interactions and onset of deconfinement
002705729 269__ $$c2019-12-23
002705729 260__ $$c2020-07-16
002705729 300__ $$a5 p
002705729 520__ $$9APS$$aThe experiment of the NA61/SHINE Collaboration at the CERN SPS is performing a unique study of the phase diagram of strongly interacting matter by varying collision energy and nuclear mass number of colliding nuclei. In central Pb+Pb collisions, the experiment of the NA49 Collaboration found structures in the energy dependence of several observables in the energy range of the CERN SPS that had been predicted for the transition to a deconfined phase. New measurements of the NA61/SHINE Collaboration find intriguing similarities in p+p interactions for which no deconfinement transition is expected at the energies of the SPS. Possible implications will be discussed.
002705729 520__ $$9arXiv$$aThe NA61/SHINE experiment at the CERN SPS is performing a uniqe study of the phase diagram of strongly interacting matter by varying collision energy and nuclear mass number of colliding nuclei. In central Pb+Pb collisions the NA49 experiment found structures in the energy dependence of several observables in the CERN SPS energy range that had been predicted for the transition to a deconfined phase. New measurements of NA61/SHINE find intriguing similarities in p+p interactions for which no deconfinement transition is expected at SPS energies. Possible implications will be discussed.
002705729 540__ $$3preprint$$aarXiv nonexclusive-distrib 1.0$$uhttp://arxiv.org/licenses/nonexclusive-distrib/1.0/
002705729 540__ $$3publication$$aCC-BY-4.0
002705729 542__ $$3publication$$dauthors$$g2020
002705729 595__ $$aFor annual report
002705729 65017 $$2arXiv$$ahep-ph
002705729 65017 $$2SzGeCERN$$aParticle Physics - Phenomenology
002705729 65017 $$2arXiv$$ahep-ex
002705729 65017 $$2SzGeCERN$$aParticle Physics - Experiment
002705729 695__ $$aonset of deconfinement
002705729 690C_ $$aCERN
002705729 690C_ $$aARTICLE
002705729 700__ $$aAndronov, E.V.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aAnticic, T.$$uBoskovic Inst., Zagreb$$vRuder Boškovi ́c Institute, Zagreb, Croatia
002705729 700__ $$aBabkin, V.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aBaszczyk, M.$$uAGH-UST, Cracow$$vAGH - University of Science and Technology, Cracow, Poland
002705729 700__ $$aBhosale, S.$$uCracow, INP$$vInstitute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
002705729 700__ $$aBlondel, A.$$uParis U., VI-VII$$vLPNHE, University of Paris VI and VII, Paris, France
002705729 700__ $$aBogomilov, M.$$uSofiya, Inst. Phys.$$vFaculty of Physics, University of Sofia, Sofia, Bulgaria
002705729 700__ $$aBrandin, A.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aBravar, A.$$uGeneva U.$$vUniversity of Geneva, Geneva, Switzerland
002705729 700__ $$aBrylinski, W.$$uWarsaw U. of Tech. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aBrzychczyk, J.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aBuryakov, M.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aBusygina, O.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aBzdak, A.$$uAGH-UST, Cracow$$vAGH - University of Science and Technology, Cracow, Poland
002705729 700__ $$aCherif, H.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$áCirkovic, M.$$uBelgrade U.$$vUniversity of Belgrade, Belgrade, Serbia
002705729 700__ $$aCsanad, M.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, Budapest, Hungary
002705729 700__ $$aCybowska, J.$$uWarsaw U. of Tech. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aCzopowicz, T.$$uWarsaw U. of Tech. (main)$$uJan Kochanowski U., Kielce (main)$$vWarsaw University of Technology, Warsaw, Poland$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aDamyanova, A.$$uGeneva U.$$vUniversity of Geneva, Geneva, Switzerland
002705729 700__ $$aDavis, N.$$uCracow, INP$$vInstitute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
002705729 700__ $$aDeliyergiyev, M.$$uJan Kochanowski U., Kielce (main)$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aDeveaux, M.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aDmitriev, A.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aDominik, W.$$uWarsaw U. (main)$$vUniversity of Warsaw, Warsaw, Poland
002705729 700__ $$aDorosz, P.$$uAGH-UST, Cracow$$vAGH - University of Science and Technology, Cracow, Poland
002705729 700__ $$aDumarchez, J.$$uParis U., VI-VII$$vLPNHE, University of Paris VI and VII, Paris, France
002705729 700__ $$aEngel, R.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology, Karlsruhe, Germany
002705729 700__ $$aFeofilov, G.A.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aFields, L.$$uFermilab$$vFermilab, Batavia, USA
002705729 700__ $$aFodor, Z.$$uWigner RCP, Budapest$$uU. Wroclaw (main)$$vUniversity of Wrocław, Wrocław, Poland$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, Budapest, Hungary
002705729 700__ $$aGaribov, A.$$uNNRC, Baku$$vNational Nuclear Research Center, Baku, Azerbaijan
002705729 700__ $$aGazdzicki, M.$$uJan Kochanowski U., Kielce (main)$$uFrankfurt U.$$vJan Kochanowski University in Kielce, Poland$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aGolosov, O.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aGolovatyuk, V.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aGolubeva, M.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aGrebieszkow, K.$$uWarsaw U. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aGuber, F.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aHaesler, A.$$uGeneva U.$$vUniversity of Geneva, Geneva, Switzerland
002705729 700__ $$aIgolkin, S.N.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aIlieva, S.$$uSofiya, Inst. Phys.$$vFaculty of Physics, University of Sofia, Sofia, Bulgaria
002705729 700__ $$aIvashkin, A.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aJohnson, S.R.$$uColorado U.$$vUniversity of Colorado, Boulder, USA
002705729 700__ $$aKadija, K.$$uBoskovic Inst., Zagreb$$vRuder Boškovi ́c Institute, Zagreb, Croatia
002705729 700__ $$aKargin, N.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aKashirin, E.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aKiełbowicz, M.$$uCracow, INP$$vInstitute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
002705729 700__ $$aKireyeu, V.A.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aKlochkov, V.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aKolesnikov, V.I.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aKolev, D.$$uSofiya, Inst. Phys.$$vFaculty of Physics, University of Sofia, Sofia, Bulgaria
002705729 700__ $$aKorzenev, A.$$uGeneva U.$$vUniversity of Geneva, Geneva, Switzerland
002705729 700__ $$aKovalenko, V.N.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aKowalski, S.$$uSilesia U.$$vUniversity of Silesia, Katowice, Poland
002705729 700__ $$aKoziel, M.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aKrasnoperov, A.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aKucewicz, W.$$uAGH-UST, Cracow$$vAGH - University of Science and Technology, Cracow, Poland
002705729 700__ $$aKuich, M.$$uWarsaw U. (main)$$vUniversity of Warsaw, Warsaw, Poland
002705729 700__ $$aKurepin, A.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aLarsen, D.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aLászló, A.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, Budapest, Hungary
002705729 700__ $$aLazareva, T.V.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aLewicki, M.$$uU. Wroclaw (main)$$vUniversity of Wrocław, Wrocław, Poland
002705729 700__ $$aŁojek, K.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aLyubushkin, V.V.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aMackowiak-Pawłowska, M.$$uWarsaw U. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aMajka, Z.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aMaksiak, B.$$uNCBJ, Warsaw$$vNational Centre for Nuclear Research, Warsaw, Poland
002705729 700__ $$aMalakhov, A.I.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aMarcinek, A.$$uCracow, INP$$vInstitute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
002705729 700__ $$aMarino, A.D.$$uColorado U.$$vUniversity of Colorado, Boulder, USA
002705729 700__ $$aMarton, K.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, Budapest, Hungary
002705729 700__ $$aMathes, H.J.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology, Karlsruhe, Germany
002705729 700__ $$aMatulewicz, T.$$uWarsaw U. (main)$$vUniversity of Warsaw, Warsaw, Poland
002705729 700__ $$aMatveev, V.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aMelkumov, G.L.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aMerzlaya, A.O.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aMesserly, B.$$uPittsburgh U.$$vUniversity of Pittsburgh, Pittsburgh, USA
002705729 700__ $$aMik, Ł.$$uAGH-UST, Cracow$$vAGH - University of Science and Technology, Cracow, Poland
002705729 700__ $$aMorozov, S.$$uMoscow Phys. Eng. Inst.$$uMoscow, INR$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aMrówczynski, S.$$uJan Kochanowski U., Kielce (main)$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aNagai, Y.$$uColorado U.$$vUniversity of Colorado, Boulder, USA
002705729 700__ $$aNaskret, M.$$uWroclaw U.$$vUniversity of Wrocław, Wrocław, Poland
002705729 700__ $$aOzvenchuk, V.$$uCracow, INP$$vInstitute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
002705729 700__ $$aPaolone, V.$$uPittsburgh U.$$vUniversity of Pittsburgh, Pittsburgh, USA
002705729 700__ $$aPetukhov, O.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aPłaneta, R.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aPodlaski, P.$$uWarsaw U. (main)$$vUniversity of Warsaw, Warsaw, Poland
002705729 700__ $$aPopov, B.A.$$uParis U., VI-VII$$uDubna, JINR$$vLPNHE, University of Paris VI and VII, Paris, France$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aPorfy, B.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences, Budapest, Hungary
002705729 700__ $$aPosiadała-Zezula, M.$$uWarsaw U. (main)$$vUniversity of Warsaw, Warsaw, Poland
002705729 700__ $$aProkhorova, D.S.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aPszczel, D.$$uNCBJ, Warsaw$$vNational Centre for Nuclear Research, Warsaw, Poland
002705729 700__ $$aPuławski, S.$$uSilesia U.$$vUniversity of Silesia, Katowice, Poland
002705729 700__ $$aPuzovic, J.$$uBelgrade U.$$vUniversity of Belgrade, Belgrade, Serbia
002705729 700__ $$aRavonel, M.$$uGeneva U.$$vUniversity of Geneva, Geneva, Switzerland
002705729 700__ $$aRenfordt, R.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aRöhrich, D.$$uBergen U.$$vUniversity of Bergen, Bergen, Norway
002705729 700__ $$aRondio, E.$$uNCBJ, Warsaw$$vNational Centre for Nuclear Research, Warsaw, Poland
002705729 700__ $$aRoth, M.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology, Karlsruhe, Germany
002705729 700__ $$aRumberger, B.T.$$uColorado U.$$vUniversity of Colorado, Boulder, USA
002705729 700__ $$aRumyantsev, M.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aRustamov, A.$$uFrankfurt U.$$uNNRC, Baku$$vUniversity of Frankfurt, Frankfurt, Germany$$vNational Nuclear Research Center, Baku, Azerbaijan
002705729 700__ $$aRybczynski, M.$$uJan Kochanowski U., Kielce (main)$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aRybicki, A.$$uCracow, INP$$vInstitute of Nuclear Physics, Polish Academy of Sciences, Cracow, Poland
002705729 700__ $$aSadovsky, A.$$uMoscow, INR$$vInstitute for Nuclear Research, Moscow, Russia
002705729 700__ $$aSchmidt, K.$$uSilesia U.$$vUniversity of Silesia, Katowice, Poland
002705729 700__ $$aSelyuzhenkov, I.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aSeryakov, A.Yu.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aSeyboth, P.$$uJan Kochanowski U., Kielce (main)$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aSłodkowski, M.$$uWarsaw U. of Tech. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aStaszel, P.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aStefanek, G.$$uJan Kochanowski U., Kielce (main)$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aStepaniak, J.$$uNCBJ, Warsaw$$vNational Centre for Nuclear Research, Warsaw, Poland
002705729 700__ $$aStrikhanov, M.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aStröbele, H.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aŠuša, T.$$uBoskovic Inst., Zagreb$$vRuder Boškovi ́c Institute, Zagreb, Croatia
002705729 700__ $$aTaranenko, A.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear University (Moscow Engineering Physics Institute), Moscow, Russia
002705729 700__ $$aTefelska, A.$$uWarsaw U. of Tech. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aTefelski, D.$$uWarsaw U. of Tech. (main)$$vWarsaw University of Technology, Warsaw, Poland
002705729 700__ $$aTereshchenko, V.$$uDubna, JINR$$vJoint Institute for Nuclear Research, Dubna, Russia
002705729 700__ $$aToia, A.$$uFrankfurt U.$$vUniversity of Frankfurt, Frankfurt, Germany
002705729 700__ $$aTsenov, R.$$uSofiya, Inst. Phys.$$vFaculty of Physics, University of Sofia, Sofia, Bulgaria
002705729 700__ $$aTurko, L.$$uU. Wroclaw (main)$$vUniversity of Wrocław, Wrocław, Poland
002705729 700__ $$aUlrich, R.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology, Karlsruhe, Germany
002705729 700__ $$aUnger, M.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology, Karlsruhe, Germany
002705729 700__ $$aValiev, F.F.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aVeberic, D.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology, Karlsruhe, Germany
002705729 700__ $$aVechernin, V.V.$$uSt. Petersburg State U.$$vSt. Petersburg State University, St.Petersburg, Russia
002705729 700__ $$aWickremasinghe, A.$$uFermilab$$uSt. Petersburg State U.$$vFermilab, Batavia, USA$$vUniversity of Pittsburgh, Pittsburgh, USA
002705729 700__ $$aWłodarczyk, Z.$$uJan Kochanowski U., Kielce (main)$$vJan Kochanowski University in Kielce, Poland
002705729 700__ $$aWyszynski, O.$$uJagiellonian U. (main)$$vJagiellonian University, Cracow, Poland
002705729 700__ $$aZimmerman, E.D.$$uColorado U.$$vUniversity of Colorado, Boulder, USA
002705729 700__ $$aZwaska, R.$$uFermilab$$vFermilab, Batavia, USA
002705729 700__ $$aKaptur, E.$$uSilesia U.$$vUniversity of Silesia , Katowice, Poland
002705729 700__ $$aŁysakowski, B.$$uSilesia U.$$vUniversity of Silesia , Katowice, Poland
002705729 700__ $$aRichter-Wąs, E.$$uJagiellonian U. (main)$$vJagiellonian University , Kraków, Poland
002705729 710__ $$gNA61/SHINE Collaboration
002705729 773__ $$c011901$$pPhys. Rev. C$$v102$$y2020
002705729 8564_ $$uhttps://lss.fnal.gov/archive/2019/pub/fermilab-pub-19-664-ad-scd.pdf$$yFermilab Library Server (fulltext available)
002705729 8564_ $$81594444$$s25738$$uhttps://cds.cern.ch/record/2705729/files/ppStep6_48.png$$y00008 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594445$$s11484$$uhttps://cds.cern.ch/record/2705729/files/w19_stepKM.png$$y00019 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594446$$s11484$$uhttps://cds.cern.ch/record/2705729/files/w39_stepKM.png$$y00039 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594447$$s13545$$uhttps://cds.cern.ch/record/2705729/files/w35_omegaNhp.png$$y00035 \textbf{Collision energy dependence of the scaled variance of the multiplicity distribution of charged hadrons for inelastic p+p interactions and most central Pb+Pb collisions.}
002705729 8564_ $$81594448$$s13583$$uhttps://cds.cern.ch/record/2705729/files/w37_hornKP.png$$y00037 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594449$$s25699$$uhttps://cds.cern.ch/record/2705729/files/w24_ppStepKP7_88.png$$y00020 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594450$$s27921$$uhttps://cds.cern.ch/record/2705729/files/w31_ppHorn4pi7_7.png$$y00031 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594451$$s11484$$uhttps://cds.cern.ch/record/2705729/files/w12_stepKM.png$$y00012 \textbf{Energy dependence of the inverse slope parameter $T$ of transverse mass spectra of charged kaons at mid-rapidity.}
002705729 8564_ $$81594452$$s13583$$uhttps://cds.cern.ch/record/2705729/files/w17_hornKP.png$$y00017 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594453$$s25738$$uhttps://cds.cern.ch/record/2705729/files/w32_ppStep6_48.png$$y00032 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594454$$s13583$$uhttps://cds.cern.ch/record/2705729/files/w10_hornKP.png$$y00010 \textbf{Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions.}
002705729 8564_ $$81594455$$s22730$$uhttps://cds.cern.ch/record/2705729/files/w11_hornKP4pi.png$$y00011 \textbf{Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions.}
002705729 8564_ $$81594456$$s11484$$uhttps://cds.cern.ch/record/2705729/files/w50_stepKM.png$$y00050 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are compared with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Abelev:2008ab,Abelev:2014laa,Aamodt:2011zj}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594457$$s22458$$uhttps://cds.cern.ch/record/2705729/files/w52_hornKM.png$$y00052 Energy dependence of the \km/\pim ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{left}) and in the full phase-space (\emph{right}).The \NASixtyOne results for inelastic p+p interactions are compared with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Abelev:2008ab,Abelev:2014laa,Aamodt:2011zj}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594458$$s27921$$uhttps://cds.cern.ch/record/2705729/files/w44_ppHorn4pi7_7.png$$y00044 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. }
002705729 8564_ $$81594459$$s13583$$uhttps://cds.cern.ch/record/2705729/files/hornKP.png$$y00000 Energy dependence of the \kp/\pip ratio at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well as the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are shown together with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Aamodt:2011zj,Alper:1975jm,Abelev:2008ab,Abelev:2014laa,Ahle:1998jc,Ahle:1998gv,Ahle:1999va,Ahle:1999uy,Ahle:2000wq,Barrette:1999ry,Pelte:1997rg,Bearden:2004yx,Adamczyk:2017iwn,Abelev:2013vea,Adam:2015qaa}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594460$$s11204$$uhttps://cds.cern.ch/record/2705729/files/w34_omegaNhn.png$$y00034 \textbf{Collision energy dependence of the scaled variance of the multiplicity distribution of charged hadrons for inelastic p+p interactions and most central Pb+Pb collisions.}
002705729 8564_ $$81594461$$s25738$$uhttps://cds.cern.ch/record/2705729/files/w45_ppStep6_48.png$$y00045 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. }
002705729 8564_ $$81594462$$s25699$$uhttps://cds.cern.ch/record/2705729/files/w57_ppStepKP7_88.png$$y00057 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594463$$s27921$$uhttps://cds.cern.ch/record/2705729/files/ppHorn4pi7_7.png$$y00007 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594464$$s20144$$uhttps://cds.cern.ch/record/2705729/files/w53_hornKM4pi.png$$y00053 Energy dependence of the \km/\pim ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{left}) and in the full phase-space (\emph{right}).The \NASixtyOne results for inelastic p+p interactions are compared with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Abelev:2008ab,Abelev:2014laa,Aamodt:2011zj}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594465$$s22458$$uhttps://cds.cern.ch/record/2705729/files/hornKM.png$$y00004 Energy dependence of the \km/\pim ratio at mid-rapidity (\emph{left}) and in the full phase-space (\emph{right}). The \NASixtyOne results for inelastic p+p interactions are shown together with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Aamodt:2011zj,Alper:1975jm,Abelev:2008ab,Abelev:2014laa,Ahle:1998jc,Ahle:1998gv,Ahle:1999va,Ahle:1999uy,Ahle:2000wq,Barrette:1999ry,Pelte:1997rg,Bearden:2004yx,Adamczyk:2017iwn,Abelev:2013vea,Adam:2015qaa}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594466$$s352083$$uhttps://cds.cern.ch/record/2705729/files/phase001.png$$y00016 \textbf{ Phase diagram of strongly interacting matter in the temperature T and baryon chemical potential $\mu_B$ plane with regions covered by running and planned experiments}
002705729 8564_ $$81594467$$s22730$$uhttps://cds.cern.ch/record/2705729/files/w49_hornKP4pi.png$$y00049 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are compared with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Abelev:2008ab,Abelev:2014laa,Aamodt:2011zj}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594468$$s11453$$uhttps://cds.cern.ch/record/2705729/files/w29_stepKP.png$$y00029 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594469$$s11453$$uhttps://cds.cern.ch/record/2705729/files/w40_stepKP.png$$y00040 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594470$$s25738$$uhttps://cds.cern.ch/record/2705729/files/w23_ppStep6_48.png$$y00019 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594471$$s11453$$uhttps://cds.cern.ch/record/2705729/files/w51_stepKP.png$$y00051 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are compared with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Abelev:2008ab,Abelev:2014laa,Aamodt:2011zj}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594472$$s440433$$uhttps://cds.cern.ch/record/2705729/files/1912.10871.pdf$$yFulltext
002705729 8564_ $$81594473$$s11453$$uhttps://cds.cern.ch/record/2705729/files/w20_stepKP.png$$y00020 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594474$$s36826$$uhttps://cds.cern.ch/record/2705729/files/w47_na61setup_DetectorPaper.png$$y00047 \textbf{ The schematic layout of the NA61/SHINE experiment at the CERN SPS (horizontal cut, not to scale).}
002705729 8564_ $$81594475$$s20144$$uhttps://cds.cern.ch/record/2705729/files/hornKM4pi.png$$y00005 Energy dependence of the \km/\pim ratio at mid-rapidity (\emph{left}) and in the full phase-space (\emph{right}). The \NASixtyOne results for inelastic p+p interactions are shown together with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Aamodt:2011zj,Alper:1975jm,Abelev:2008ab,Abelev:2014laa,Ahle:1998jc,Ahle:1998gv,Ahle:1999va,Ahle:1999uy,Ahle:2000wq,Barrette:1999ry,Pelte:1997rg,Bearden:2004yx,Adamczyk:2017iwn,Abelev:2013vea,Adam:2015qaa}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594476$$s11453$$uhttps://cds.cern.ch/record/2705729/files/stepKP.png$$y00003 Energy dependence of the \kp/\pip ratio at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well as the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are shown together with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Aamodt:2011zj,Alper:1975jm,Abelev:2008ab,Abelev:2014laa,Ahle:1998jc,Ahle:1998gv,Ahle:1999va,Ahle:1999uy,Ahle:2000wq,Barrette:1999ry,Pelte:1997rg,Bearden:2004yx,Adamczyk:2017iwn,Abelev:2013vea,Adam:2015qaa}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594477$$s13207$$uhttps://cds.cern.ch/record/2705729/files/ppHorn8_26.png$$y00006 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594478$$s22730$$uhttps://cds.cern.ch/record/2705729/files/w38_hornKP4pi.png$$y00038 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594479$$s11453$$uhttps://cds.cern.ch/record/2705729/files/w13_stepKP.png$$y00013 \textbf{Energy dependence of the inverse slope parameter $T$ of transverse mass spectra of charged kaons at mid-rapidity.}
002705729 8564_ $$81594480$$s20144$$uhttps://cds.cern.ch/record/2705729/files/w42_hornKM4pi.png$$y00023 \textbf{ \blue{ Energy dependence of the \km/\pim ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{left}) and in the full phase-space (\emph{right}).}}
002705729 8564_ $$81594481$$s13545$$uhttps://cds.cern.ch/record/2705729/files/omegaNhp.png$$y00015 \textbf{Collision energy dependence of the scaled variance of the multiplicity distribution of charged hadrons for inelastic p+p interactions and most central Pb+Pb collisions.}
002705729 8564_ $$81594482$$s11484$$uhttps://cds.cern.ch/record/2705729/files/stepKM.png$$y00002 Energy dependence of the \kp/\pip ratio at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well as the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are shown together with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Aamodt:2011zj,Alper:1975jm,Abelev:2008ab,Abelev:2014laa,Ahle:1998jc,Ahle:1998gv,Ahle:1999va,Ahle:1999uy,Ahle:2000wq,Barrette:1999ry,Pelte:1997rg,Bearden:2004yx,Adamczyk:2017iwn,Abelev:2013vea,Adam:2015qaa}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594483$$s25699$$uhttps://cds.cern.ch/record/2705729/files/w33_ppStepKP7_88.png$$y00033 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594484$$s11204$$uhttps://cds.cern.ch/record/2705729/files/omegaNhn.png$$y00014 \textbf{Collision energy dependence of the scaled variance of the multiplicity distribution of charged hadrons for inelastic p+p interactions and most central Pb+Pb collisions.}
002705729 8564_ $$81594485$$s11484$$uhttps://cds.cern.ch/record/2705729/files/w28_stepKM.png$$y00028 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594486$$s25699$$uhttps://cds.cern.ch/record/2705729/files/w46_ppStepKP7_88.png$$y00046 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. }
002705729 8564_ $$81594487$$s13583$$uhttps://cds.cern.ch/record/2705729/files/w48_hornKP.png$$y00048 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are compared with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Abelev:2008ab,Abelev:2014laa,Aamodt:2011zj}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594488$$s25699$$uhttps://cds.cern.ch/record/2705729/files/ppStepKP7_88.png$$y00009 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594489$$s352083$$uhttps://cds.cern.ch/record/2705729/files/w36_phase001.png$$y00036 \textbf{ Phase diagram of strongly interacting matter in the temperature T and baryon chemical potential $\mu_B$ plane with regions covered by running and planned experiments}
002705729 8564_ $$81594490$$s27921$$uhttps://cds.cern.ch/record/2705729/files/w55_ppHorn4pi7_7.png$$y00055 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594491$$s13207$$uhttps://cds.cern.ch/record/2705729/files/w30_ppHorn8_26.png$$y00030 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594492$$s22458$$uhttps://cds.cern.ch/record/2705729/files/w41_hornKM.png$$y00022 \textbf{ \blue{ Energy dependence of the \km/\pim ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{left}) and in the full phase-space (\emph{right}).}}
002705729 8564_ $$81594493$$s22730$$uhttps://cds.cern.ch/record/2705729/files/w27_hornKP4pi.png$$y00027 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594494$$s13207$$uhttps://cds.cern.ch/record/2705729/files/w54_ppHorn8_26.png$$y00054 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594495$$s25738$$uhttps://cds.cern.ch/record/2705729/files/w56_ppStep6_48.png$$y00056 Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. The experimental results are compared with predictions of the resonance-string model, UrQMD~\protect{\cite{Bleicher:1999xi}}.
002705729 8564_ $$81594496$$s13207$$uhttps://cds.cern.ch/record/2705729/files/w43_ppHorn8_26.png$$y00043 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The data are fitted by two straight lines in order to locate a position of the break in the energy dependence. }
002705729 8564_ $$81594497$$s13583$$uhttps://cds.cern.ch/record/2705729/files/w26_hornKP.png$$y00026 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594498$$s22730$$uhttps://cds.cern.ch/record/2705729/files/hornKP4pi.png$$y00001 Energy dependence of the \kp/\pip ratio at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}) as well as the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. The \NASixtyOne results for inelastic p+p interactions are shown together with the world data on p+p interactions as well as central Pb+Pb and Au+Au collisions~{\protect{\cite{Kliemant:2003sa,Aamodt:2011zj,Alper:1975jm,Abelev:2008ab,Abelev:2014laa,Ahle:1998jc,Ahle:1998gv,Ahle:1999va,Ahle:1999uy,Ahle:2000wq,Barrette:1999ry,Pelte:1997rg,Bearden:2004yx,Adamczyk:2017iwn,Abelev:2013vea,Adam:2015qaa}}}. Shaded bands show the systematic uncertainty.
002705729 8564_ $$81594499$$s27921$$uhttps://cds.cern.ch/record/2705729/files/w22_ppHorn4pi7_7.png$$y00018 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594500$$s13207$$uhttps://cds.cern.ch/record/2705729/files/w21_ppHorn8_26.png$$y00017 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons. }
002705729 8564_ $$81594501$$s22730$$uhttps://cds.cern.ch/record/2705729/files/w18_hornKP4pi.png$$y00018 \textbf{ Energy dependence of the \kp/\pip ratio in inelastic p+p interactions as well as central Pb+Pb and Au+Au collisions at mid-rapidity (\emph{top-left}) and in the full phase-space (\emph{top-right}). Energy dependence of the inverse slope parameter $T$ of transverse mass spectra at mid-rapidity for \km (\emph{bottom-left}) and \kp (\emph{bottom-right}) mesons.}
002705729 8564_ $$81594502$$s36826$$uhttps://cds.cern.ch/record/2705729/files/na61setup_DetectorPaper.png$$y00021 \textbf{ The schematic layout of the NA61/SHINE experiment at the CERN SPS (horizontal cut, not to scale).}
002705729 8564_ $$81599351$$s541364$$uhttps://cds.cern.ch/record/2705729/files/fermilab-pub-19-664-ad-scd.pdf$$yFulltext
002705729 8564_ $$82238544$$s594146$$uhttps://cds.cern.ch/record/2705729/files/scoap3-fulltext.pdf$$yArticle from SCOAP3
002705729 960__ $$a13
002705729 980__ $$aARTICLE