002059558 001__ 2059558
002059558 003__ SzGeCERN
002059558 005__ 20220810144516.0
002059558 0248_ $$aoai:cds.cern.ch:2059558$$pcerncds:CERN$$pcerncds:CERN:FULLTEXT$$pcerncds:FULLTEXT
002059558 0247_ $$2DOI$$a10.1140/epjc/s10052-016-4003-2
002059558 035__ $$9arXiv$$aoai:arXiv.org:1510.03720
002059558 035__ $$9Inspire$$a1397634
002059558 037__ $$9arXiv$$aarXiv:1510.03720$$chep-ex
002059558 037__ $$aCERN-PH-EP-2015-274
002059558 041__ $$aeng
002059558 084__ $$2CERN Library$$aPH-EP-2015-274
002059558 088__ $$9CERN-PH-EP-DRAFT-NA61-2015-002
002059558 088__ $$aCERN-PH-EP-2015-274
002059558 100__ $$aAduszkiewicz, A.$$uWarsaw U.$$vWarsaw U. - Warsaw - Poland
002059558 245__ $$aProduction of $\Lambda$ hyperons in inelastic p+p interactions at 158 GeV/$c$
002059558 269__ $$c13 Oct 2015
002059558 269__ $$aGeneva$$bCERN$$c28 Sep 2015
002059558 260__ $$c2016-04-12
002059558 300__ $$a19 p
002059558 506__ [email protected]
002059558 506__ $$mcds-edboard-na61 [CERN]
002059558 506__ $$mcds-ph-ep-publications-referee-non-lhc [CERN]
002059558 500__ $$9arXiv$$a19 pages, 20 figures, 6 tables
002059558 520__ $$aInclusive production of $\Lambda$-hyperons was measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS in inelastic p+p interactions at beam momentum of 158 GeVc. Spectra of transverse momentum and transverse mass as well as distributions of rapidity and x$_{_F}$ are presented. The mean multiplicity was estimated to be $0.120\,\pm0.006\;(stat.)\,\pm 0.010\;(sys.)$. The results are compared with previous measurements and predictions of the EPOS, UrQMD and FRITIOF models.
002059558 520__ $$9HEPDATA$$hCERN-NA. Inclusive production of $\Lambda$-hyperons was measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS in inelastic p+p interactions at beam momentum of 158 GeV/$c$. Spectra of transverse momentum and transverse mass as well as distributions of rapidity and x$_{_F}$ are presented. The mean multiplicity was estimated to be $0.120 \pm 0.006(stat.) \pm 0.010(sys.)$. The results are compared with previous measurements and predictions of the EPOS, UrQMD and FRITIOF models.
002059558 520__ $$9Springer$$aInclusive production of $\Lambda $ -hyperons was measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS in inelastic p+p interactions at beam momentum of 158 ${\mathrm{GeV}}\!/\!c$ . Spectra of transverse momentum and transverse mass as well as distributions of rapidity and x$_{_F}$ are presented. The mean multiplicity was estimated to be $0.120\,{\pm }\,0.006\,(stat.)\,{\pm }0.010\,(sys.)$ . The results are compared with previous measurements and predictions of the Epos, Urqmd and Fritiof models.
002059558 520__ $$9arXiv$$aInclusive production of $\Lambda$-hyperons was measured with the large acceptance NA61/SHINE spectrometer at the CERN SPS in inelastic p+p interactions at beam momentum of 158~\GeVc. Spectra of transverse momentum and transverse mass as well as distributions of rapidity and x$_{_F}$ are presented. The mean multiplicity was estimated to be $0.120\,\pm0.006\;(stat.)\,\pm 0.010\;(sys.)$. The results are compared with previous measurements and predictions of the EPOS, UrQMD and FRITIOF models.
002059558 540__ $$3preprint$$aCC-BY-4.0
002059558 540__ $$3publication$$aCC-BY-4.0$$fSCOAP3
002059558 542__ $$3preprint$$dCERN$$g2015
002059558 542__ $$3publication$$dThe Author(s)$$g2016
002059558 562__ $$cComments submitted after 09-11-2015 16:48
002059558 595__ $$aCERN-PH-EP
002059558 595__ $$aCERN EDS
002059558 595__ $$aLANL EDS
002059558 65017 $$2arXiv$$aParticle Physics - Experiment
002059558 65027 $$2arXiv$$aNuclear Physics - Experiment
002059558 6531_ $$9CERN$$aQCD
002059558 6531_ $$9CERN$$arelativistic heavy ion physics
002059558 6531_ $$9CERN$$aquark gluon plasma
002059558 6531_ $$9CERN$$aparticle and resonance production
002059558 6531_ $$9CERN$$aexperimental results
002059558 6531_ $$9CERN$$aInclusive production with identified hadrons
002059558 6531_ $$9CERN$$aInelastic scattering: many-particle final states
002059558 6531_ $$9CERN$$aHyperons
002059558 693__ $$aCERN SPS$$eSHINE NA61
002059558 695__ $$9LANL EDS$$ahep-ex
002059558 695__ $$9LANL EDS$$anucl-ex
002059558 690C_ $$aCERN
002059558 690C_ $$aARTICLE
002059558 690C_ $$aNA61_Papers
002059558 700__ $$aAli, Y.$$uJagiellonian U.$$vJagiellonian U.$$vDepartment of Physics - COMSATS Institute of Information Technology - Islamabad - 44000 - Pakistan
002059558 700__ $$aAndronov, E.$$uSt. Petersburg State U.$$vSt. Petersburg State U. - St. Petersburg - Russia
002059558 700__ $$aAntićić, T.$$uBoskovic Inst., Zagreb$$vRuđer Bošković Institute - Zagreb - Croatia
002059558 700__ $$aAntoniou, N.$$uAthens U.$$vAthens U. - Athens - Greece
002059558 700__ $$aBaatar, B.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aBay, F.$$uZurich, ETH$$vETH Zürich - Zürich - Switzerland
002059558 700__ $$aBlondel, A.$$uU. Geneva (main)$$vGeneva U. - Geneva - Switzerland
002059558 700__ $$aBogomilov, M.$$uSofiya U.$$vFaculty of Physics - Sofia U. - Sofia - Bulgaria
002059558 700__ $$aBrandin, A.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear U. “MEPhI” (Moscow Engineering Physics Institute) - Moscow - Russia
002059558 700__ $$aBravar, A.$$uGeneva U.$$vGeneva U. - Geneva - Switzerland
002059558 700__ $$aBrzychczyk, J.$$uJagiellonian U.$$vJagiellonian U.
002059558 700__ $$aBunyatov, S.A.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aBusygina, O.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia
002059558 700__ $$aChristakoglou, P.$$uAthens U.$$vAthens U. - Athens - Greece
002059558 700__ $$aĆirković, M.$$uBelgrade U.$$vBelgrade U. - Belgrade - Serbia
002059558 700__ $$aCzopowicz, T.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aDamyanova, A.$$uGeneva U.$$vGeneva U. - Geneva - Switzerland
002059558 700__ $$aDavis, N.$$uGeneva U.$$vAthens U. - Athens - Greece
002059558 700__ $$aDembinski, H.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aDeveaux, M.$$uFrankfurt U., Inst. Kernphys.$$vFrankfurt U. - Frankfurt - Germany
002059558 700__ $$aDiakonos, F.$$uAthens U.$$vAthens U. - Athens - Greece
002059558 700__ $$aDi Luise, S.$$uZurich, ETH$$vETH Zürich - Zürich - Switzerland
002059558 700__ $$aDominik, W.$$uWarsaw U.$$vWarsaw U. - Warsaw - Poland
002059558 700__ $$aDumarchez, J.$$uParis U., VI-VII$$vLPNHE - Paris VI U. and VII - Paris - France
002059558 700__ $$aDynowski, K.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aEngel, R.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aEreditato, A.$$uU. Bern (main)$$vBern U. - Bern - Switzerland
002059558 700__ $$aFeofilov, G.A.$$uSt. Petersburg State U.$$vSt. Petersburg State U. - St. Petersburg - Russia
002059558 700__ $$aFodor, Z.$$uWigner RCP, Budapest$$uU. Wroclaw (main)$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences - Budapest - Hungary$$vWrocław U. - Wrocław - Poland
002059558 700__ $$aGaribov, A.$$uNNRC, Baku$$vNational Nuclear Research Center - Baku - Azerbaijan
002059558 700__ $$aGazdzicki, M.$$uFrankfurt U.$$uJan Kochanowski U.$$vFrankfurt U. - Frankfurt - Germany$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aGolubeva, M.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia
002059558 700__ $$aGrebieszkow, K.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aGrzeszczuk, A.$$uSilesia U.$$vSilesia U. - Katowice - Poland
002059558 700__ $$aGuber, F.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia
002059558 700__ $$aHaesler, A.$$uGeneva U.$$vGeneva U. - Geneva - Switzerland
002059558 700__ $$aHasegawa, T.$$uKEK, Tsukuba$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aHervé, A.E.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aHierholzer, M.$$uBern U.$$vBern U. - Bern - Switzerland
002059558 700__ $$aIgolkin, S.$$uSt. Petersburg State U.$$vSt. Petersburg State U. - St. Petersburg - Russia
002059558 700__ $$aIvashkin, A.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia
002059558 700__ $$aJohnson, S.R.$$uColorado U.$$vColorado U. - Boulder - USA
002059558 700__ $$aKadija, K.$$uBoskovic Inst., Zagreb$$vRuđer Bošković Institute - Zagreb - Croatia
002059558 700__ $$aKapoyannis, A.$$uAthens U.$$vAthens U. - Athens - Greece
002059558 700__ $$aKaptur, E.$$uSilesia U.$$vSilesia U. - Katowice - Poland
002059558 700__ $$aKisiel, J.$$uSilesia U.$$vSilesia U. - Katowice - Poland
002059558 700__ $$aKobayashi, T.$$uINS, Tokyo$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aKolesnikov, V.I.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aKolev, D.$$uSofiya U.$$vFaculty of Physics - Sofia U. - Sofia - Bulgaria
002059558 700__ $$aKondratiev, V.P.$$uSt. Petersburg State U.$$vSt. Petersburg State U. - St. Petersburg - Russia
002059558 700__ $$aKorzenev, A.$$uGeneva U.$$vGeneva U. - Geneva - Switzerland
002059558 700__ $$aKowalik, K.$$uNCBJ, Swierk$$vNational Centre for Nuclear Research - Warsaw - Poland
002059558 700__ $$aKowalski, S.$$uSilesia U.$$vSilesia U. - Katowice - Poland
002059558 700__ $$aKoziel, M.$$uFrankfurt U.$$vFrankfurt U. - Frankfurt - Germany
002059558 700__ $$aKrasnoperov, A.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aKuich, M.$$uWarsaw U.$$vWarsaw U. - Warsaw - Poland
002059558 700__ $$aKurepin, A.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia
002059558 700__ $$aLarsen, D.$$uJagiellonian U.$$vJagiellonian U.
002059558 700__ $$aLászló, A.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences - Budapest - Hungary
002059558 700__ $$aLewicki, M.$$uWroclaw U.$$vWrocław U. - Wrocław - Poland
002059558 700__ $$aLyubushkin, V.V.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aMaćkowiak-Pawłowska, M.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aMaksiak, B.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aMalakhov, A.I.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aManić, D.$$uBelgrade U.$$vBelgrade U. - Belgrade - Serbia
002059558 700__ $$aMarcinek, A.$$uJagiellonian U.$$uWroclaw U.$$vWrocław U. - Wrocław - Poland
002059558 700__ $$aMarino, A.D.$$uColorado U.$$vColorado U. - Boulder - USA
002059558 700__ $$aMarton, K.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences - Budapest - Hungary
002059558 700__ $$aMathes, H.J.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aMatulewicz, T.$$uWarsaw U.$$vWarsaw U. - Warsaw - Poland
002059558 700__ $$aMatveev, V.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aMelkumov, G.L.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aMesserly, B.$$uPittsburgh U.$$vPittsburgh U. - Pittsburgh - USA
002059558 700__ $$aMills, G.B.$$uLos Alamos$$vLos Alamos National Laboratory - Los Alamos - USA
002059558 700__ $$aMorozov, S.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia$$vNational Research Nuclear U. “MEPhI” (Moscow Engineering Physics Institute) - Moscow - Russia
002059558 700__ $$aMrówczyński, S.$$uJan Kochanowski U.$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aNagai, Y.$$uColorado U.$$vColorado U. - Boulder - USA
002059558 700__ $$aNakadaira, T.$$uKEK, Tsukuba$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aNaskręt, M.$$uWroclaw U.$$vWrocław U. - Wrocław - Poland
002059558 700__ $$aNirkko, M.$$uU. Bern (main)$$vBern U. - Bern - Switzerland
002059558 700__ $$aNishikawa, K.$$uKEK, Tsukuba$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aPanagiotou, A.D.$$uAthens U.$$vAthens U. - Athens - Greece
002059558 700__ $$aPaolone, V.$$uPittsburgh U.$$vPittsburgh U. - Pittsburgh - USA
002059558 700__ $$aPavin, M.$$uBoskovic Inst., Zagreb$$uParis U., VI-VII$$vRuđer Bošković Institute - Zagreb - Croatia$$vLPNHE - Paris VI U. and VII - Paris - France
002059558 700__ $$aPetukhov, O.$$uMoscow, INR$$uMoscow Phys. Eng. Inst.$$vInstitute for Nuclear Research - Moscow - Russia$$vNational Research Nuclear U. “MEPhI” (Moscow Engineering Physics Institute) - Moscow - Russia
002059558 700__ $$aPistillo, C.$$uU. Bern (main)$$vBern U. - Bern - Switzerland
002059558 700__ $$aPłaneta, R.$$uJagiellonian U.$$vJagiellonian U.
002059558 700__ $$aPopov, B.A.$$uDubna, JINR$$uParis U., VI-VII$$vLPNHE - Paris VI U. and VII - Paris - France$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aPosiadała, M.$$uWarsaw U.$$vWarsaw U. - Warsaw - Poland
002059558 700__ $$aPuławski, S.$$uSilesia U.$$vSilesia U. - Katowice - Poland
002059558 700__ $$aPuzović, J.$$uBelgrade U.$$vBelgrade U. - Belgrade - Serbia
002059558 700__ $$aRauch, W.$$uFachhochschule Frankfurt$$vFachhochschule Frankfurt - Frankfurt - Germany
002059558 700__ $$aRavonel, M.$$uGeneva U.$$vGeneva U. - Geneva - Switzerland
002059558 700__ $$aRedij, A.$$uBern U.$$vBern U. - Bern - Switzerland
002059558 700__ $$aRenfordt, R.$$uFrankfurt U., Inst. Kernphys.$$vFrankfurt U. - Frankfurt - Germany
002059558 700__ $$aRichter-Wąs, E.$$uJagiellonian U.$$vJagiellonian U.
002059558 700__ $$aRobert, A.$$uParis U., VI-VII$$vLPNHE - Paris VI U. and VII - Paris - France
002059558 700__ $$aRöhrich, D.$$uBergen U.$$vBergen U. - Bergen - Norway
002059558 700__ $$aRondio, E.$$uNCBJ, Swierk$$vNational Centre for Nuclear Research - Warsaw - Poland
002059558 700__ $$aRoth, M.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aRubbia, A.$$uZurich, ETH$$vETH Zürich - Zürich - Switzerland
002059558 700__ $$aRumberger, B.T.$$uColorado U.$$vColorado U. - Boulder - USA
002059558 700__ $$aRustamov, A.$$uFrankfurt U., Inst. Kernphys.$$uNNRC, Baku$$vNational Nuclear Research Center - Baku - Azerbaijan$$vFrankfurt U. - Frankfurt - Germany
002059558 700__ $$aRybczynski, M.$$uJan Kochanowski U.$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aSadovsky, A.$$uMoscow, INR$$vInstitute for Nuclear Research - Moscow - Russia
002059558 700__ $$aSakashita, K.$$uKEK, Tsukuba$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aSchmidt, K.$$uSilesia U.$$vSilesia U. - Katowice - Poland
002059558 700__ $$aSekiguchi, T.$$uWarsaw U. of Tech.$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aSelyuzhenkov, I.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear U. “MEPhI” (Moscow Engineering Physics Institute) - Moscow - Russia
002059558 700__ $$aSeryakov, A.$$uSt. Petersburg State U.$$vSt. Petersburg State U. - St. Petersburg - Russia
002059558 700__ $$aSeyboth, P.$$uJan Kochanowski U.$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aSgalaberna, D.$$uZurich, ETH$$vETH Zürich - Zürich - Switzerland
002059558 700__ $$aShibata, M.$$uKEK, Tsukuba$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aSłodkowski, M.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aStaszel, P.$$uJagiellonian U.$$vJagiellonian U.
002059558 700__ $$aStepaniak, J.$$uJan Kochanowski U.$$vNational Centre for Nuclear Research - Warsaw - Poland
002059558 700__ $$aStefanek, G.$$uJan Kochanowski U.$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aStröbele, H.$$uNCBJ, Swierk$$vFrankfurt U. - Frankfurt - Germany
002059558 700__ $$aŠuša, T.$$jORCID:0000-0001-7430-2552$$uFrankfurt U., Inst. Kernphys.$$vRuđer Bošković Institute - Zagreb - Croatia
002059558 700__ $$aSzuba, M.$$uBoskovic Inst., Zagreb$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aTada, M.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aTaranenko, A.$$uKEK, Tsukuba$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aTefelski, D.$$uMoscow Phys. Eng. Inst.$$vNational Research Nuclear U. “MEPhI” (Moscow Engineering Physics Institute) - Moscow - Russia
002059558 700__ $$aTereshchenko, V.$$uWarsaw U. of Tech.$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aTsenov, R.$$uWarsaw U. of Tech.$$vWarsaw Technology U. - Warsaw - Poland
002059558 700__ $$aTurko, L.$$uDubna, JINR$$vJoint Institute for Nuclear Research - Dubna - Russia
002059558 700__ $$aUlrich, R.$$uSofiya U.$$vFaculty of Physics - Sofia U. - Sofia - Bulgaria
002059558 700__ $$aUnger, M.$$uWroclaw U.$$vWrocław U. - Wrocław - Poland
002059558 700__ $$aVassiliou, M.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aVeberič, D.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aVechernin, V.V.$$uAthens U.$$vAthens U. - Athens - Greece
002059558 700__ $$aVesztergombi, G.$$uKIT, Karlsruhe$$vKarlsruhe Institute of Technology - Karlsruhe - Germany
002059558 700__ $$aVinogradov, L.$$uSt. Petersburg State U.$$vSt. Petersburg State U. - St. Petersburg - Russia
002059558 700__ $$aWilczek, A.$$uWigner RCP, Budapest$$vWigner Research Centre for Physics of the Hungarian Academy of Sciences - Budapest - Hungary
002059558 700__ $$aWłodarczyk, Z.$$uJan Kochanowski U.$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aWojtaszek-Szwarc, A.$$uSilesia U.$$vJan Kochanowski U. in Kielce - Kielce - Poland
002059558 700__ $$aWyszyński, O.$$uJan Kochanowski U.$$vJagiellonian U.
002059558 700__ $$aZambelli, L.$$uJan Kochanowski U.$$vLPNHE - Paris VI U. and VII - Paris - France$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aZimmerman, E.D.$$uColorado U.$$vColorado U. - Boulder - USA
002059558 700__ $$aZambelli, L.$$uParis U., VI-VII$$uKEK, Tsukuba$$vLPNHE - Paris VI U. and VII - Paris - France$$vInstitute for Particle and Nuclear Studies - Tsukuba - Japan
002059558 700__ $$aZimmermann, E.D.$$uColorado U.
002059558 710__ $$gNA61/SHINE Collaboration
002059558 773__ $$c198$$pEur. Phys. J. C$$v76$$y2016
002059558 859__ [email protected]
002059558 8564_ $$s1735971$$uhttp://inspirehep.net/record/1397634/files/scoap3-fulltext.pdf?subformat=pdfa$$xpdfa$$yArticle from SCOAP3
002059558 8564_ $$81178995$$s946462$$uhttps://cds.cern.ch/record/2059558/files/arXiv:1510.03720.pdf
002059558 8564_ $$81178976$$s20519$$uhttps://cds.cern.ch/record/2059558/files/epsilonypT.png$$y00010 Correction factors $c_{_{MC}}$ for binning in ($y,p_T$) at top, ($y,m_T-m_{\Lambda}$) at centre and ($x_F,p_T$) at bottom. The error $\Delta c_{_{MC}}$ ranges from 0.02 to 1.48 for binning in ($y,p_T$) and ($y,m_T$), and from 0.02 to 8.70 for ($x_F,p_T$).
002059558 8564_ $$81178977$$s22464$$uhttps://cds.cern.ch/record/2059558/files/bxyDef.png$$y00001 Definition of distance of the closest approach (dca), and $b_x$. The variable $b_y$ is defined on the yz-plane in analogy with $b_x$. The target plane is defined as the plane parallel to the xy-plane containing the main vertex marked with a cross (taken from Ref. \cite{Yates}).
002059558 8564_ $$81178978$$s26620$$uhttps://cds.cern.ch/record/2059558/files/31FULL.png$$y00007 The invariant mass distribution of $\Lambda$ candidates for $y\in[-0.25,0.25]$ and $p_{_T}\in[0.2,0.4]$ \GeVc with the LH inserted after subtraction of the fitted background (a), and for the simulation (b).
002059558 8564_ $$81178979$$s12038$$uhttps://cds.cern.ch/record/2059558/files/na49comp.png$$y00022 Rapidity spectra of $\Lambda$ hyperons divided by the mean number of wounded nucleons in inelastic p+p interactions (\NASixtyOne) and central C+C, Si+Si~\cite{CCSiSi}, and Pb+Pb~\cite{PbPb} collisions at 158~\AGeVc.
002059558 8564_ $$81178980$$s32696$$uhttps://cds.cern.ch/record/2059558/files/xFRewMulti.png$$y00018 Spectra $f_n$ for eight bins in $x_{_F}$. The fitted function was obtained from Eq.~(\ref{eq:scaling}) by multiplying the right-hand side by $p_{_T}$. The numerical data are listed in Table~\ref{tab:d2ndxFdpT} for $x_{_F} > 0 $ and in Table~\ref{tab:2d2ndxFdpT} for $x_{_F} < 0$.
002059558 8564_ $$81178981$$s25082$$uhttps://cds.cern.ch/record/2059558/files/armenAfter.png$$y00005 Armenteros-Podolanski plot for reconstructed $V^0$ decays before the $\Lambda$ candidate selection cuts (a), and after the cuts are applied (b). The shading indicates the number of entries per bin. The axis variables are: $p_T^{Arm}$, the transverse momentum of the decay particles with respect to the direction of motion of the $V^0$ and $\alpha^{Arm} = (p_L^+ - p_L^-)/(p_L^+ + p_L^-)$ where $p_L^+$ and $p_L^-$ are the longitudinal momenta of the positive and negative decay particle respectively.
002059558 8564_ $$81178982$$s24515$$uhttps://cds.cern.ch/record/2059558/files/lambdaFit_y2pT1.png$$y00006 The invariant mass distribution of $\Lambda$ candidates for $y\in[-0.75,-0.25]$ and $p_{_T}\in[0.2,0.4]$ \GeVc is shown in the upper plot (LH inserted). The solid line shows a fit to signal plus background, while the dashed line represents the background contribution. The lower part of the plot shows the difference between the data points and the fit, normalised to the statistical error of the data points.
002059558 8564_ $$81178983$$s7705$$uhttps://cds.cern.ch/record/2059558/files/lifetime_vs_y.png$$y00014 {\it Top:} An example of the corrected proper life-time distribution for $\Lambda$ hyperons produced in inelastic p+p interactions at 158~\GeVc in the rapidity interval y=-1.0$\pm$0.25. {\it Bottom:} The ratio of the fitted mean life-time to its PDG~\cite{PDG} value as a function of rapidity.
002059558 8564_ $$81178984$$s34965$$uhttps://cds.cern.ch/record/2059558/files/worldxF.png$$y00021 Comparison of the invariant $x_{F}$ spectra (see Eq.~(\ref{eq:Fsigma}), $\sigma_{inel.}=31.8$~mb~\cite{PDG}) from the \NASixtyOne with the data from bubble-chamber experiments at beam momenta close to 158~\GeVc~\cite{Ammosov,Brick,Jaeger,Sheng,Asai,Kichimi}. The \NASixtyOne data points are indicated by filled circles. The systematic uncertainty is shown as a band around the points.
002059558 8564_ $$81178985$$s44922$$uhttps://cds.cern.ch/record/2059558/files/armenBefore.png$$y00004 Armenteros-Podolanski plot for reconstructed $V^0$ decays before the $\Lambda$ candidate selection cuts (a), and after the cuts are applied (b). The shading indicates the number of entries per bin. The axis variables are: $p_T^{Arm}$, the transverse momentum of the decay particles with respect to the direction of motion of the $V^0$ and $\alpha^{Arm} = (p_L^+ - p_L^-)/(p_L^+ + p_L^-)$ where $p_L^+$ and $p_L^-$ are the longitudinal momenta of the positive and negative decay particle respectively.
002059558 8564_ $$81178986$$s18970$$uhttps://cds.cern.ch/record/2059558/files/phiDef.png$$y00003 Definition of $\phi$-variable used for the $V^{0}$ selection (see text).
002059558 8564_ $$81178987$$s39284$$uhttps://cds.cern.ch/record/2059558/files/mcAllModels.png$$y00024 Comparison of $\frac{dn}{dy}$ (a), and $\frac{dn}{dx_{_F}}$ (b) distributions with calculations of the \Epos~\cite{EPOS}, \Urqmd~\cite{UrQMD1,UrQMD2} and \Fritiof~\cite{FRITIOF} models. The chain line was used to extrapolate the \NASixtyOne measurements to full phase space. For details see text.
002059558 8564_ $$81178988$$s35960$$uhttps://cds.cern.ch/record/2059558/files/mTMulti.png$$y00016 Spectra $\frac{d^2n}{dydm_{_T}}$ for six bins in rapidity $y$. The fitted function is given by Eq.~(\ref{eq:scaling}). The numerical data are listed in Table~\ref{tab:d2ndydmT} and the mean transverse mass $\langle m_{_T}\rangle -m_{_\Lambda}$ for each of the bins in Table~\ref{tab:dndy}.
002059558 8564_ $$81178989$$s20063$$uhttps://cds.cern.ch/record/2059558/files/epsilonxFpT.png$$y00012 Correction factors $c_{_{MC}}$ for binning in ($y,p_T$) at top, ($y,m_T-m_{\Lambda}$) at centre and ($x_F,p_T$) at bottom. The error $\Delta c_{_{MC}}$ ranges from 0.02 to 1.48 for binning in ($y,p_T$) and ($y,m_T$), and from 0.02 to 8.70 for ($x_F,p_T$).
002059558 8564_ $$81178990$$s33889$$uhttps://cds.cern.ch/record/2059558/files/meanLambdaPt.png$$y00020 Collision energy dependence of mean multiplicity of $\Lambda$ hyperons produced in inelastic p+p interactions. Full symbols indicate bubble chamber results~\cite{Ammosov,Chapman,Brick,Jaeger,LoPinto}, the solid red dot shows the \NASixtyOne result. Open symbols depict the remaining world data~\cite{Marek}. The \EposLong~\cite{EPOS} prediction is shown by the curve. The systematic uncertainty of the \NASixtyOne result is indicated by the shaded bar.
002059558 8564_ $$81178991$$s39299$$uhttps://cds.cern.ch/record/2059558/files/na49midComp.png$$y00023 Spectra of m$_{_T}$ at mid-rapidity ($|y|\leq0.4$ for A+A, $|y|\leq0.25$ for p+p) from \NASixtyOne inelastic p+p interactions and central C+C, Si+Si~\cite{CCSiSi}, and Pb+Pb~\cite{PbPb} collisions for beam momentum of 158~\AGeVc. The lines are fitted using Eq.~(\ref{eq:scaling}).
002059558 8564_ $$81178992$$s37591$$uhttps://cds.cern.ch/record/2059558/files/world.png$$y00019 The scaled $\Lambda$ yield as function of scaled rapidity $z=y/y_{beam}$ in inelastic p+p interactions measured by \NASixtyOne and selected bubble-chamber experiments~\cite{Ammosov,Chapman,Brick,Jaeger,LoPinto}. The symmetric polynomial of 4$^{th}$ order used for estimation of the systematic uncertainty of $\Lambda$ mean multiplicity (see Sec.~\ref{subs:spectra}) is plotted to guide the eye.
002059558 8564_ $$81178993$$s38884$$uhttps://cds.cern.ch/record/2059558/files/mcAllModelsxF.png$$y00025 Comparison of $\frac{dn}{dy}$ (a), and $\frac{dn}{dx_{_F}}$ (b) distributions with calculations of the \Epos~\cite{EPOS}, \Urqmd~\cite{UrQMD1,UrQMD2} and \Fritiof~\cite{FRITIOF} models. The chain line was used to extrapolate the \NASixtyOne measurements to full phase space. For details see text.
002059558 8564_ $$81178994$$s40146$$uhttps://cds.cern.ch/record/2059558/files/xFMulti.png$$y00017 Spectra $\frac{d^2n}{dx_{_F}dp_{_T}}$ for eight bins in $x_{_F}$. The fitted function is given by Eq.~(\ref{eq:scaling}). The numerical data are listed in Table~\ref{tab:d2ndxFdpT} for $x_{_F} > 0$ and in Table~\ref{tab:2d2ndxFdpT} for $x_{_F} > 0$.
002059558 8564_ $$81178996$$s18616$$uhttps://cds.cern.ch/record/2059558/files/cosThetaDef.png$$y00002 Definition of $\Delta z$ variable used for the $V^{0}$ selection (see text).
002059558 8564_ $$81178997$$s19377$$uhttps://cds.cern.ch/record/2059558/files/epsilonymT.png$$y00011 Correction factors $c_{_{MC}}$ for binning in ($y,p_T$) at top, ($y,m_T-m_{\Lambda}$) at centre and ($x_F,p_T$) at bottom. The error $\Delta c_{_{MC}}$ ranges from 0.02 to 1.48 for binning in ($y,p_T$) and ($y,m_T$), and from 0.02 to 8.70 for ($x_F,p_T$).
002059558 8564_ $$81178998$$s10482$$uhttps://cds.cern.ch/record/2059558/files/lifetime_t1.png$$y00013 {\it Top:} An example of the corrected proper life-time distribution for $\Lambda$ hyperons produced in inelastic p+p interactions at 158~\GeVc in the rapidity interval y=-1.0$\pm$0.25. {\it Bottom:} The ratio of the fitted mean life-time to its PDG~\cite{PDG} value as a function of rapidity.
002059558 8564_ $$81178999$$s7357$$uhttps://cds.cern.ch/record/2059558/files/feeddown.png$$y00009 Feed-down correction: the contribution from $\Xi^-$ and $\Xi^0$ to total $\Lambda$ decays calculated using \EposLong model.
002059558 8564_ $$81179000$$s36643$$uhttps://cds.cern.ch/record/2059558/files/pTMulti.png$$y00015 Spectra $\frac{d^2n}{dydp_{_T}}$ for six bins in rapidity $y$. The fitted function is given by Eq.~(\ref{eq:scaling}). The numerical data are listed in the Table~\ref{tab:d2ndydpT} and the fitted inverse slope parameter for each of the bins in Table~\ref{tab:dndy}.
002059558 8564_ $$81179001$$s37293$$uhttps://cds.cern.ch/record/2059558/files/na61A.png$$y00000 Schematic layout of the NA61/SHINE experiment at the CERN SPS (horizontal cut in the beam plane, not to scale). The beam and trigger counter configuration used for data taking on p+p interactions in 2009 is presented. The chosen right-handed coordinate system is shown on the plot. The incoming beam direction is along the z axis. The magnetic field bends charged particle trajectories in the x-z (horizontal) plane. The drift direction in the TPCs is along the y (vertical) axis~\cite{Facility}. See details in Section~\ref{sec:setup}.
002059558 8564_ $$81179002$$s22814$$uhttps://cds.cern.ch/record/2059558/files/31EPOS.png$$y00008 The invariant mass distribution of $\Lambda$ candidates for $y\in[-0.25,0.25]$ and $p_{_T}\in[0.2,0.4]$ \GeVc with the LH inserted after subtraction of the fitted background (a), and for the simulation (b).
002059558 8564_ $$81194971$$s1735971$$uhttps://cds.cern.ch/record/2059558/files/Eur. Phys. J. C 76 (2016) 198.pdf$$ySpringer Open Access article
002059558 8564_ $$81194971$$s5283853$$uhttps://cds.cern.ch/record/2059558/files/Eur. Phys. J. C 76 (2016) 198.pdf?subformat=pdfa$$xpdfa$$ySpringer Open Access article
002059558 8564_ $$81402318$$s1735971$$uhttps://cds.cern.ch/record/2059558/files/scoap3-fulltext.pdf?subformat=pdfa$$xpdfa$$yArticle from SCOAP3
002059558 8564_ $$82333903$$s1735971$$uhttps://cds.cern.ch/record/2059558/files/scoap.pdf$$yArticle from SCOAP3
002059558 9031_ $$aApproval requested for number CERN-PH-EP-2015-274$$bCERN-PH-EP-2015-274$$cEPPHAPP$$d2015-09-28 19:18:19$$e2015-10-05 19:18:[email protected]$$swaiting
002059558 9031_ $$aDocument approved$$bCERN-PH-EP-2015-274$$cEPPHAPP$$d2015-10-05 10:51:[email protected]$$sapproved
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