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Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions

The NA44 collaboration has measured charged kaon and pion distributions at midrapidity in sulphur and proton collisions with nuclear targets at 200 and 450 GeV/c per nucleon, respectively. The inverse slopes of kaons are larger than those of pions. The difference in the inverse slopes of pions, kaon...

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Autores principales: Boggild, H., Boissevain, J., Dodd, J., Esumi, S., Fabjan, C.W., Fields, D.E., Franz, A., Hansen, K.H., Humanic, T.J., Jacak, B.V., Kalechofsky, H., Lee, Y.Y., Leltchouk, M., Lorstad, B., Maeda, N., Miyabayashi, A., Murray, M., Nishimura, S., Pandey, S.U., Piuz, F., Polychronakos, V., Potekhin, M., Poulard, G., Sakaguchi, A., Sarabura, M., Simon-Gillo, J., Schmidt-Sorensen, J., Sondheim, W., Sugitate, T., Sullivan, J.P., Sumi, Y., van Hecke, H., Willis, W.J., Wolf, K.
Lenguaje:eng
Publicado: 1999
Materias:
Acceso en línea:https://dx.doi.org/10.1103/PhysRevC.59.328
http://cds.cern.ch/record/362434
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author Boggild, H.
Boissevain, J.
Dodd, J.
Esumi, S.
Fabjan, C.W.
Fields, D.E.
Franz, A.
Hansen, K.H.
Humanic, T.J.
Jacak, B.V.
Kalechofsky, H.
Lee, Y.Y.
Leltchouk, M.
Lorstad, B.
Maeda, N.
Miyabayashi, A.
Murray, M.
Nishimura, S.
Pandey, S.U.
Piuz, F.
Polychronakos, V.
Potekhin, M.
Poulard, G.
Sakaguchi, A.
Sarabura, M.
Simon-Gillo, J.
Schmidt-Sorensen, J.
Sondheim, W.
Sugitate, T.
Sullivan, J.P.
Sumi, Y.
van Hecke, H.
Willis, W.J.
Wolf, K.
author_facet Boggild, H.
Boissevain, J.
Dodd, J.
Esumi, S.
Fabjan, C.W.
Fields, D.E.
Franz, A.
Hansen, K.H.
Humanic, T.J.
Jacak, B.V.
Kalechofsky, H.
Lee, Y.Y.
Leltchouk, M.
Lorstad, B.
Maeda, N.
Miyabayashi, A.
Murray, M.
Nishimura, S.
Pandey, S.U.
Piuz, F.
Polychronakos, V.
Potekhin, M.
Poulard, G.
Sakaguchi, A.
Sarabura, M.
Simon-Gillo, J.
Schmidt-Sorensen, J.
Sondheim, W.
Sugitate, T.
Sullivan, J.P.
Sumi, Y.
van Hecke, H.
Willis, W.J.
Wolf, K.
author_sort Boggild, H.
collection CERN
description The NA44 collaboration has measured charged kaon and pion distributions at midrapidity in sulphur and proton collisions with nuclear targets at 200 and 450 GeV/c per nucleon, respectively. The inverse slopes of kaons are larger than those of pions. The difference in the inverse slopes of pions, kaons and protons, all measured in our spectrometer, increases with system size and is consistent with the buildup of collective flow for larger systems. The target dependence of both the yields and inverse slopes is stronger for the sulphur beam suggesting the increased importance of secondary rescattering for SA reactions. The rapidity density, dN/dy, of both K+ and K- increases more rapidly with system size than for pi+ in a similar rapidity region. This trend continues with increasing centrality, and according to RQMD, it is caused by secondary reactions between mesons and baryons. The K-/K+ ratio falls with increasing system size but more slowly than the pbar/p ratio. The pi-/pi+ ratio is close to unity for all systems. From pBe to SPb the K+/p ratio decreases while K-/pbar increases and ({K+*K-}/{p*pbar})**1/2 stays constant. These data suggest that as larger nuclei collide, the resulting system has a larger transverse expansion, baryon density and an increasing fraction of strange quarks.
id cern-362434
institution Organización Europea para la Investigación Nuclear
language eng
publishDate 1999
record_format invenio
spelling cern-3624342021-10-08T02:24:31Zdoi:10.1103/PhysRevC.59.328http://cds.cern.ch/record/362434engBoggild, H.Boissevain, J.Dodd, J.Esumi, S.Fabjan, C.W.Fields, D.E.Franz, A.Hansen, K.H.Humanic, T.J.Jacak, B.V.Kalechofsky, H.Lee, Y.Y.Leltchouk, M.Lorstad, B.Maeda, N.Miyabayashi, A.Murray, M.Nishimura, S.Pandey, S.U.Piuz, F.Polychronakos, V.Potekhin, M.Poulard, G.Sakaguchi, A.Sarabura, M.Simon-Gillo, J.Schmidt-Sorensen, J.Sondheim, W.Sugitate, T.Sullivan, J.P.Sumi, Y.van Hecke, H.Willis, W.J.Wolf, K.Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisionsNuclear Physics - ExperimentThe NA44 collaboration has measured charged kaon and pion distributions at midrapidity in sulphur and proton collisions with nuclear targets at 200 and 450 GeV/c per nucleon, respectively. The inverse slopes of kaons are larger than those of pions. The difference in the inverse slopes of pions, kaons and protons, all measured in our spectrometer, increases with system size and is consistent with the buildup of collective flow for larger systems. The target dependence of both the yields and inverse slopes is stronger for the sulphur beam suggesting the increased importance of secondary rescattering for SA reactions. The rapidity density, dN/dy, of both K+ and K- increases more rapidly with system size than for pi+ in a similar rapidity region. This trend continues with increasing centrality, and according to RQMD, it is caused by secondary reactions between mesons and baryons. The K-/K+ ratio falls with increasing system size but more slowly than the pbar/p ratio. The pi-/pi+ ratio is close to unity for all systems. From pBe to SPb the K+/p ratio decreases while K-/pbar increases and ({K+*K-}/{p*pbar})**1/2 stays constant. These data suggest that as larger nuclei collide, the resulting system has a larger transverse expansion, baryon density and an increasing fraction of strange quarks.The NA44 collaboration has measured charged kaon and pion distributions at midrapidity in sulphur and proton collisions with nuclear targets at 200 and 450 GeV/c per nucleon, respectively. The inverse slopes of kaons are larger than those of pions. The difference in the inverse slopes of pions, kaons and protons, all measured in our spectrometer, increases with system size and is consistent with the buildup of collective flow for larger systems. The target dependence of both the yields and inverse slopes is stronger for the sulphur beam suggesting the increased importance of secondary rescattering for SA reactions. The rapidity density, dN/dy, of both K+ and K- increases more rapidly with system size than for pi+ in a similar rapidity region. This trend continues with increasing centrality, and according to RQMD, it is caused by secondary reactions between mesons and baryons. The K-/K+ ratio falls with increasing system size but more slowly than the pbar/p ratio. The pi-/pi+ ratio is close to unity for all systems. From pBe to SPb the K+/p ratio decreases while K-/pbar increases and ({K+*K-}/{p*pbar})**1/2 stays constant. These data suggest that as larger nuclei collide, the resulting system has a larger transverse expansion, baryon density and an increasing fraction of strange quarks.The NA44 collaboration has measured charged kaon and pion distributions at midrapidity in sulphur and proton collisions with nuclear targets at 200 and 450 GeV/c per nucleon, respectively. The inverse slopes of kaons are larger than those of pions. The difference in the inverse slopes of pions, kaons and protons, all measured in our spectrometer, increases with system size and is consistent with the buildup of collective flow for larger systems. The target dependence of both the yields and inverse slopes is stronger for the sulphur beam suggesting the increased importance of secondary rescattering for SA reactions. The rapidity density, dN/dy, of both K+ and K- increases more rapidly with system size than for pi+ in a similar rapidity region. This trend continues with increasing centrality, and according to RQMD, it is caused by secondary reactions between mesons and baryons. The K-/K+ ratio falls with increasing system size but more slowly than the pbar/p ratio. The pi-/pi+ ratio is close to unity for all systems. From pBe to SPb the K+/p ratio decreases while K-/pbar increases and ({K+*K-}/{p*pbar})**1/2 stays constant. These data suggest that as larger nuclei collide, the resulting system has a larger transverse expansion, baryon density and an increasing fraction of strange quarks.nucl-ex/9808002TAMU-CYCL-9803TAMU-98-3oai:cds.cern.ch:3624341999
spellingShingle Nuclear Physics - Experiment
Boggild, H.
Boissevain, J.
Dodd, J.
Esumi, S.
Fabjan, C.W.
Fields, D.E.
Franz, A.
Hansen, K.H.
Humanic, T.J.
Jacak, B.V.
Kalechofsky, H.
Lee, Y.Y.
Leltchouk, M.
Lorstad, B.
Maeda, N.
Miyabayashi, A.
Murray, M.
Nishimura, S.
Pandey, S.U.
Piuz, F.
Polychronakos, V.
Potekhin, M.
Poulard, G.
Sakaguchi, A.
Sarabura, M.
Simon-Gillo, J.
Schmidt-Sorensen, J.
Sondheim, W.
Sugitate, T.
Sullivan, J.P.
Sumi, Y.
van Hecke, H.
Willis, W.J.
Wolf, K.
Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
title Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
title_full Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
title_fullStr Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
title_full_unstemmed Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
title_short Charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
title_sort charged kaon and pion production at midrapidity in proton nucleus and sulphur nucleus collisions
topic Nuclear Physics - Experiment
url https://dx.doi.org/10.1103/PhysRevC.59.328
http://cds.cern.ch/record/362434
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