Deep sub-threshold K*(892)0 production in collisions of Ar + KCl at 1.76 A GeV

T. Liu | A. Tarantola | P. Fonte | J. Lange | J. Mousa | E. Castro | M. Palka | M. Traxler | M. Destefanis | S. Chernenko | B. Spruck | C. Sturm | J. Stroth | L. Naumann | A. Belyaev | M. Weber | L. Fabbietti | T. Karavicheva | F. Krizek | A. Kurepin | K. Lapidus | J. Otwinowski | Y. Pachmayer | A. Rustamov | A. Schmah | Y. Zanevsky | A. Reshetin | F. Guber | K. Kanaki | V. Wagner | E. Epple | G. Agakishiev | T. Galatyuk | S. Spataro | A. Kugler | T. Eberl | B. Sailer | J. Wüstenfeld | A. Sadovsky | M. Jurkovič | R. Krücken | A. Blanco | L. Lopes | B. Kämpfer | R. Gernhäuser | L. Maier | J. D́ıaz | J. Michel | P. Finocchiaro | P. Salabura | W. Kühn | V. Metag | T. Hennino | B. Ramstein | R. Holzmann | D. Belver | A. Ivashkin | D. Mishra | J. Boyard | M. Roy-Stéphan | Y. Sobolev | M. Böhmer | J. Friese | P. Huck | T. Christ | M. Golubeva | H. Ströbele | S. Yurevich | O. Fateev | Y. Parpottas | I. Iori | J. A. Garzón | E. Morinière | B. Kolb | P. Tlustý | W. Koenig | J. Markert | J. Pietraszko | B. Michalska | R. Bassini | I. Fröhlich | E. Schwab | J. Siebenson | D. González-Díaz | T. Pérez Cavalcanti | A. Mangiarotti | R. Kotte | A. Balanda | P. Cabanelas | A. Dybczak | A. Gil | M. Gumberidze | T. Heinz | I. Koenig | M. Lorenz | C. Müntz | V. Pechenov | O. Pechenova | W. Przygoda | K. Teilab | R. Trebacz | H. Tsertos | C. Wendisch | D. Kirschner | F. Dohrmann | M. Heilmann | S. Lang | M. Wiśniowski | T. Wójcik | P. Zumbruch | C. Gilardi | The Hades Collaboration | J. Díaz | T. Liu

[1]  F. Becattini,et al.  Energy and system size dependence of chemical freeze-out in relativistic nuclear collisions , 2005, hep-ph/0511092.

[2]  H Germany,et al.  Strangeness production from πN collisions in nuclear matter , 2000, nucl-th/0004011.

[3]  B W Kolb,et al.  Dielectron production in 12C+12C collisions at 2A GeV with the HADES spectrometer. , 2007, Physical review letters.

[4]  W. Cassing,et al.  Excitation functions of hadronic observablesfrom SIS to RHIC energies , 2000, nucl-th/0001024.

[5]  Y. Wang,et al.  The high-acceptance dielectron spectrometer HADES , 2009, 0902.3478.

[6]  E. Epple,et al.  Dielectron production in Ar+KCl collisions at 1.76A GeV , 2011, 1103.0876.

[7]  E. Epple,et al.  In-Medium Effects on K$^0$ Mesons in Relativistic Heavy-Ion Collisions , 2010, 1004.3881.

[8]  J. Cleymans,et al.  THERMUS - A thermal model package for ROOT , 2004, Comput. Phys. Commun..

[9]  G. Torrieri,et al.  Hadron resonances and phase threshold in heavy ion collisions , 2006, nucl-th/0608061.

[10]  G. Stoicea,et al.  Systematics of central heavy ion collisions in the 1A GeV regime , 2010, 1005.3418.

[11]  F. Laue,et al.  Production of K+ and of K- mesons in heavy-ion collisions from 0.6A to 2.0A GeV incident energy , 2007, nucl-ex/0701014.

[12]  Jr.,et al.  K*0 production in Cu + Cu and Au + Au collisions at √sNN=62.4 GeV and 200 GeV , 2010, 1006.1961.

[13]  T. Liu,et al.  Hyperon production in Ar + KCl collisions at 1.76A GeV , 2010, 1010.1675.

[14]  B W Kolb,et al.  Deep subthreshold Xi;{-} production in Ar + KCl reactions at 1.76A GeV. , 2009, Physical review letters.

[15]  Jørgen Randrup,et al.  Maximum freeze-out baryon density in nuclear collisions , 2006 .

[16]  E. al.,et al.  Measurement of K*(892)0 and K0 mesons in Al+Al collisions at 1.9A GeV , 2010, 1006.1905.

[17]  S. Bass,et al.  Microscopic models for ultrarelativistic heavy ion collisions , 1998, nucl-th/9803035.

[18]  E. al.,et al.  K(892)* resonance production in Au+Au and p + p collisions at sNN = 200 GeV , 2004, nucl-ex/0412019.

[19]  S. Bass,et al.  RELATIVISTIC HADRON-HADRON COLLISIONS IN THE ULTRA-RELATIVISTIC QUANTUM MOLECULAR DYNAMICS MODEL , 1999, hep-ph/9909407.

[20]  H. Oeschler,et al.  Strangeness production close to the threshold in protonnucleus and heavy-ion collisions , 2011, 1106.2083.

[21]  A. Andronic,et al.  Hadron production in central nucleus-nucleus collisions at chemical freeze-out , 2005, nucl-th/0511071.

[22]  M. A. Diaz Corchero,et al.  Production of K ∗ ( 892 ) 0 and φ ( 1020 ) in pp collisions at √ s = 7 TeV , 2012 .

[23]  R. Gernhäuser,et al.  φ decay: A relevant source for K − production at energies available at the GSI Schwerionen-Synchrotron (SIS)? , 2009 .

[24]  C. Markert,et al.  Strange hadron production in heavy ion collisions from SPS to RHIC , 2011, 1105.2798.

[25]  Alan D. Martin,et al.  Review of Particle Physics , 2010 .

[26]  E. al.,et al.  K*(892)0 and K*(892)0 production in central Pb + Pb, Si + Si, C + C, and inelastic p + p collisions at 158A GeV , 2011, 1105.3109.

[27]  A. Tarantola,et al.  Measurement of charged pions in 12C + 12C collisions at 1 A GeV and 2 A GeV with HADES , 2009, 0902.4377.

[28]  S. Bass,et al.  Strangeness dynamics and transverse pressure in relativistic nucleus-nucleus collisions , 2004, nucl-th/0402026.