1,668 research outputs found

    Hadronic ratios in Si - Au collisions

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    Cleymans J, Elliott D, Satz H, Thews RL. Hadronic ratios in Si - Au collisions. 1996

    ESTIMATES OF AXION SIGNAL FROM POSITRONIUM DECAY

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    CLEYMANS J, Faisal F, RAY PS. ESTIMATES OF AXION SIGNAL FROM POSITRONIUM DECAY. PHYSICS LETTERS B. 1982;116(6):447-449

    ON THE PHENOMENOLOGY OF DECONFINEMENT AND CHIRAL SYMMETRY RESTORATION

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    CLEYMANS J, REDLICH K, Satz H, SUHONEN E. ON THE PHENOMENOLOGY OF DECONFINEMENT AND CHIRAL SYMMETRY RESTORATION. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS. 1986;33(1):151-156

    HADRONIZATION OF QUARK-GLUON PLASMA

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    REDLICH K, CLEYMANS J, Satz H, SUHONEN E. HADRONIZATION OF QUARK-GLUON PLASMA. In: Nuclear Physics A. NUCLEAR PHYSICS A. Vol 566. ELSEVIER SCIENCE BV; 1994: C391-C394

    HADRONIC CORRELATIONS AT LARGE TRANSVERSE-MOMENTA IN PARTON MODEL

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    Baier R, CLEYMANS J, KINOSHITA K, Petersson B. HADRONIC CORRELATIONS AT LARGE TRANSVERSE-MOMENTA IN PARTON MODEL. NUCLEAR PHYSICS B. 1977;118(1-2):139-173

    TRANSVERSE-MOMENTUM DISTRIBUTION OF LEPTON-PAIRS AND HARD INTERACTION MECHANISM OF CONSTITUENTS

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    KINOSHITA K, KINOSHITA Y, CLEYMANS J, Petersson B. TRANSVERSE-MOMENTUM DISTRIBUTION OF LEPTON-PAIRS AND HARD INTERACTION MECHANISM OF CONSTITUENTS. PHYSICS LETTERS B. 1977;68(4):355-360

    THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS

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    CLEYMANS J, Satz H. THERMAL HADRON-PRODUCTION IN HIGH-ENERGY HEAVY-ION COLLISIONS. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS. 1993;57(1):135-147.We provide a method to test if hadrons produced in high energy heavy ion collisions were emitted at freeze-out from an equilibrium hadron gas. Our considerations are based on an ideal gas at fixed temperature T(f), baryon number density n(B), and vanishing total strangeness. The constituents of this gas are all hadron resonances up to a mass of 2 GeV; they are taken to decay according to the experimentally observed branching ratios. The ratios of the various resulting hadron production rates are tabulated as functions of T(f) and n(B). These tables can be used for the equilibration analysis of any heavy ion data; we illustrate this for some specific cases

    STRANGENESS PRODUCTION IN HEAVY-ION COLLISIONS AT FINITE BARYON NUMBER DENSITY

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    CLEYMANS J, Satz H, SUHONEN E, VONOERTZEN DW. STRANGENESS PRODUCTION IN HEAVY-ION COLLISIONS AT FINITE BARYON NUMBER DENSITY. PHYSICS LETTERS B. 1990;242(1):111-114

    Relations for hadron pairs at large pT in the elastic quark-quark scattering model

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    Baier R, Cleymans J, Petersson B. Relations for hadron pairs at large pT in the elastic quark-quark scattering model. Physical review D: Particles, fields, gravitation, and cosmology. 1978;17(9):2310-2313.Relations between cross sections for producing hadrons pairs with large transverse momenta are presented. They follow from the isospin and charge-conjugation properties of the elastic quark-quark scattering model. These relations are independent of any specific parametrization for the quark-distribution and quark-fragmentation functions and of any specific form for the hard-scattering cross section

    Thermal hadron production in Si-Au collisions

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    Cleymans J, Elliott D, Satz H, Thews RL. Thermal hadron production in Si-Au collisions. ZEITSCHRIFT FUR PHYSIK C-PARTICLES AND FIELDS. 1997;74(2):319-323.The most abundantly produced hadron species in Si-Au collisions at the BNL-AGS (nucleons, pions, kaons, antikaons and hyperons) are shown to be in accord with emission from a thermal resonance gas source. Within the uncertainties of the present data, two freeze-out points are possible. The best agreement is obtained for a temperature T similar or equal to 110 MeV and a baryochemical potential mu(B) similar or equal to 540 MeV, corresponding to about 1/3 standard nuclear density. Another possible point lies at about twice nuclear density, with T similar or equal to 110 MeV and mu(B) similar or equal to 620 MeV. Our analysis takes the isopin asymmetry of the initial state fully into account
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