The frequency of the protonium annihilation channel <(p)over bar p> --> KSKL has been measured at three different target densities: liquid hydrogen (LH), gaseous hydrogen at NTP conditions and gaseous hydrogen at low pressure (5 mbar). The obtained results are: f(<(p)over bar p> --> KSKL, LH) = (7.8 +/- 0.7(stat) +/- 0.3(sys)) x 10(-4), f(<(p)over bar p> --> KSKL, NTP) = (3.5 +/- 0.5(stat) +/- 0.2(sys)) x 10(-4) and f(<(p)over bar p> --> KSKL, 5 mbar) = (1.0 +/- 0.3(stat) +/- 0.1(sys)) x 10(-4). Since the KSKL final state can be originated only from the S-3(1) initial state, these values give direct information on the scaling of the protonium spin-triplet S-wave annihilation probability with the density.

Protonium annihilation into KSKL at three different target densities

BALESTRA, Ferruccio;BOTTA, Elena;BRESSANI, Tullio;BUSSA, Maria Pia;BUSSO, Luigi;COSTA, Sergio;FERRERO, Livio;GARFAGNINI, Raffaello;GRASSO, Antonino;MARCELLO, Simonetta;PANZIERI, Daniele;
1996-01-01

Abstract

The frequency of the protonium annihilation channel <(p)over bar p> --> KSKL has been measured at three different target densities: liquid hydrogen (LH), gaseous hydrogen at NTP conditions and gaseous hydrogen at low pressure (5 mbar). The obtained results are: f(<(p)over bar p> --> KSKL, LH) = (7.8 +/- 0.7(stat) +/- 0.3(sys)) x 10(-4), f(<(p)over bar p> --> KSKL, NTP) = (3.5 +/- 0.5(stat) +/- 0.2(sys)) x 10(-4) and f(<(p)over bar p> --> KSKL, 5 mbar) = (1.0 +/- 0.3(stat) +/- 0.1(sys)) x 10(-4). Since the KSKL final state can be originated only from the S-3(1) initial state, these values give direct information on the scaling of the protonium spin-triplet S-wave annihilation probability with the density.
1996
386
486
494
A. Bertin;M. Bruschi;M. Capponi;A. Collamati;I. DAntone;S. DeCastro;R. Dona;A. Ferretti;D. Galli;B. Giacobbe;U. Marconi;I. Massa;M. Piccinini;M. Poli;N. SempriniCesari;R. Spighi;S. Vecchi;A. Vezzani;F. Vigotti;M. Villa;A. Vitale;A. Zoccoli;A. Zenoni;M. Corradini;A. Donzella;E. L. Rizzini;L. Venturelli;C. Cicalo;A. Masoni;G. Puddu;S. Serci;P. P. Temnikov;G. Usai;O. E. Gorchakov;S. N. Prakhov;A. M. Rozhdestvensky;C. Guaraldo;A. Lanaro;V. Lucherini;M. G. Sapozhnikov;V. I. Tretyak;P. Gianotti;F. Nichitiu;C. Petrascu;A. Rosca;V. G. Ableev;C. Cavion;U. Gastaldi;M. Lombardi;G. Maron;L. Vannucci;G. Vedovato;M. Morando;G. Bendiscioli;V. Filippini;A. Fontana;P. Montagna;A. Rotondi;A. Saino;P. Salvini;F. Balestra;E. Botta;T. Bressani;M. P. Bussa;L. Busso;D. Calvo;P. Cerello;S. Costa;A. Feliciello;L. Ferrero;A. Filippi;R. Garfagnini;A. Grasso;A. Maggiora;S. Marcello;N. Mirfakhrai;D. Panzieri;D. Parena;E. Rossetto;F. Tosello;M. Agnello;F. Iazzi;B. Minetti;G. Pauli;S. Tessaro;L. Santi
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Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/2318/109441
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