The measurement of different reactions of anti-p d annihilation at rest in a gaseous target has been performed using the OBELIX spectrometer at LEAR (CERN). A strong deviation from the OZI-rule prediction was found from the measurement of the ratio R = ϕπ/ωπ in two regions of proton momenta, P < 200 MeV/c and P > 400 MeV/c: R(ϕπ-/ωπ-) = (133 ± 26) x 10^-3 and (113 ± 30) x 10^-3, respectively. These values are about 30 times greater than the theoretical prediction. For the first time the excitation of the Δ-resonance was observed among the final-state products of anti-p d annihilation. The existence of a broad enhancement in the 4π invariant mass at m ≈ 1480 MeV, seen in previous experiments, was confirmed. A ≈ 100 MeV downward shift of the bump position, when the proton momentum increased up to P > 400 MeV/c, was also observed, while the positions of ω, ρ and f_2(1270) did not change with the proton momentum. The following branching ratios were measured: BR(anti-p d → π- ϕ p) = (6.62 ± 0.49) x 10^-4, for P < 200 MeV/c; BR(anti-p d → π- ϕ p) = (0.95 ± 0.22) x 10^-4, for P > 400 MeV/c; BR(anti-p d → π- ω p) = (49.7 ± 8.9) x 10^-4, for P < 200 MeV/c; BR(anti-p d → π- ω p) = (8.38 ± 1.09) x 10^-4 for P > 400 MeV/c; BR(anti-p d → 2 π- π+ p) = (150 ± 6) x 10^-4 for P < 200 MeV/c; BR(anti-p d → 2 π- π+ p) = (16.6 ± 0.9) x 10^-4, for P > 400 MeV/c; BR(anti-p d → 3π- 2π+ p) = (326 ± 12) x 10^-4, for P < 200 MeV/c; BR(anti-p d → 3π- 2π+ p) = (44 ± 7) x 10^-4, for P > 400 MeV/c; BR(anti-p d → Λ K+ π-) = (0.96 ± 0.19) x 10^-4, for P > 400 MeV/c; BR(anti-p d → Λ K+ π- π0) = (3.5 ± 0.8) x 10^-4, for P > 400 MeV/c; BR(anti-p p → 2π- 2π+) = (540 ± 20) x 10^-4; BR(anti-p p → 3π- 3π+) = (251 ± 21) x 10^-4.

Measurements of the anti-p d Annihilation at Rest

BERTIN, A;CAPPONI, M;DECASTRO, S;GALLI, D;SEMPRINICESARI, N;VILLA, M;VITALE, A;ZOCCOLI, A;
1995

Abstract

The measurement of different reactions of anti-p d annihilation at rest in a gaseous target has been performed using the OBELIX spectrometer at LEAR (CERN). A strong deviation from the OZI-rule prediction was found from the measurement of the ratio R = ϕπ/ωπ in two regions of proton momenta, P < 200 MeV/c and P > 400 MeV/c: R(ϕπ-/ωπ-) = (133 ± 26) x 10^-3 and (113 ± 30) x 10^-3, respectively. These values are about 30 times greater than the theoretical prediction. For the first time the excitation of the Δ-resonance was observed among the final-state products of anti-p d annihilation. The existence of a broad enhancement in the 4π invariant mass at m ≈ 1480 MeV, seen in previous experiments, was confirmed. A ≈ 100 MeV downward shift of the bump position, when the proton momentum increased up to P > 400 MeV/c, was also observed, while the positions of ω, ρ and f_2(1270) did not change with the proton momentum. The following branching ratios were measured: BR(anti-p d → π- ϕ p) = (6.62 ± 0.49) x 10^-4, for P < 200 MeV/c; BR(anti-p d → π- ϕ p) = (0.95 ± 0.22) x 10^-4, for P > 400 MeV/c; BR(anti-p d → π- ω p) = (49.7 ± 8.9) x 10^-4, for P < 200 MeV/c; BR(anti-p d → π- ω p) = (8.38 ± 1.09) x 10^-4 for P > 400 MeV/c; BR(anti-p d → 2 π- π+ p) = (150 ± 6) x 10^-4 for P < 200 MeV/c; BR(anti-p d → 2 π- π+ p) = (16.6 ± 0.9) x 10^-4, for P > 400 MeV/c; BR(anti-p d → 3π- 2π+ p) = (326 ± 12) x 10^-4, for P < 200 MeV/c; BR(anti-p d → 3π- 2π+ p) = (44 ± 7) x 10^-4, for P > 400 MeV/c; BR(anti-p d → Λ K+ π-) = (0.96 ± 0.19) x 10^-4, for P > 400 MeV/c; BR(anti-p d → Λ K+ π- π0) = (3.5 ± 0.8) x 10^-4, for P > 400 MeV/c; BR(anti-p p → 2π- 2π+) = (540 ± 20) x 10^-4; BR(anti-p p → 3π- 3π+) = (251 ± 21) x 10^-4.
1995
ABLEEV, VG; AGNELLO, M; BALESTRA, F; BENDISCIOLI, G; BERTIN, A; BOCCACCIO, P; BOTTA, E; BRESSANI, T; BRUSCHI, M; BUSSA, MP; BUSSO, L; CALVO, D; CAPPONI, M; CEREDA, B; CERELLO, P; CICALO, C; COSTA, S; DECASTRO, S; DENISOV, OY; DISEP, D; DONZELLA, A; FAVA, L; FELICIELLO, A; FERRERO, L; FILIPPI, A; FILIPPINI, V; FONTANA, A; GALLI, D; GARFAGNINI, R; GASTALDI, U; GIACOBBE, B; GIANOTTI, P; GORCHAKOV, OE; GRASSO, A; GUARALDO, C; IAZZI, F; LANARO, A; RIZZINI, EL; LOMBARDI, M; LUCHERINI, V; MAGGIORA, A; MANEVA, G; MARCELLO, S; MARCONI, U; MARGAGLIOTTI, GV; MARON, G; MASONI, A; MINETTI, B; MONTAGNA, P; MORANDO, M; NICHITIU, F; PANZIERI, D; PAULI, G; PICCININI, M; POLI, M; PRAKHOV, SN; PUDDU, G; RICCI, RA; ROSSETTO, E; ROTONDI, A; ROSHDESTVENSKY, AM; SAINO, A; SALVINI, P; SANTI, L; SAPOZHNIKOV, MG; SEMPRINICESARI, N; SERCI, S; SPIGHI, R; TEMNIKOV, PP; TESSARO, S; TOSELLO, F; TRETYAK, VI; USAI, G; VANNUCCI, L; VECCHI, S; VEDOVATO, G; VENTURELLI, L; VILLA, M; VITALE, A; ZENONI, A; ZOCCOLI, A; ZOSI, G
File in questo prodotto:
Eventuali allegati, non sono esposti

I documenti in IRIS sono protetti da copyright e tutti i diritti sono riservati, salvo diversa indicazione.

Utilizza questo identificativo per citare o creare un link a questo documento: https://hdl.handle.net/11585/954790
 Attenzione

Attenzione! I dati visualizzati non sono stati sottoposti a validazione da parte dell'ateneo

Citazioni
  • ???jsp.display-item.citation.pmc??? ND
  • Scopus 43
  • ???jsp.display-item.citation.isi??? 44
social impact