Date

New analysis of the radiative decay omega --> eta gamma in proton - anti-proton annihilation at rest

Case, T. ; Crowe, K.M. ; Heinsius, F.H. ; et al.
Phys.Rev.D 61 (2000) 032002, 2000.
Inspire Record 522711 DOI 10.17182/hepdata.22247

We report on a measurement of the branching ratio of the rare decay ω→ηγ relative to the well known decay ω→π0γ. The ω’s are produced in pp¯→ηω and pp¯→π0ω. Eigenstate mixing and interference effects of the ω and ρ0 are taken into account, as well as coherent interference with the background. We find evidence for the non-resonant annihilation channel B(pp¯→ηηγ)=(3.5±1.3)×10−5 and limit the value of B(ω→ηγ) to the range of (0.7to5.5)×10−4 depending on the degree of coherence with the background.

1 data table match query

No description provided.


Resonances formed by anti-p p and decaying into pi0 pi0 eta for masses 1960-MeV to 2410-MeV.

Anisovich, A.V. ; Baker, C.A. ; Batty, C.J. ; et al.
Nucl.Phys.A 651 (1999) 253-276, 1999.
Inspire Record 504411 DOI 10.17182/hepdata.36177

Data on pbar-b annihilation in flight into pizero-pizero-eta are presented for nine beam momenta 600 to 1940 MeV/c. The strongest four intermediate states are found to be f_2(1270)-eta, a_2(1320)-pi, sigma-eta and a_0(980)-pi. Partial wave analysis is performed mainly to look for resonances formed by pbar-p and decaying into pizero-pizero-eta through these intermediate states. There is evidence for the following s-channel I = 0 resonances : two 4^{++} resonances with mass and width (M,Gamma) at (2044, 208) MeV and (2320+-30, 220+-30) MeV/ three 2^{++} resonances at (2020+-50, 200+-70) MeV, (2240+-40, 170+-50) MeV and (2370+-50, 320+-50) MeV/ two 3^{++} resonances at (2000+-40, 250+-40) MeV and (2280+-30, 210+-30) MeV/ a 1^{++} resonance at (2340+-40, 340+-40) MeV/ and two 2^{-+} resonances at (2040+-40, 190+-40) MeV and (2300+-40, 270+-40) MeV.

1 data table match query

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Further analysis of anti-p p ---> 3pi0, eta eta pi0 and eta pi0 pi0 at rest

Abele, A. ; Adomeit, J. ; Armstrong, D.S. ; et al.
Nucl.Phys.A 609 (1996) 562-584, 1996.
Inspire Record 431685 DOI 10.17182/hepdata.36492

A fresh analysis is reported of high statistics Crystal Barrel data on p p → 3π 0 , ηηπ 0 , ηπ 0 π 0 and ηη ′ π 0 at rest. This analysis is made fully consistent with CERN-Munich data on π + π − → π + π − up to a mass of 1900 MeV, with GAMS data on π + π − → π 0 π 0 , and with BNL and ANL data on π + π − → K K , which are fitted simultaneously. There is evidence for an I = 0, J PC = 2 ++ resonance with weak (≤ 7%) coupling to ππ, strong coupling to both ϱϱ and ωω and pole position 1534 - i90 MeV. This resonance agrees qualitatively with GAMS and VES data on ππ → ωω, previously interpreted in terms of a resonance at 1590–1640 MeV. New masses and widths for (A) ƒ 0 (1370) and (B) ƒ 0 (1500) , fitted to all eight data sets, are M A = 1300 ± 15 Mev, Γ A = 230 ± 15 MeV, M B = 1500 ± 8 MeV, Γ B = 132 ± 15 MeV. Branching ratios to ππ and ηη are given, and differ significantly from earlier determinations because of a new procedure.

1 data table match query

A fraction of the initial P-state annihilation into F2(1270) cannot be ruled out. Therefore, the ratio magnitudes include the contribution due to this channel. MESON0 denotes A2(1630) state, not present in RPP.


Resonances in anti-p p --> f2(1270) pi.

The Crystal Barrel collaboration Anisovich, A.V. ; Nikonov, V.A. ; Sarantsev, A.V. ; et al.
Phys.Lett.B 452 (1999) 187-193, 1999.
Inspire Record 501658 DOI 10.17182/hepdata.28093

We present data on p ̄ p→3π 0 at nine p̄ momenta from 600 to 1940 MeV/c. This process is dominated by the f 2 (1270) π 0 channel, where we observe I =1 resonances with the following masses and widths: 4 ++ (2260±15), Γ =180±20 MeV, 4 ++ (2005±25), Γ =360±80 MeV, 3 ++ (2310±40), Γ =180 +120 −60 MeV, 3 ++ (2070±20), Γ =170±40 MeV, 2 ++ (2280±30), Γ =280±50 MeV, 2 ++ (2100 +10 −30 ), Γ =360 +40 −100 MeV, 1 ++ (2100±20), Γ =300 +30 −60 MeV, and 1 ++ (2340±40), Γ =230±70 MeV.

1 data table match query

No description provided.


Coupled channel analysis of anti-p p annihilation into pi0 pi0 pi0, pi0 eta eta and pi0 pi0 eta

The Crystal Barrel collaboration Amsler, C. ; Armstrong, D.S. ; Baker, C.A. ; et al.
Phys.Lett.B 355 (1995) 425-432, 1995.
Inspire Record 406130 DOI 10.17182/hepdata.28523

We confirm the existence of the two I G ( J PC ) = 0 + (0 ++ ) resonances f 0 (1370) and f 0 (1500) reported by us in earlier analyses. The analysis presented here couples the final states π 0 π 0 π 0 , π 0 π 0 η and π 0 ηη of p p annihilation at rest. It is based on a 3 × 3 K -matrix. We find masses and widths of M = (1390±30) MeV, Γ = (380±80) MeV; and M = (1500±10) MeV, Γ = (154 ± 30) MeV, respectively. The product branching ratios for the production and decay into π 0 π 0 and ηη of the f 0 (1500) are (1.27 ± 0.33) · 10 −3 and (0.60 ± 0.17) · 10 −3 , respectively.

1 data table match query

No description provided.


Anti-p d annihilation at rest into pi+ pi- pi- p(spectator).

The Crystal Barrel collaboration Abele, A. ; Adomeit, J. ; Amsler, C. ; et al.
Phys.Lett.B 450 (1999) 275-280, 1999.
Inspire Record 500218 DOI 10.17182/hepdata.28089

A study of antiproton annihilation in liquid deuterium into π + π − π − and a spectator proton is presented. For a long time this reaction resisted a description by final state interactions which is surprising (and disturbing) given the success of the final state interaction model in other annihilation reactions. It is shown that the introduction of ρ (1450) is essential to get a reasonable description of the measured Dalitz plot. This resonance was never tried in previous attempts to understand this data. A possible isospin-2- ππ S-wave contribution was tested, but no evidence was found for such a contribution.

1 data table match query

No description provided.


Evidence for a pi eta P-wave in anti-p p annihilations at rest into pi0 pi0 eta.

The Crystal Barrel collaboration Abele, A. ; Adomeit, J. ; Amsler, C. ; et al.
Phys.Lett.B 446 (1999) 349-355, 1999.
Inspire Record 498113 DOI 10.17182/hepdata.28121

A partial wave analysis is presented of two high-statistics data samples of protonium annihilation into π 0 π 0 η in liquid and 12 atm gaseous hydrogen. The contributions from the 1 S 0 , 3 P 1 and 3 P 2 initial atomic fine structure states to the two data sets are different. The change of their fractional contributions when going from liquid to gaseous H 2 as calculated in a cascade model is imposed in fitting the data. Thus the uncertainty in the fraction of S-state and P-state capture is minimized. Both data sets allow a description with a common set of resonances and resonance parameters. The inclusion of a π η P-wave in the fit gives supportive evidence for the ρ ̂ (1405) , with parameters compatible with previous findings.

1 data table match query

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Observation of radiative anti-p p annihilation into a phi meson

The Crystal Barrel collaboration Amsler, C. ; Armstrong, D.S. ; Augustin, I. ; et al.
Phys.Lett.B 346 (1995) 363-370, 1995.
Inspire Record 401140 DOI 10.17182/hepdata.28709

The annihilation p p → Φγ has been investigated with the Crystal Barrel detector at LEAR for antiprotons stopped in liquid hydrogen. The observed branching ratio BR ( p p → Φγ = (1.7 ± 0.4) · 10 −5 is almost two orders of magnitude higher than expected from the OZI-rule. As a by-product, the branching ratios BR ( p p → K L K S ) = (9.0 ± 0.6) · 10 −4 and BR ( p p → Φπ 0 ) = (5.5 ± 0.7) · 10 −4 have been measured.

1 data table match query

No description provided.


First observation of the production of nucleon resonances in anti-proton annihilation in liquid deuterium

The Crystal Barrel collaboration Amsler, C. ; Armstrong, D.S. ; Augustin, I. ; et al.
Phys.Lett.B 352 (1995) 187-192, 1995.
Inspire Record 405540 DOI 10.17182/hepdata.28705

None

1 data table match query

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Study of anti-p p --> pi0 pi0 eta from 600-MeV/c to 1940-MeV/c.

The Crystal Barrel collaboration Anisovich, A.V. ; Nikonov, V.A. ; Sarantsev, A.V. ; et al.
Phys.Lett.B 452 (1999) 180-186, 1999.
Inspire Record 501657 DOI 10.17182/hepdata.28094

Antiproton-proton annihilation into π 0 π 0 η has been studied with incident beam momenta of 0.6 to 1.94 GeV/c. The main aim is to look for resonances formed by p ̄ p and decaying into π 0 π 0 η . Resonances observed are: two 4 ++ resonances with mass and width (M, Γ ) at (2044, 208) MeV and (2320±30, 220±30) MeV; three 2 ++ resonances at (2020±50, 220±70) MeV, (2240±40, 170±50) MeV and (2370±50, 320±50) MeV; two 3 ++ resonances at (2000±40, 250±40) MeV and (2280±30, 210±30) MeV; a 1 ++ resonance at (2340±40, 340±40) MeV; and two 2 −+ resonances at (2040±40, 190±40) MeV and (2300±40, 270±40) MeV.

1 data table match query

No description provided.