F.H. Heinsius
University of California, Berkeley
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Featured researches published by F.H. Heinsius.
Physics Letters B | 1995
C. Amsler; C. J. Batty; D. Engelhardt; R.P. Haddock; H. Stock; J. Brose; K.M. Crowe; M. Suffert; D. Walther; D. Jamnik; C. Kolo; T. Degener; R. Landua; H. Kalinowsky; F. Loser; N. P. Hessey; E. Schäfer; C. Strassburger; L. Montanet; J. Salk; E. Klempt; O. Cramer; W. Dünnweber; M. Merkel; U. Strohbusch; S. Ravndal; Mark J. Burchell; R. Bossingham; S. Spanier; M. Kunze
Abstract A partial-wave analysis of the reaction p p →π 0 π 0 π 0 has been performed using a high-quality high-statistics data set of 712 000 events. In addition to the f0(975) and f0(1300), the scalar resonance with mass m = (1500 ± 15) MeV and width Γ = (120 ± 25) MeV is necessary to describe the data.
Physics Letters B | 1995
C. Amsler; D.S. Armstrong; C. A. Baker; B.M. Barnett; C. J. Batty; M. Benayoun; K. Beuchert; P. Birien; Philipp Blum; R. Bossingham; K. Braune; J. Brose; D.V. Bugg; T. Case; S. U. Chung; A. Cooper; O. Cramer; K.M. Crowe; T. Degener; H.P. Dietz; N. Djaoshvili; S.v. Dombroski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; P. Giarritta; R. Hackmann
We confirm the existence of the two IG(JPC) = 0+(0++) resonances f0(1370) and f0(1500) reported by us in earlier analyses. The analysis presented here couples the final states π0π0π0, π0π0η and π0ηη of pp 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 π0π0 and ηη of the f0(1500) are (1.27 ± 0.33) · 10−3 and (0.60 ± 0.17) · 10−3, respectively.
Physics Letters B | 1994
C. Amsler; V.V. Anisovich; D.S. Armstrong; I. Augustin; C. A. Baker; B.M. Barnett; C.J. Batty; K. Beuchert; P. Birien; Philipp Blum; R. Bossingham; K. Braune; J. Brose; D.V. Bugg; Mark J. Burchell; T. Case; S. U. Chung; A. Cooper; K.M. Crowe; T. Degener; H.P. Dietz; S. von Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; R. Hackmann; R.P. Haddock
Abstract A new IG=1− JPC=0++πη resonance is observed in pp annihilation at rest into π0π0η. It has a mass M=(1450±40)MeV and a width Γ=(270±40)MeV.
Physics Letters B | 1998
Andreas Abele; C.J. Batty; D.V. Bugg; M. Tischhauser; C. Kolo; H. Stock; K.M. Crowe; M. Suffert; P. Kammel; C. Strassburger; Dirk Walther; U. Thoma; D. Engelhardt; Michael Heinzelmann; T. Degener; N. Djaoshvili; C. Völcker; H. Kalinowsky; R. Seibert; N.P. Hessey; C. Hodd; C. Pietra; A. Ehmanns; R. Landua; U. Kurilla; E. Klempt; O. Cramer; W. Dünnweber; A. Herbstrith; Steve G. Wallis
Abstract With antiprotons stopped in liquid deuterium, the p n annihilation channel π−π0η was studied using a final sample of 52xa0576 events obtained for a spectator proton momentum q q quantum numbers IG=1−, JPC=1−+. The extracted Breit-Wigner resonance parameters are m=(1400±20±20) MeV/c2 and Γ=(310±50+50−30) MeV/c2.
Physics Letters B | 1999
Andreas Abele; J. Adomeit; C. Amsler; C. A. Baker; B.M. Barnett; C. J. Batty; M. Benayoun; A. Berdoz; K. Beuchert; S. Bischoff; Philipp Blum; K. Braune; T. Case; O. Cramer; V. Crede; K.M. Crowe; T. Degener; N. Djaoshvili; S.v. Dombrowski; M. Doser; W. Dünnweber; A. Ehmanns; D. Engelhardt; M. Faessler; P. Giarritta; R.P. Haddock; F.H. Heinsius; Michael Heinzelmann; A. Herbstrith; M. Herz
Abstract A partial wave analysis is presented of two high-statistics data samples of protonium annihilation into π 0 π 0 η in liquid and 12xa0atm gaseous hydrogen. The contributions from the 1 S 0 xa0, 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.
Physics Letters B | 1994
C. Amsler; D.S. Armstrong; I. Augustin; C. A. Baker; B.M. Barnett; C. J. Batty; K. Beuchert; P. Birien; Philipp Blum; R. Bossingham; K. Braune; J. Brose; D.V. Bugg; Mark J. Burchell; T. Case; S. U. Chung; A. Cooper; O. Cramer; K.M. Crowe; T. Degener; H.P. Dietz; S.v. Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; R. Hackmann; R.P. Haddock
Abstract We report on the observation of an ηη′ threshold enhancement produced in pp annihilations at rest into π0ηη′, which we identify with the recently discovered ƒ 0 (1500) .
Physics Letters B | 1995
C. Amsler; D.S. Armstrong; I. Augustin; C. A. Baker; B.M. Barnett; C. J. Batty; K. Beuchert; P. Birien; Philipp Blum; R. Bossingham; K. Braune; J. Brose; D.V. Bugg; Mark J. Burchell; T. Case; A. Cooper; O. Cramer; K.M. Crowe; T. Degener; H.P. Dietz; S.v. Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; R. Hackmann; R.P. Haddock; F.H. Heinsius
Abstract 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.
Physics Letters B | 1997
Andreas Abele; J. Adomeit; C. Amsler; C. A. Baker; B.M. Barnett; C. J. Batty; M. Benayoun; A. Berdoz; K. Beuchert; S. Bischoff; Philipp Blum; K. Braune; J. Brose; D.V. Bugg; T. Case; A. Cooper; O. Cramer; K.M. Crowe; T. Degener; N. Djaoshvili; S.v. Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Faessler; P. Giarritta; R. Hackmann; R.P. Haddock; F.H. Heinsius; Michael Heinzelmann
Abstract The distribution of m ( π + π − ) in the decay η ′ → π + π − γ has been measured with the Crystal Barrel detector. The results are based on a total of 7392 observed η′ decays. The box anomaly constant is extracted from this and its value is found to agree well with theoretical expectations. The pseudoscalar nonet parameters ( f 1 , f 8 and θ PS ) are determined. Finally, we find that there is a problem of consistency between QCD and the standard VDM assumption.
Physics Letters B | 1995
C. Amsler; D.S. Armstrong; C. A. Baker; B.M. Barnett; C. J. Batty; K. Beuchert; P. Birien; Philipp Blum; R. Bossingham; K. Braune; J. Brose; D.V. Bugg; Mark J. Burchell; T. Case; S. U. Chung; A. Cooper; O. Cramer; K.M. Crowe; T. Degener; H.P. Dietz; N. Djaoshvili; S.v. Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; P. Giarritta; R. Hackmann
Abstract A partial wave analysis of the reaction p p →π o ηη has been performed, using a high quality, high statistics data set of 198,000 events. In addition to the ƒ 0 (1370), a second scalar resonance decaying into ηη, the ƒ 0 (1500), with mass m = (1505 ± 15) MeV and width Γ = (120 ± 30) MeV has to be introduced to describe the data.
Physics Letters B | 1995
C. Amsler; D.S. Armstrong; C. A. Baker; B.M. Barnett; C. J. Batty; M. Benayoun; K. Beuchert; P. Birien; Philipp Blum; R. Bossingham; K. Braune; J. Brose; D.V. Bugg; T. Case; A. Cooper; O. Cramer; K.M. Crowe; T. Degener; H.P. Dietz; N. Djaoshvili; S.v. Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; P. Giarritta; R. Hackmann; R.P. Haddock; F.H. Heinsius
Abstract We have observed the ηπ + π − and ηπ 0 π 0 decay modes of the E meson in p p annihilation at rest into π + π − π 0 π 0 η . The mass and width of the E meson are 1409 ± 3 and 86 ± 10 MeV. The production and decay branching ratio is B( p p → Eππ)B(E → ηππ) = (3.3 ± 1.0) × 10 −3 . With a spin-parity analysis we determine that J P = 0 − . The observation of the ηπ 0 π 0 decay mode establishes that E is isoscalar ( C = +1). We find that E decays to η ( ππ ) s (where ( ππ ) s is an S-wave dipion) and πa 0 (980)(→ πη ) with a relative branching ratio of (78 ± 16) %. Using the K K π production and decay branching ratio measured earlier we determine that B[E → K K π] B[E → ηππ] = 0.61 ± 0.19 . A comparison with observations in radiative J Ψ decays suggests that E and ι η (1416) are identical.