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Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1992

The Crystal Barrel spectrometer at LEAR

E. Aker; C. Amsler; I. Augustin; C.A. Baker; B. M. Barnett; C.J. Batty; R. Beckmann; P. Birien; J. Bistirlich; Philipp Blum; R. Bossingham; H. Bossy; K. Braune; D.V. Bugg; Mark J. Burchell; T. Case; S. Cierjacks; K.M. Crowe; K. Dederichs; M. Doser; W. Dünnweber; H. Emerich; D. Engelhardt; M. Faessler; C. Felix; G. Folger; J. Friedrich; R. Hackmann; R.P. Haddock; H. Hammer

The crystal Barrel spectrometer used at LEAR, CERN to study the products of pd annihilations is described. A 1380 element array of Csl crystals measures photons from the decay of π0, η, η′ and ω mesons. A segmented drift chamber in a 1.5T magnetic field is used to identify and measure charged particles. A fast on-line trigger on charged and neutral multiplicities and on the invariant mass of secondary particles is available. The performance of the detector is discussed.


Physics Letters B | 1994

Observation of two JPC=0++ isoscalar resonances at 1365 and 1520 MeV

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; A. Cooper; K.M. Crowe; T. Degener; H.P. Dietz; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; G. Folger; R. Hackmann; R.P. Haddock; F.-H. Heinsius; N. P. Hessey

From a simultaneous analysis of data on pp → π0π0π0 and pp → ηηπ0 at rest, two I = 0, JPC = 0++ resonances are identified above 1 GeV. The first has mass M = 1365−55+20 MeV and width г = 268 ± 70 MeV, close to the ƒ0(1400) of the Particle Data Group. The second has M = 1520 ± 25 MeV, г = 148−25+20 MeV.


Physics Letters B | 1995

High-statistics study of f0(1500) decay into π0π0

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

Coupled channel analysis of pp annihilation into π0π0π0, π0ηη and π0π0η

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

Observation of a new IG(JPC)=1−(0++) resonance at 1450 MeV

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 | 1991

Observation of a 2+ + resonance at 1515 MeV in proton-antiproton annihilations into 3π0

E. Aker; C. Amsler; I. Augustin; C. A. Baker; B. M. Barnett; C. J. Batty; R. Beckmann; P. Birien; J. Bistirlich; Philipp Blum; R. Bossingham; H. Bossy; K. Braune; Mark J. Burchell; T. Case; S. Cierjacks; K.M. Crowe; K. Dederichs; W. Dünnweber; D. Engelhardt; M. Faessler; C. Felix; G. Folger; R.P. Haddock; F.-H. Heinsius; N. P. Hessey; P. Hidas; P. Illinger; D. Jamnik; H. Kalinowsky

Abstract Antiproton-proton annihilations at rest into 3 π 0 are analyzed in terms of π 0 π 0 final state interactions. A J PC = 2 + + resonance at a mass of 1515 ± 10 MeV with a width of 120 ± 10 MeV is required to explain the data. This result is supported by previous observations made on the ππ system in p p and p n annihilations which show that the resonance has I = 0. This resonance is practically degenerate in mass with the f′ 2 (1525) but the two resonances have very different production and decay characteristics.


Physics Letters B | 1992

The pseudoscalar mixing angle ΘPS from ν and ν′ production in p annihiltion at rest

C. Amsler; I. Augustin; C. A. Baker; B.M. Barnett; C. J. Batty; K. Beuchert; P. Birien; J. Bistirlich; Philipp Blum; R. Bossingham; H. Bossy; K. Braune; D.V. Bugg; Mark J. Burchell; T. Case; S. U. Chung; A. Cooper; K.M. Crowe; H.P. Dietz; S.v. Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; G. Folger; R. Hackmann; R.P. Haddock; F.-H. Heinsius

Abstract We have determined ratios of branching ratios for p p annihilations at rest into π 0 η and π 0 η ′, into ηη and ηη ′, and into ωη and ωη ′. All reactins are observed in two different all-neutral final states. The ratios permit a determination of the pseudoscalar mixing angle. We find Θ PS = −(17.3±1.8)°.


Physics Letters B | 1992

Proton-antiproton annihilation into ηηπ-observation of a scalar resonance decaying into ηη

C. Amsler; C. J. Batty; D.V. Bugg; C. Kolo; B. Schmid; U. Wiedner; K.M. Crowe; M. Suffert; A. Cooper; D. Walther; D. Jamnik; D. Engelhardt; R. Landua; P. Hidas; H. Kalinowsky; N. P. Hessey; E. Schäfer; Chr. Strassburger; L. Montanet; E. Klempt; R.P. Haddock; W. Dünnweber; M. Merkel; U. Strohbusch; S. Ravndal; Mark J. Burchell; R. Bossingham; S. Spanier; C. Völcker; G. Folger

Abstract The results of a measurement of pp annihilation at rest into ηηπ 0 are presented. Assuming a resonance dominated model for the annihilation process an isoscalar J PC =0 ++ resonance decaying into ηη is observed with a mass of 1560±25 MeV/ c 2 and a width of 245±50 MeV/ c 2 .


Physics Letters B | 1992

P- versus S-wave pp-annihilation at rest in LH2

C. Amsler; I. Augustin; C. A. Baker; B.M. Barnett; C.J. Batty; K. Beuchert; P. Birien; J. Bistirlich; Philipp Blum; R. Bossingham; H. Bossy; K. Braune; J. Brose; D.V. Bugg; Mark J. Burchell; T. Case; A. Cooper; K.M. Crowe; H.P. Dietz; S. von Dombrowski; M. Doser; W. Dünnweber; D. Engelhardt; M. Englert; M. Faessler; C. Felix; G. Folger; R. Hackmann; R.P. Haddock; F.-H. Heinsius

Abstract The annihilation p p →π 0 π 0 was measured for antiprotons stopped in liquid hydrogen (LH2). This reaction is only allowed from odd angular momentum states of the p p - atom . The resulting branching ratio BR ( p p →π 0 π 0 ) LH 2 =(6.93±0.22 stat ±0.37 syst )×10 −4 , combined with a previous measurement of the branching ratio BR ( p p →π + π − ) 2 P in gas from the 2P-state of p p suggests a fraction of P-wave annihilation in LH2 of (28.8±3.5)%, much larger than the values obtained from other annihilation channels. A method of reconciling the contradictory results is discussed.


Physics Letters B | 1994

ηη′ threshold enhancement in p̄p annihilations into π0ηη′ at rest

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) .

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D. Engelhardt

Karlsruhe Institute of Technology

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K.M. Crowe

University of California

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R. Bossingham

University of California

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T. Case

University of California

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D.V. Bugg

Queen Mary University of London

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C. A. Baker

Rutherford Appleton Laboratory

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P. Birien

University of California

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K. Beuchert

Ruhr University Bochum

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