I. Mannelli
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Physics Letters B | 1988
H. Burkhardt; P. E. L. Clarke; D. Coward; D. Cundy; N. Doble; L. Gatignon; V. Gibson; R. Hagelberg; G. Kesseler; J. van der Lans; I. Mannelli; T. Miczaika; A.C. Schaffer; J. Steinberger; H. Taureg; H. Wahl; C. Youngman; G. Dietrich; W. Heinen; R. Black; D.J. Candlin; J. Muir; Ken Peach; B. Pijlgroms; I.P. Shipsey; W. Stephenson; H. Blümer; M. Kasemann; K. Kleinknecht; B. Panzer
Since CP violation was first observed in the decay of the long-lived neutral kaon into two pions [1], it remains one of the enigmas in particle physics. Whilst CP violation is manifest in neutral kaon decays, the search for CP-violating effects has elsewhere been unsuccessful. In the phenomenology of CP violation in the neutral kaon system [2], the short- and long-lived mass eigenstates are usually defined in terms of the CP eigenstates K1 (CP = + 1) and K2 (CP = - 1) as Ks ≈ K1 + ?K2 and KL ≈ K2 + ?K1. The parameter ? describes CP violation induced by kaon state-mixing. Direct CP violation may also occur in the decay of K2 into two pions with a relative amplitude ?′, which is non-zero in the case of a phase difference between the amplitudes A0 and A2 for the decay into isospin O and 2 states of two pions. Before the present measurement, all experimental results were compatible with ? = 2.27 × 10-3 exp (i 43.70) and with the Superweak Model [3], in which state-mixing is the only source of CP violation and ?′ = 0. In the Standard Model with six weakly interacting quarks [4], direct CP violation as well as state-mixing is introduced by transitions via heavy-quark intermediate states. Based on this, a small, but non-zero, value of ?′ is predicted [5]. To a good approximation, ?′ /? is related to the double ratio R of the relative decay rates of the long- and short-lived neutral kaons into two neutral and two charged pions as Re (?′/?) = 1/6 × (1 - R).
Physics Letters B | 1990
R. Carosi; P. E. L. Clarke; D. Coward; D. Cundy; N. Doble; L. Gatignon; V. Gibson; P. Grafström; R. Hagelberg; G. Kesseler; J. van der Lans; H.N. Nelson; H. Wahl; R. Black; D.J. Candlin; J. Muir; Ken Peach; H. Blümer; R. Heinz; M. Kasemann; K. Kleinknecht; P. Mayer; B. Panzer; B. Renk; S. Roehn; H. Rohrer; E. Augé; R.L. Chase; D. Fournier; P. Heusse
Abstract The phases of the CP-violating amplitudes in K0→π+π− and K0→2π0 decays, φ+−=46.9°±2.2° and φ00=47.1°±2.8°, have been measured in the same experiment, and a direct comparison gives the phase difference φ00−φ+−=0.2°±2.9°. This result leads to an upper limit on possible CPT violation in the K0 mass matrix, of |(m K 0 −m K 0 )/m K 0 | −18 at the 95% confidence level and is the most stringent test of the equality of particle and antiparticle masses.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1996
G. Barr; C. Bruschini; C. Bocquet; P. Buchholz; D. Cundy; N. Doble; W. Funk; L. Gatignon; A. Gonidec; B. Hallgren; G. Kesseler; A. Lacourt; G. Laverrière; G. Linser; M. Martini; A. Norton; D. Schinzel; W. Seidl; Marco S. Sozzi; H. Taureg; O. Vossnack; H. Wahl; P. Wertelaers; J. Weterings; M. Ziolkowski; A. M. Kalinin; V. Kekelidze; Yu. Kozhevnikov; L. Bertolotto; V. Carassiti
The NA48 collaboration is preparing a new experiment at CERN aiming to study CP violation in the K0-K0 system with an accuracy of 2 × 10−4 in the parameter Re(ϵ′/ϵ). Decays in two π0s will be recorded by a quasi-homogeneous liquid krypton calorimeter. A liquid krypton calorimeter has been chosen to combine good energy, position and time resolution with precise charge calibration and long-term stability. The prototype calorimeter incorporating the final design of the electrode read-out structure is presented in this paper. An energy resolution of ≃3.5%√E with a constant term smaller than 0.5% has been obtained. The time resolution was found to be better than 300 ps above 15 GeV.
Nuclear Physics | 1979
W.D. Apel; K. H. Augenstein; E. Bertolucci; Yu.B. Bushnin; S.V. Donskov; R. Franceschini; M. Givoletti; M.I. Grachev; A. V. Inyakin; Rolland P. Johnson; V.A. Kachanov; W. Kittenberger; R.N. Krasnokutsk; M. Krüger; G. Leder; A.A. Lednev; I. Mannelli; Yu.V. Mikhailov; H. Müller; R. Oberparleiter; M. Pernicka; G. Pierazzini; Yu.D. Prokoshkin; M. Quaglia; D. Schinzel; H. Schneider; A. Scribano; F. Sergiampietri; R.S. Shuvalov; G. Sigurdsson
A high statistics measurement of the reaction π−p → π0n has been performed at the Serpukhov accelerator for 15, 20, 25, 30 and 40 GeV/c incident pion momentum using the NICE set-up with its associated 648-channel hodoscope spectrometer for γ-ray detection. More than 3 million charge-exchange events have been recorded in total. It is found that the spin-flip and non-spin-flip amplitudes can be parametrized, for small |t|, as exponentials with the same slopes to within a few percent. Also the behaviour of the differential cross section for small and medium |t| agrees with the prediction of a geometrical s-channel model which describes binary reactions in terms of a complex pole b0(s). The imaginary part of this universal pole, Im b0(s), has been determined and found to be growing logarithmically with s.
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 1988
H. Burkhardt; P. E. L. Clarke; D. Cundy; N. Doble; L. Gatignon; R. Hagelberg; G. Kesseler; J. van der Lans; I. Mannelli; T. Miczaika; H.G. Sander; A.C. Schaffer; P. Steffen; J. Steinberger; H. Taureg; H. Wahl; C. Youngman; G. Dietrich; F. Eisele; W. Heinen; R. Black; D.J. Candlin; J. Muir; Ken Peach; B. Pijlgroms; I.P. Shipsey; W. Stephenson; H. Blümer; M. Kasemann; K. Kleinknecht
The K0 beam and detector used for a high-precision measurement of the CP-violation parameter ϵ′ at the CERN Super Proton Synchrotron (SPS) are described. The beam provides KL and KS alternately through a common decay region. The detection of the decays is based on wire chambers and calorimeters without employing a magnet. The trigger and readout system achieve a high selectively for the suppressed, CP-violating, two-pion decays of the KL by incorporation of hard-wired processors. The readout is based on Fastbus for maximum data rates.
Physics Letters B | 1979
W.D. Apel; K. H. Augenstein; Ennio Bertolucci; S. V. Donskov; A. V. Inyakin; Rolland P. Johnson; V.A. Kachanov; V. Kittenberger; R.N. Krasnokutsky; M. Krüger; G. Leder; A. A. Lednev; I. Mannelli; Yu.V. Mikhailov; H. Müller; Yu.D. Prokoshkin; G. Pierazzini; M. Quaglia; D. Schinzel; A. Scribano; H. Schneider; F. Sergiampietri; R.S. Shuvalov; G. Sigurdsson; M. Steuer; M.L. Vincelli
Abstract Measurements were made of the cross section of the reactions π−p → ν′(958)n, η′ → 2γ at momenta at 15, 20, 25, 30 and 40 GeV/c. The experiment was carried out on the IHEP 70 GeV accelerator using the 648 channel hodoscope spectrometer NICE for γ-ray detection. A total of 6000 η′ mesons were recorded. A sharp drop is seen in the differential cross section for t → 0. The dependences of the differential cross sections for the π−p → η′n and π−p → η n on t are identical. On the basis of the ratio of the cross sections for these reactions at t = 0, i.e. R( η′ n ) t=0 = 0.55 ± 0.06 , the singlet-octet mixing angle for pseudoscalar mesons was determined to be β = −(18.2 ± 1.4)°.
Physics Letters B | 1990
G. Barr; R. Carosi; D. Coward; D. Cundy; N. Doble; L. Gatignon; V. Gibson; P. Grafström; R. Hagelberg; G. Kesseler; J. van der Lans; H.N. Nelson; H. Wahl; R. Black; D.J. Candlin; J. Muir; Ken Peach; H. Blümer; R. Heinz; K. Kleinknecht; P. Mayer; B. Panzer; B. Renk; H. Rohrer; E. Augé; D. Fournier; P. Heusse; L. Iconomidou-Fayard; I. Harrus; A.M. Lutz
Abstract The decay mode K L → π 0 γγ has been observed with a signal of 21 events and an expected background of 1.5±0.9 events. A branching ratio for decays with invariant γγ masses above 280 MeV of (2.1±0.6)×10 −6 is calculated. This result is compared with the values estimated from theoretical models and has implications for the CP conserving contribution to K L → π 0 e + e − decay.
Physics Letters B | 1980
C. Kourkoumelis; L.K. Resvanis; T. A. Filippas; E. Fokitis; A.M. Cnops; J.H. Cobb; R. Hogue; S. Iwata; R.B. Palmer; D.C. Rahm; P. Rehak; I. Stumer; C. Fabjan; T. Fields; D. Lissauer; I. Mannelli; P. Mouzourakis; K. Nakamura; A. Nappi; W. Struczinski; W.J. Willis; M. Goldberg; N. Horwitz; G.C. Moneti; A.J. Lankford
We present the B(dθdy)y=0 for J/ψ over thefull range of ISR energies and for ϒ at √s = 53 and 63 GeV, using their dielectron decay mode. The average transverse momentum and the decay angles are presented. We found (pT) = 1.75 ± 0.19 GeV for ϒ, being higher than (pT) of the continuum and rising with √s. We present a comparison of the cross sections of J/ψ and ϒ with those of the continuum, at the same masses, as a function of √s. An appropriate scaling of the hadronic production of quark-antiquark narrow bound states involving ⋉, J/ψ, ψ′, ϒ, and ϒ′ is presented as a function of m/√s at y = 0, and is compared with Drell-Yan scaling.
Physics Letters B | 1979
C. Kourkoumelis; L.K. Resvanis; T. A. Filippas; E. Fokitis; A.M. Cnops; S. Iwata; R.B. Palmer; D.C. Rahm; P. Rehak; I. Stumer; C. Fabjan; T. Fields; D. Lissauer; I. Mannelli; P. Mouzourakis; A. Nappi; W.J. Willis; M. Goldberg
Abstract The inclusive η production cross section at the CERN ISR has been measured for p T values of up to 11 GeV/ c . We find that the η π 0 cross-section ratio has an average value of 0.55 ± 0.07 and varies little with p T .
Physics Letters B | 1987
H. Burkhardt; P. E. L. Clarke; D. Cundy; N. Doble; L. Gatignon; R. Hagelberg; G. Kesseler; J. van der Lans; I. Mannelli; T. Miczaika; H.G. Sander; A.C. Schaffer; P. Steffen; J. Steinberger; H. Taureg; H. Wahl; C. Youngman; G. Dietrich; W. Heinen; R. Black; D.J. Candlin; J. Muir; Ken Peach; B. Pijlgroms; I.P. Shipsey; W. Stephenson; H. Blümer; M. Kasemann; K. Kleinknecht; B. Panzer
Abstract The decay rates of K L → 2γ and K S → 2γ have been measured at the CERN SPS. The results are Γ (K L →2 γ )/ χ (K L →2 π 0 )=0.632±0.004±0.008 and Γ (K S →2 γ )/ Γ (K L →2 γ )=2.3 ±1.0±0.4. This is the first observation of K S →2γ decays.