H. Burkhardt
CERN
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Featured researches published by H. Burkhardt.
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 | 2001
H. Burkhardt; B. Pietrzyk
Abstract We have updated the evaluation of the hadronic contribution to the running of the QED fine structure constant. It is obtained from a dispersion integral over a parametrization of the measured cross section of e + e − →hadrons. We find this contribution to be Δα (5) had ( s )=0.02761±0.00036 at s = m Z 2 corresponding to 1/ α (5) ( m Z 2 )=128.936±0.046. The improved experimental accuracy is mainly due to recent BES measurements. We have also updated and parametrized the hadronic contribution to α as a function of energy.
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 | 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.
Physics Letters B | 1990
G. Barr; David Coward; D. Fournier; H. Wahl; L. Iconomidou-Fayard; L. Gatignon; D. Cundy; H.G. Sander; P. Calafiura; G. Zech; R. Heinz; H. Burkhardt; H. N. Nelson; M. Rost; W. Weihs; M. Calvetti; N. Doble; H. Rohrer; A. Nappi; G. Kesseler; A.C. Schaffer; D.J. Candlin; G. Quast; B. Panzer; R. Carosi; I. Mannelli; H. Blümer; K. Kleinknecht; P. Grafström; L. Bertanza
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 | 1996
A. Arbuzov; M. Bigi; H. Burkhardt; M. Cacciari; M. Caffo; H. Czyz; M. Dallavalle; J.H. Field; F. Filthaut; S. Jadach; F. Jegerlehner; E. Kuraev; G. Montagna; O. Nicrosini; F. Piccinini; B. Pietrzyk; Wiesiek Placzek; E. Remiddi; M. Skrzypek; Luca Trentadue; B.F.L. Ward; Z. Wa̧s
Abstract The results concerning the theoretical evaluation of the small-angle Bhabha Scattering cross section obtained during the Workshop on Physics at LEP2 (CERN, Geneva, Switzerland, 1995) by the Working Group “Event Generators for Bhabha Scattering” are summarized. The estimate of the theoretical error on the cross section in the luminometry region is updated.
Physics Letters B | 1989
G. Barr; David Coward; D. Fournier; M. Kasemann; H. Wahl; L. Iconomidou-Fayard; L. Gatignon; D. Cundy; H.G. Sander; P. Calafiura; G. Zech; R. Heinz; H. Burkhardt; H. N. Nelson; Robert L Chase; W. Weihs; M. Calvetti; P. Heusse; N. Doble; H. Rohrer; A. Nappi; G. Kesseler; H. Taureg; A.C. Schaffer; D.J. Candlin; G. Quast; B. Panzer; E. Auge; I. Mannelli; T. Miczaika
Abstract We have searched for the sequence of decays K L 0 → π 0 H 0 and H 0 →e + e − at the CERN Super Proton Synchrotron (SPS), and have allowed for a non-zero H 0 lifetime. Three candidates have been seen, consistent with an expected background of 3.3. Limits on the branching ratio product in the range 10 −8 –10 −7 are presented as a function of the mass and lifetime of the H 0 . These can be used to restrict the neutral Higgs of the minimal standard model.
arXiv: High Energy Physics - Phenomenology | 1996
S. Jadach; H. Anlauf; G. Montagna; H. Burkhardt; G.Marco Dallavalle; Z. Was; T. Ohl; Wiesiek Placzek; B.F.L. Ward; A. Arbuzov; M. Bigi; Luca Trentadue; J.H. Field; E. Kuraev; M. Caffo; M. Skrzypek; F. Jegerlehner; M. Cacciari; F. Piccinini; Henryk Czyz; F. Filthaut; E. Remiddi; B. Pietrzyk; O. Nicrosini
Archive | 1987
A Barroso; M. Caffo; W. Hollik; E Neugebauer; W.L. van Neerven; P N Ratoff; C. Mana; S. Jadach; M. Martinez; N Dombey; D Perret-Gallix; F. Dydak; Bryan W. Lynn; R G Stuart; J C Romão; Claudio Verzegnassi; W. Blum; J P Cole; G.J.H. Burgers; A Shapira; F. Jegerlehner; F.A. Berends; F. Boudjema; W. Beenakker; Errietta Simopoulou; J Salicio; H. Wachsmuth; Z. Was; L Lanceri; J Fleischer
Physics Letters B | 1990
G. Barr; R. Carosi; David Coward; Donald C Cundy; N. Doble; L. Gatignon; V. Gibson; P. Grafström; R. Hagelberg; G. Kesseler; J. van der Lans; H. N. Nelson; H. Wahl; Richard J. Black; D.J. Candlin; J. Muir; Ken Peach; H. Blümer; R. Heinz; K. Kleinknecht; P. Mayer; B. Panzer; B. Renk; H. Rohrer; E. Auge; Daniele Fournier; P. Heusse; Lydia Iconomidou-Fayard; I. Harrus; A. M. Lutz