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Physics Letters B | 1988

Search for the decay

J. Adams; A. Alavi-Harati; I. F. M. Albuquerque; T. Alexopoulos; Michael Wayne Arenton; K. Arisaka; S. Averitte; A. Barker; L. Bellantoni; A. Bellavance; J. Belz; R. Ben-David; D. R. Bergman; E. Blucher; G. J. Bock; C. Bown; S. Bright; E. Cheu; S. Childress; R. Coleman; M. Corcoran; G. Corti; B. Cox; M. Crisler; A. R. Erwin; Simon J. Field; R. Ford; G. Graham; J. Graham; K. Hagan

Abstract Data collected in Fermilab experiment E731 was used to perform the first search for the decay K L →π 0 ν ν . This decay is dominated by short distance effects and is almost entirely direct CP violating within the standard model. Cuts were developed to reject the background processes Λ→nπ0 and KL→π+e−γν. No candidate events were seen. We find BR (K L →π 0 ν ν ) −4 at the 90% confidence level.We report on a search for the rare decay K_L -> pi^0 nu nubar in the KTeV experiment at Fermilab. We searched for two-photon events whose kinematics were consistent with an isolated pi^0 coming from the decay K_L -> pi^0 nu nubar. One candidate event was observed, which was consistent with the expected level of background. An upper limit on the branching ratio was determined to be B(K_L -> pi^0 nu nubar) < 1.6E-6 at the 90% confidence level.We report on a search for the rare decay K_L -> pi^0 nu nubar in the KTeV experiment at Fermilab. We searched for two-photon events whose kinematics were consistent with an isolated pi^0 coming from the decay K_L -> pi^0 nu nubar. One candidate event was observed, which was consistent with the expected level of background. An upper limit on the branching ratio was determined to be B(K_L -> pi^0 nu nubar) < 1.6E-6 at the 90% confidence level.


nuclear science symposium and medical imaging conference | 2010

Handling of the generation of primary events in Gauss, the LHCb simulation framework

I. Beiyaev; T. Brambach; N. H. Brooke; N. Gauvh; G. Corti; K. Harrison; P. F. Harrison; Jibo He; P. H. Ilten; C. Jones; M. Lieng; G. Manca; S. Miglioranzi; P. Robbe; Vincenzo Vagnoni; M. Whitehead; J. Wishahi

The LHCb simulation application. Gauss, consists or two independent phases, the generation of the primary event and the tracking of particles produced in the experimental setup. For the LHCh experimental program it is particularly important to model IS meson decays: the KvtGcn code developed in CLEO and BaBah has been chosen and customized for non-coherent B production as necuring in pp collisions at the LHC, The initial proton-proto n collision is provided by a different generator engine, currently PYTHIA 6 for massive prwluclion of signal and generic pp collisions events. Beam gas events, background events originating from proton halo, cosmics and calibration events for different detectors can be generated in addition to pp collisions. Different generator packages as available in the physics community or specifically developed in LHCb are used for the different purposes. Running conditions affecting the events generated such as the size of the luminous region, the number of collisions occuring in a bunch crossing and the number of spill-over events from neighbouring bunches are modeled via dedicated algorithms appropriately configured. The design of the generator phase of Gauss will be described: a modular structure with well defined interfaces specific to the various tasks, e.g. pp collisions, particles decays, selections, etc. has been chosen. Different implementations are available for the various tasks allowing selecting and combining them as most appropriate at run time as in the case of Pythia 6 im pp collisions or HIJING for beam gas. The advantages of such structure, allowing for example to adopt transparently new generators packages will be discussed.

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J. Wishahi

Technical University of Dortmund

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M. Lieng

Technical University of Dortmund

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P. F. Harrison

Technical University of Dortmund

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T. Brambach

Technical University of Dortmund

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K. Harrison

University of Cambridge

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N. Gauvh

École Polytechnique Fédérale de Lausanne

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