Amendolia, S.R.; Batignani, G.; Bertolucci, E.; Bosisio, L.; Bradaschia, C.; Dell'Orso, M.; Fidecaro, F.; Foa, L.; Focardi, E.; Gianetti, P.; Giazzotto, A.; Giorgi, M.A.; Marrocchesi, P.S.; Menzione, A.; Ristori, L.; Scribano, A.; Tonelli, G.; Triggiani, G.; Beck, G.A.; Bologna, G.; D'Ettorre Piazzoli, B.; Mannocchi, G.; Picchi, P.; Budinich, M.; Liello, F.; Ragusa, F.; Rolandi, L.; Stefanini, A.; Fabbri, F.L.; Laurelli, P.; Zallo, A.; Gren, M.G.; Landon, M.P.J.; March, P.V.; Strong, J.A.; Tenchini, R.; Meroni, E.1986
AbstractAbstract
[en] The negative kaon electromagnetic form factor has been measured in the space-like q2 range 0.015-0.10 (GeV/c)2 by the direct scattering of 250 GeV kaons from electrons at the CERN SPS. It is found that the kaon mean square charge radius < rK2>=0.34±0.05 fm2. From data collected simultaneously for πe scattering, the difference between the charged pion and kaon mean square radii (which is less sensitive to systematic errors) is found to be < rπ2>-< rK2>=0.10±0.045 fm2. (orig.)
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Record Type
Journal Article
Literature Type
Numerical Data
Journal
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ANTIMATTER, ANTIMESONS, ANTIPARTICLES, BOSONS, CROSS SECTIONS, DATA, ELECTRON-MESON INTERACTIONS, ELEMENTARY PARTICLES, ENERGY RANGE, FERMIONS, FORM FACTORS, GEV RANGE, HADRONS, INFORMATION, INTERACTIONS, KAONS, LEPTON-HADRON INTERACTIONS, LEPTON-MESON INTERACTIONS, LEPTONS, MATTER, MESONS, NUMERICAL DATA, PARTICLE INTERACTIONS, PARTICLE PROPERTIES, PIONS, PSEUDOSCALAR ANTIMESONS, PSEUDOSCALAR MESONS, SCATTERING, STRANGE PARTICLES
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Abe, F.; Fukui, Y.; Mikamo, S.; Mishina, M.; Amidei, D.; Atac, M.; Beretvas, A.; Berge, J.P.; Binkley, M.; Booth, A.W.; Carroll, J.T.; Chadwick, K.; Cihangir, S.; Clark, A.G.; Cooper, J.; Crane, D.; Day, C.; Elias, J.E.; Foster, G.W.; Freeman, J.; Hahn, S.R.; Huth, J.; Jensen, H.; Johnson, R.P.; Joshi, U.; Kadel, R.W.; Kephart, R.; Maas, P.; Marriner, J.P.; Mukherjee, A.; Nelson, C.; Newman-Holmes, C.; Para, A.; Patrick, J.; Plunkett, R.; Quarrie, D.; Savvoy-Navarro, A.; Schmidt, E.E.; Segler, S.; Theriot, D.; Thaczyk, S.; Tollestrup, A.; Vidal, R.; Wagner, R.L.; Yagil, A.; Yeh, G.P.; Yoh, J.; Yun, J.C.; Apollinari, G.; Bedeschi, F.; Belforte, S.; Bellettini, G.; Cervelli, F.; Dell'Agnello, S.; Dell'Orso, M.; Gianetti, P.; Grassmann, H.; Incagli, M.; Mangano, M.; Menzione, A.; Paoletti, R.; Punzi, G.; Ristori, L.; Scribano, A.; Sestini, P.; Smith, D.A.; Stefanini, A.; Tonelli, G.; Westhusing, T.; Zetti, F.; Auchincloss, P.; Buckley, E.; Devlin, T.; Flaugher, B.; Hu, P.; Kuns, E.; Watts, T.; Baden, A.R.; Bradenburgh, G.; Brown, D.; Carey, R.; Franklin, M.; Geer, S.; Jessop, C.P.; Kearns, E.; Ng, J.S.T.; Pare, E.; Phillips, T.J.; Schwitters, R.; Shapiro, M.; St Denis, R.; Trischuk, W.; Barbaro-Galtieri, A.; Carithers, W.; Chinowsky, W.; Drucker, R.B.; Ely, R.; Gold, M.; Haber, C.; Harris, R.M.; Hubbard, B.; Siegrist, J.; Tipton, P.; Wester, W.C. III; Winer, B.L.; Barnes, V.E.; Byon, A.; Garfinkel, A.F.; Huffman, B.T.; Laasanen, A.T.; Schub, M.H.; Tonnison, J.; Behrends, S.; Bensinger, J.; Blocker, C.; Contreras, M.; Demortier, L.; Kesten, P.; Kirsch, L.; Mattingly, R.; Moulding, S.; Nakae, L.F.; Tarem, S.; Bellinger, J.; Byrum, K.L.; Carlsmith, D.; Handler, R.; Lamoureux, J.I.; Markeloff, R.; Markosky, L.A.; Pondrom, L.; Rhoades, J.; Sheaff, M.; Skarha, J.; Wendt, C.; Bertolucci, S.; Chiarelli, G.; Cordelli, M.; Curatolo, M.; Esposito, B.; Giromini, P.; Miscetti, S.; Sansoni, A.; Bhadra, S.; Errede, S.
Gauge bosons and heavy quarks: Proceedings of Summer Institute on Particle Physics1991
Gauge bosons and heavy quarks: Proceedings of Summer Institute on Particle Physics1991
AbstractAbstract
[en] During the 1988/1989 run at the Fermilab Tevatron, the CDF detector collected ≅ 4.1 pb-1 of p bar p data at √s = 1.8 TeV. The main goals of this run being physics at high pt, the CDF trigger was tuned for maximizing signals from Z0s, Ws, t-quarks, and etc. As such, compared to the high pt physics, the b-physics program was of secondary importance other than that which would be used for background calculations. Also, CDF had no vertex chamber capability for seeing displaced vertices. However, significant b-quark physics results are evident in two data samples: (1) inclusive electrons; (2) inclusive J/ψ where J/ψ → μ+μ-. In this paper, the author will try to specify the goals for b-physics using the inclusive electrons and J/ψ signals for the 1988/89 data set. He will then provide a brief look at the data, and will finish with some highly speculative guesses as to whether or not experiments at the Tevatron which look for CP violation in the b sector are possible
Primary Subject
Secondary Subject
Source
Hawthorne, J.F. (ed.); Stanford Linear Accelerator Center, Menlo Park, CA (United States); 528 p; Jan 1991; p. 489-506; 18. SLAC summer institute on particle physics: heavy quarks and gauge bosons; Stanford, CA (United States); 16-27 Jul 1990; CONF-900799--; OSTI as DE91011248; NTIS; INIS
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Report
Literature Type
Conference
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ASYMMETRY, B MESONS, BEAUTY BARYONS, BEAUTY PARTICLES, CHARMED MESONS, CP INVARIANCE, DESIGN, DISTRIBUTION, EXCLUSIVE INTERACTIONS, FERMILAB COLLIDER DETECTOR, FERMILAB TEVATRON, INCLUSIVE INTERACTIONS, J PSI-3097 MESONS, MUON DETECTION, PARTICLE IDENTIFICATION, PARTICLE PRODUCTION, PERFORMANCE, QUARKS, RESEARCH PROGRAMS, SEMILEPTONIC DECAY, SHOWER COUNTERS, TRIGGER CIRCUITS
ACCELERATORS, BARYONS, BOSONS, CHARGED PARTICLE DETECTION, CHARM PARTICLES, CHARMONIUM, CYCLIC ACCELERATORS, DECAY, DETECTION, ELECTRONIC CIRCUITS, ELEMENTARY PARTICLES, FERMIONS, HADRONS, INTERACTIONS, INVARIANCE PRINCIPLES, MEASURING INSTRUMENTS, MESONS, PARTICLE DECAY, PARTICLE INTERACTIONS, POSTULATED PARTICLES, PSEUDOSCALAR MESONS, PULSE CIRCUITS, QUARKONIUM, RADIATION DETECTION, RADIATION DETECTORS, SYNCHROTRONS, VECTOR MESONS, WEAK PARTICLE DECAY
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