By D. Haidt, H. Pietschmann, H. Schopper
ISBN-10: 3540183795
ISBN-13: 9783540183792
ISBN-10: 3540479317
ISBN-13: 9783540479314
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Additional resources for Electroweak Interactions. Experimental Facts and Theoretical Foundation
Sample text
This prompted W. Pauli to postulate (in a famous unpublished letter dated Dec. 4, 1930, to colleagues at a congress in Tubingen) the existence of a hitherto unobserved neutral particle which should take care of energy-momentum balance and which he dubbed the “neutron”. After the discovery of the neutral nucleon, Fermi changed its name into “neutrino”. It took about a quarter of a century, until the first direct experimental evidence for neutrino induced reactions was obtained by F. L. Cowan [53REIN; 59REINl.
Subtraction A MOM A MS Am 54GELL 73THOO 74COLL Eq. 42) shows that the running coupling constant vanishes at infinite energy scales. This is known as asymptotic freedom of QCD and supports the successof the naive quark mode! for high energy processes. In the low energy domain, non-perturbative effects become important. It is believed that this gives rise to the confining potential for all colored states. 1 Renormalization schemesin QFD The basic principles of renormalization are outlined in Sect.
The signal consisted of 86 events with a 25% background due to the moderate hadron/lepton rejection. The signature with large missing momentum and apparent lepton number violation was very striking. li-p cm2 20 0 0 t;' 10 0 5 I 15 0s 2 Fig 3 1. The observed cross sectionfor e--p events,oe,,vs. total dnergy E,,, [75PERL]. ’ 3 L 5 Etot - 6 7 GeV 8 neutrino interactions dilepton events have been observed, however accompanied by hadrons (seeSect. 5). 0 GeV decaying leptonically. g. the production of charged bosons (charmed meson) or even the intermediate vector boson (chapter 4).
Electroweak Interactions. Experimental Facts and Theoretical Foundation by D. Haidt, H. Pietschmann, H. Schopper
by David
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