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The intermediate vector boson

The trouble with (1.2.1) is that it cannot be correct, at least in the high energy domain. If, for instance, one evaluates the cross-section for the elastic reaction [Pg.23]

Since the interaction is point-like the scattering goes entirely via the s-wave, and partial wave unitarity then requires that [Pg.23]

Even worse, if one blames this on the lowest order approximation used and tries to evaluate higher order corrections, one immediately finds horrible divergences. Thus to order G, for the amplitude in Fig. 2.1, these divergences, unlike QED, cannot be eliminated by proper renormalization. To make the various matrix elements finite new arbitrary constants would have to be introduced in each order—the Fermi theory of weak interactions is non-renormalizable. [Pg.24]

Historically (see, for example, Lee and Wu, 1965) the vector boson was given the following properties  [Pg.24]

two charge states ( ) since the familiar / -decay reactions require charge-changing currents  [Pg.24]


The coupling of the was designed to agree exactly with the intermediate vector boson description of the weak interactions which in turn was designed to reproduce the highly successful four-fermion Fermi description, at least for momentum transfers such that This... [Pg.69]

At the time of writing, LEP 1 is the great focus of excitement in the field. It was constructed to study the intermediate vector boson Z which was expected to dominate e" e collisions in the energy region aroimd 90 GeV (Fig. 8.1). [Pg.122]

Cline, D.B, C RliLibia, and S. van tier Meer The Search for Intermediate Vector Bosons. (March 1982). A classic reference in The Laureates Anthology, 133, Scientific American. Inc., New York, NY, 1990. [Pg.1218]

The weak interaction, some lO times weaker than the electrom neUc interaction, occurs between "leptons and in the decay of hadrons. It is responsible for the "beta decay of particles and nuclei. In the current model, the weak interaction is visualized as a force mediated by the exchange of virtual particles, called intermediate vector bosons. The weak interactions are described by "electro-weak theory, which unifies them with the electromagnetic interactions. [Pg.339]

In gauge theories the interactions between particles can be explained by the exchange of particles (intermediate vector bosons, or gauge bosons), such as gluons, photons, and W and Z bosons. [Pg.346]

W boson (W particle) Either of a pair of elementary particles (W or W ), classified as intermediate vector bosons, that are believed to transmit the weak interaction (see FUNDAMENTAL INTERACTIONS) in much the same way as photons transmit the electromagnetic interaction. They are not, however, massless like photons, and are believed to... [Pg.872]

Later, when we come to discuss intermediate vector mesons or gauge bosons which mediate the weak interactions, the picture will be altered to that in Fig. 1.6. It will often be convenient to visualize weak interaction... [Pg.12]


See other pages where The intermediate vector boson is mentioned: [Pg.652]    [Pg.644]    [Pg.698]    [Pg.23]    [Pg.25]    [Pg.631]    [Pg.726]    [Pg.704]    [Pg.690]    [Pg.724]    [Pg.644]    [Pg.652]    [Pg.644]    [Pg.698]    [Pg.23]    [Pg.25]    [Pg.631]    [Pg.726]    [Pg.704]    [Pg.690]    [Pg.724]    [Pg.644]    [Pg.43]    [Pg.228]    [Pg.278]    [Pg.65]    [Pg.366]    [Pg.208]    [Pg.85]    [Pg.6]    [Pg.39]    [Pg.603]   


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