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Subatomic Physics

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94 The <strong>Subatomic</strong> Zoo<br />

Table 5.2: Interactions and <strong>Subatomic</strong> Particles. Entries not in<br />

parentheses are for particles that exist free in nature. The particles<br />

in parentheses are permanently confined.<br />

Particle Type Weak Electromagnetic Hadronic<br />

Photon Gauge boson No Yes No<br />

W ± ,Z0 Gauge bosons Yes Yes No<br />

(Gluon)<br />

Leptons<br />

Gauge boson No No Yes<br />

Neutrino Fermion Yes No No<br />

Electron Fermion Yes Yes No<br />

Muon Fermion Yes Yes No<br />

Tau<br />

Hadrons<br />

Fermion Yes Yes No<br />

Mesons Bosons Yes Yes Yes<br />

Baryons Fermions Yes Yes Yes<br />

(Quarks) Fermions Yes Yes Yes<br />

a weak interaction. The charged leptons, in addition, are also subject to the electromagnetic<br />

force. All other particles, including nuclei, are hadrons; their behavior<br />

is governed by the strong, the electromagnetic, and the weak interactions. In the<br />

following sections we describe the particles listed in Table 5.2 in more detail. We<br />

include quarks and gluons; they cannot be observed directly but their existence is<br />

basedonfirmarguments.<br />

5.5 Gauge Bosons<br />

The first group of particles in Table 5.2 lists three types of quanta, called gauge<br />

bosons, the photon, the W + ,W − and Z 0 , and the gluons. We are all familiar<br />

with the photon, but the other quanta and the name “gauge boson” require some<br />

introductory remarks. These particles are the carriers of forces as will be discussed in<br />

Section 5.8. Three types of forces are important in subatomic physics, the hadronic,<br />

the electromagnetic, and the weak. We therefore expect three types of particles to<br />

be responsible for the three forces between the leptons and quarks. Indeed, the<br />

photon mediates the electromagnetic force, the massive bosons, W ± and Z 0 carry<br />

the weak force, and the gluons are the field quanta of the hadronic force. As we<br />

will show later, the form of the interaction is determined by a symmetry principle<br />

called gauge invariance; hence the name gauge bosons. We begin the discussion of<br />

the gauge bosons with the photon, the quantum of light. The particle properties of<br />

light invariably lead to some confusion. It is not possible to eliminate all confusion<br />

at an elementary level because a satisfactory treatment of photons requires quantum<br />

electrodynamics. However, a few remarks may at least make some of the important<br />

physical properties clearer.

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