bei48482_FM

Nuclear Structure 415

We therefore have

E t 

(mc^2 ) 

m (11.19)

which gives a value for mof

m 



2  10 ^28 kg

This rough figure is about 220 times the rest mass meof the electron.

Discovery of the Pion

A dozen years after Yukawa’s proposal, particles with the properties he had predicted

were actually discovered. The rest mass of charged pions is 273 meand that of neutral

pions is 264 me, not far from the above estimate.

Two factors contributed to the belated discovery of the free pion. First, enough

energy must be supplied to a nucleon so that its emission of a pion conserves energy.

Thus at least mc^2 of energy, about 140 MeV, is required. To furnish a stationary nucleon

with this much energy in a collision, the incident particle must have considerably more

kinetic energy than mc^2 in order that momentum as well as energy be conserved. Par-

ticles with kinetic energies of several hundred MeV are therefore required to produce

free pions, and such particles are found in nature only in the diffuse stream of cosmic

radiation that bombards the earth. Hence the discovery of the pion had to await the

development of sufficiently sensitive and precise methods of investigating cosmic-ray

1.05 10 ^34 J s



(1.7 10 ^15 m)(3 108 m /s)





rc

r



c

S

ome years before Yukawa’s work, particle exchange had been suggested as the mechanism

of electromagnetic forces. In this case the particles are photons which, being massless, are

not limited in range by Eq.(11.19). However, the greater the distance between two charges, the

smaller must be the energies of the photons that pass between them (and hence the less the mo-

menta of the photons and the weaker the resulting force) in order that the uncertainty princi-

ple not be violated. For this reason electric forces decrease with distance. Because the photons

exchanged in the interactions of electric charges cannot be detected, they are called virtual pho-

tons.As in the case of pions, they can become actual photons if enough energy is somehow

supplied to liberate them from the energy-conservation constraint.

The idea of photons as carriers of electromagnetic forces is attractive on many counts, an ob-

vious one being that it explains why such forces are transmitted with the speed of light and not,

say, instantaneously. As subsequently developed, the full theory is called quantum electrody-

namics (see Sec. 6.9). Its conclusions have turned out to be in extraordinanly precise agreement

with the data on such phenomena as the photoelectric and Compton effects, pair production

and annihilation, bremsstrahlung, and photon emission by excited atoms. Unfortunately the

details of the theory are too mathematically complex to consider here.

Virtual Photons

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