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Single-Particle Electrodynamics - Assassination Science

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to particles carrying dipole moments, and obtain new, simplified expressions<br />

for the results. Finally, in Section 5.5, we review various aspects of the static<br />

fields from such particles, insofar as are required for the radiation reaction<br />

calculations to be undertaken in Chapter 6; as a by-product, we obtain the<br />

expression for the extra delta-function field required on the worldline of the<br />

particle, in the case of a magnetic moment, in order that the Maxwell equations<br />

be correctly satisfied.<br />

5.2 History of the retarded dipole fields<br />

That the fields generated by a particle carrying a dipole moment are richer<br />

(and, correspondingly, more mathematically complicated) than those generated<br />

by an electric charge can be appreciated before even writing down an<br />

equation. Firstly, one knows that a dipole must have internal degrees of freedom<br />

describing the orientation of the dipole in the rest frame of the particle;<br />

these degrees of freedom (and, in particular, their rates of change) will enter<br />

into the equations for the generated fields, in addition to those quantities<br />

already present in the electric charge case. Secondly, the static fields of a<br />

dipole fall off like R −3 (rather than R −2 as for an electric charge), which<br />

means that two time derivatives of the velocity and/or spin must be present<br />

to generate the “radiation” fields. (This can be seen on dimensional grounds:<br />

the four-velocity and unit four-spin are themselves dimensionless; there are<br />

no other kinematical quantities available apart from the proper time; and<br />

the radiation fields must, by definition, fall off like R −1 so that the energy it<br />

carries may propagate out indefinitely.)<br />

Perhaps due to this premonitory warning of extra complexity, the question<br />

of obtaining the general retarded fields for a particle with a dipole moment<br />

has not attracted much attention over the decades. Bhabha and Corben [40]<br />

appear to have been the first to make a substantial attack on this problem,<br />

in 1941, using methods developed two years earlier by Bhabha [39]. (See<br />

174

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