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Single-Particle Electrodynamics - Assassination Science

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) dependence to extract the three-gradient at t = 0. That this would begin<br />

to blow out the length of the algebraic expressions involved is recognised simply<br />

by considering the combinatorics of the available three-vector quantities.<br />

Nevertheless, the calculations in progress (to one lower of ε than ultimately<br />

required) were completed, for the kinematical expressions listed explicitly in<br />

Chapter 6. From there, the retarded fields of the electric charge only were<br />

expanded to this extra order in ε. This allowed a computation of all of the<br />

radiation reaction effects due to the electric charge fields, since there was<br />

now sufficient orders of ε to compute the gradient dipole forces.<br />

When this was done, the “spin renormalisation” effect, described in Chapter<br />

6, was one consequence. At first, this was perplexing. However, once the<br />

origin in terms of the static fields was clearly understood—and, moreover,<br />

agreement was found between the expression derived from the radiation reaction<br />

calculations and that from first principles—the feeling that the computations<br />

being undertaken were indeed physically correct was cemented.<br />

The results, to this point, had all been extensively cross-checked. All<br />

calculations were carried out twice, at separated intervals. The crucial threevector<br />

Taylor series expressions have a nice consistency check: the quantity<br />

γ(τ) may be computed two ways: from v(τ), or by taking the derivative<br />

d τ t(τ); these results agree. Quantities such as n, n ′ and n ′′ were dotproducted<br />

together, and the results compared with that expected (for example,<br />

n 2 = 1). The high degree of cancellation of a number of the terms<br />

in the integrated results also indicated that the calculations were most likely<br />

sound.<br />

The task of extending these calculations to another order in ε were then<br />

begun. They were carried out—and double-checked—up to the calculation of<br />

n. However, at this point, the combinatorical explosion began to wear down<br />

the author. Simply writing out expressions with more than seventy terms,<br />

with half a dozen or more factors in each, was excessively time-consuming.<br />

Moreover, little insight is required from that point, to the end of the com-<br />

412

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