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wCT S the particles 4-velocity 12.13 Specalize the Darwin Lagrangian (12.82) to the interaction of two charged particles (m,

action is known as the Breit interaction (1930). For system of interacting charged particles the complete Darwin can be writt

wCT S the particle's 4-velocity 12.13 Specalize the Darwin Lagrangian (12.82) to the interaction of two charged particles (m, q) and (m, qa). Introduce reduced particle coordinates X1X2, V -2 and also center of mass coordinates. Write out the Lagrangian in the reference frame in which the velocity of the center of mass vanishes and evaluate the canonical momentum components, p, aLlau (a) r = etc.
action is known as the Breit interaction (1930). For system of interacting charged particles the complete Darwin can be written down by expanding a Lagrangian, correct to order 1/c2 inclusive, the free-particle Lagrangian (12.7) for each particle and summing up all the in- teraction terms of the form (12.81). The result is 1 mo+ 2 LDarwin mot 8c 2 rii o od n (12.82) 1 + (v + where r= x, - x, , is a unit vector in the direction x, the double summation indicates the omission of the (self-energy) terms, i = Although the Darwin Lagrangian has had its most celebrated application in the quantum-mechanical context of the Breit interaction, it has uses in the purely classical domain. Two examples are cited in the suggested reading at the end of X, and the prime the chapter. See also the problems.
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