The Existence and Uniqueness of Solutions to N-Body Problem of Electrodynamics
Given $n$ charges interacting with each other according to Feynman's law. Let $(r_j(t),v_j(t))$ denote the position and velocity of the charge $q_j.$ The list $y(t)$ of all such vectors is called a trajectory. A Lipschitzian trajectory $x(t), (t\le0),$ with continuous derivative, on which the v...
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Zusammenfassung: | Given $n$ charges interacting with each other according to Feynman's law. Let
$(r_j(t),v_j(t))$ denote the position and velocity of the charge $q_j.$ The
list $y(t)$ of all such vectors is called a trajectory. A Lipschitzian
trajectory $x(t), (t\le0),$ with continuous derivative, on which the velocities
do not exceed some limiting velocity $v |
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DOI: | 10.48550/arxiv.0909.1493 |