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Lyapunov Modes of Two-Dimensional Many-Body Systems; Soft ...

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768 Hoover et al.<br />

factor s into the Hamiltonian, (analogous to simple changes <strong>of</strong> length and<br />

mass units which leave phase volume unchanged)<br />

H=F+K 0 (F/s)+Ks,<br />

where the potential energy is the usual pairwise-additive sum:<br />

F — C fij; K— C p<br />

i

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