Abstract
By "causality of matter" one means its property not to admit superluminal excitations, i.e. excitations that propagate faster than the vacuum speed of light c. In discussing the propagation of small excitations, one has to distinguish between phase velocities ωj/k, (1≦j≦g=number of dispersion branches), group velocities dωj/dk, a front velocity vf: = {Mathematical expression} and the propagation speed vq:=(dp/dρ{variant})1/2 of isotropic quasistatic (small) perturbations. We discuss some of their properties. In particular, the (maximal) speed vs of small signals is not smaller than vf, and equals vf whenever the dispersion branches ωj(k) behave reasonably at infinity of the complex k-plane. In essence stronger conditions guarantee vq<vf (in which case vq≧c would imply superluminal behaviour).
| Original language | English |
|---|---|
| Pages (from-to) | 171-180 |
| Number of pages | 10 |
| Journal | Communications in Mathematical Physics |
| Volume | 60 |
| Issue number | 2 |
| DOIs | |
| State | Published - Jun 1978 |
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