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In Ref. [6] the distribution function is assumed to be constant in space and time. This is certainly not the most general situation imaginable in real heavy-ion collisions. However, the growth rate of the plasma instabilities is expected to be such that the time dependence due to the expansion of a realistic plasma can be neglected [8].
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18144399066
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note
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We have convinced ourselves of its generic nature by evolving, on various lattices, a few dozen configurations with randomly varying seed fields and different script N sign.
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28
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18144414432
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note
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This definition coincides with the definition in Ref. [7] in the simplifying case (10), but is gauge invariant also when the restriction to (1 + 1)-dimensional configurations is removed.
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29
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note
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* is zero there, the dominant energy component is from transverse electric fields, whereas the relative importance of magnetic fields drops with time.
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