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84894023101
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note
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In the present context left-handed and right-handed are unrelated to chirality.
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14
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84894018742
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note
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0 as ω → ∞.
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∞s(t′)g (z,t-t′)dt′. Given that g(z,t)=0 for t<(z/c), the field ψ(z,t) depends only on the source s(t) for a time later than t>(z/c), such that the onset of the disturbance (Academic) propagates at exactly the speed c
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∞s(t′) g(z,t-t′)dt′. Given that g(z,t)=0 for t<(z/c), the field ψ(z,t) depends only on the source s(t) for a time later than t>(z/c), such that the onset of the disturbance (see Ref. 11) propagates at exactly the speed c.
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Wave Propagation and Group Velocity
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Brillouin, L.1
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18
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84894015588
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note
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μ are entirely determined by the zero-pole pair on the positive frequency side. Our results do not rely on this particular simplification and they apply to the general case where the contribution from the negative frequency zero-pole pairs is included.
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24
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84894022212
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note
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i.
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