Bounded temporal growth condition for cubic dispersion

ID: bounded-temporal-growth-condition-for-cubic-dispersion

For , real-wavenumber growth is . A nonzero cubic coefficient is unbounded above on one side; after it vanishes, a positive quadratic coefficient is unbounded above on both sides. The displayed conditions are therefore necessary and sufficient for a finite temporal upper bound, which is then . The bound permits the initial causal temporal contour required by the Briggs-Bers criterion.

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