1992
DOI: 10.1016/0022-0396(92)90143-b
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Steady solutions of the Kuramoto-Sivashinsky equation for small wave speed

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Cited by 13 publications
(17 citation statements)
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“…For this system, an unfolding of (3) which has been widely studied (see [Mic86], [JTM92], [KT76], [RMT97]), there is a rigorous proof of an asymptotic formula of the heteroclinic splitting given in [RMT97]. The proof, which falls in the context of singular perturbation theory, draws heavily on the fact that the Michelson system comes from a third-order differential equation.…”
Section: Some Comments About the Singular Case P = −2mentioning
confidence: 99%
“…For this system, an unfolding of (3) which has been widely studied (see [Mic86], [JTM92], [KT76], [RMT97]), there is a rigorous proof of an asymptotic formula of the heteroclinic splitting given in [RMT97]. The proof, which falls in the context of singular perturbation theory, draws heavily on the fact that the Michelson system comes from a third-order differential equation.…”
Section: Some Comments About the Singular Case P = −2mentioning
confidence: 99%
“…We are therefore led to the bounded existence interval of the solution to (11). Lemma 2.3 is also utilized to prove (7), (8). We show (8); the proof of (7) is handled similarly.…”
Section: By Virtue Of Yoe(x)=−`v(y(x))mentioning
confidence: 95%
“…We remark that Toland [17] already made an elementary but ingenious approach to proving the nonexistence of monotonic solutions of (1), (2) if l \ 2/9. Expanding on the existence of solutions to (1), (2), we recall that Jones et al [8] exhibit that there is an odd periodic solution for all small l > 0. We again refer to [15], where the existence of a unique monotonic solution to (1), (2) is shown with l=1/2 on the half interval {0 [ x < .}…”
Section: F(y) Ymentioning
confidence: 98%
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