KdV hierarchy: Difference between revisions
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The [[Korteweg-de Vries equation]] | The [[Korteweg-de Vries equation]] | ||
<center><math>\partial_t V | <center><math>\partial_t V + \partial_x^3 V = 6 V \partial_x V</math></center> | ||
<span class="GramE">can</span> be rewritten in the Lax Pair form | <span class="GramE">can</span> be rewritten in the Lax Pair form | ||
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where <math>L</math> is the second-order operator | where <math>L</math> is the second-order operator | ||
<center><math>L = -D^2 | <center><math>L = -D^2 + V</math></center> | ||
<math>(D = d/dx)</math> and <math>P</math> is the third-order antiselfadjoint operator | <math>(D = d/dx)</math> and <math>P</math> is the third-order antiselfadjoint operator | ||
<center><math>P = 4D^3 | <center><math>P = 4D^3 + 3(DV + VD)</math>.</center> | ||
''Note''that <math>P</math> consists of the zeroth order and higher terms of the formal power series expansion of <math>4i L^{3/2}</math>). | ''Note'' that <math>P</math> consists of the zeroth order and higher terms of the formal power series expansion of <math>4i L^{3/2}</math>). | ||
One can replace <math>P</math> with other fractional powers of L. For instance, the zeroth order and higher terms of <math>4i L^{5/2}</math> are | One can replace <math>P</math> with other fractional powers of L. For instance, the zeroth order and higher terms of <math>4i L^{5/2}</math> are | ||
<center><math>P = 4D^5 | <center><math>P = 4D^5 + 5(D^3 V + V D^3) - 5/4 (D \partial^2_x V + \partial_x^2 V D) + 15/4 (D V^2 + V^2 D)</math></center> | ||
and the Lax pair equation becomes | and the Lax pair equation becomes | ||
<center><math>\partial_t V | <center><math>\partial_t V + \partial_x^5 u = \partial_x (5 V_x^2 + 10 V V_xx + 10 V^3)</math></center> | ||
with Hamiltonian | with Hamiltonian | ||
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The ''KdV hierarchy'' are examples of higher order water wave models; a general formulation is | The ''KdV hierarchy'' are examples of higher order water wave models; a general formulation is | ||
<center><math>\partial_t u | <center><math>\partial_t u + \partial_x^{2j+1} u = P(u, u_x , ..., \partial_x^{2j} u)</math></center> | ||
where <math>u</math> is real-valued and <math>P</math> is a polynomial with no constant or linear terms; thus KdV and gKdV correspond to j=1, and the higher order equations in the hierarchy correspond to j=2,3,etc. LWP for these equations in high regularity Sobolev spaces is in [[KnPoVe1994]], and independently by Cai (ref?); see also [[CrKpSr1992]].The case j=2 was studied by Choi</span> (ref?).The non-scalar diagonal case was treated in [[KnSt1997]]; the periodic case was studied in [Bo-p3].Note in the periodic case it is possible to have ill-posedness for every regularity, for instance <math>\partial_t u | where <math>u</math> is real-valued and <math>P</math> is a polynomial with no constant or linear terms; thus KdV and gKdV correspond to j=1, and the higher order equations in the hierarchy correspond to j=2,3,etc. LWP for these equations in high regularity Sobolev spaces is in [[KnPoVe1994]], and independently by Cai (ref?); see also [[CrKpSr1992]].The case j=2 was studied by Choi</span> (ref?).The non-scalar diagonal case was treated in [[KnSt1997]]; the periodic case was studied in [Bo-p3].Note in the periodic case it is possible to have ill-posedness for every regularity, for instance <math>\partial_t u + u_{xxx} = u^2 u_x^2</math> is ill-posed in every <math>H^s</math> [Bo-p3] | ||
[[Category:Integrability]] | [[Category:Integrability]] | ||
[[Category:Equations]] [[Category:Airy]] | [[Category:Equations]] [[Category:Airy]] |
Latest revision as of 20:10, 11 June 2007
The Korteweg-de Vries equation
can be rewritten in the Lax Pair form
where is the second-order operator
and is the third-order antiselfadjoint operator
Note that consists of the zeroth order and higher terms of the formal power series expansion of ).
One can replace with other fractional powers of L. For instance, the zeroth order and higher terms of are
and the Lax pair equation becomes
with Hamiltonian
These flows all commute with each other and their Hamiltonians are conserved by all the flows simultaneously.
The KdV hierarchy are examples of higher order water wave models; a general formulation is
where is real-valued and is a polynomial with no constant or linear terms; thus KdV and gKdV correspond to j=1, and the higher order equations in the hierarchy correspond to j=2,3,etc. LWP for these equations in high regularity Sobolev spaces is in KnPoVe1994, and independently by Cai (ref?); see also CrKpSr1992.The case j=2 was studied by Choi (ref?).The non-scalar diagonal case was treated in KnSt1997; the periodic case was studied in [Bo-p3].Note in the periodic case it is possible to have ill-posedness for every regularity, for instance is ill-posed in every [Bo-p3]