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Dispersionless (or quasi-classical) limits of
integrable In mathematics, integrability is a property of certain dynamical systems. While there are several distinct formal definitions, informally speaking, an integrable system is a dynamical system with sufficiently many conserved quantities, or first ...
partial differential equations In mathematics, a partial differential equation (PDE) is an equation which imposes relations between the various partial derivatives of a multivariable function. The function is often thought of as an "unknown" to be solved for, similarly to ...
(PDE) arise in various problems of mathematics and physics and have been intensively studied in recent literature (see e.g. references below). They typically arise when considering slowly modulated long waves of an integrable dispersive PDE system.


Examples


Dispersionless KP equation

The dispersionless
Kadomtsev–Petviashvili equation In mathematics and physics, the Kadomtsev–Petviashvili equation (often abbreviated as KP equation) is a partial differential equation to describe nonlinear wave motion. Named after Boris Borisovich Kadomtsev and Vladimir Iosifovich Petviash ...
(dKPE), also known (up to an inessential linear change of variables) as the Khokhlov–Zabolotskaya equation, has the form : (u_t+uu_)_x+u_=0,\qquad (1) It arises from the commutation : _1, L_20.\qquad (2) of the following pair of 1-parameter families of vector fields : L_1=\partial_y+\lambda\partial_x-u_x\partial_,\qquad (3a) : L_2=\partial_t+(\lambda^2+u)\partial_x+(-\lambda u_x+u_y)\partial_,\qquad (3b) where \lambda is a spectral parameter. The dKPE is the x-dispersionless limit of the celebrated
Kadomtsev–Petviashvili equation In mathematics and physics, the Kadomtsev–Petviashvili equation (often abbreviated as KP equation) is a partial differential equation to describe nonlinear wave motion. Named after Boris Borisovich Kadomtsev and Vladimir Iosifovich Petviash ...
, arising when considering long waves of that system. The dKPE, like many other (2+1)-dimensional integrable dispersionless systems, admits a (3+1)-dimensional generalization.


The Benney moment equations

The dispersionless KP system is closely related to the
Benney Benney () is a commune in the Meurthe-et-Moselle department in northeastern France. Population See also *Communes of the Meurthe-et-Moselle department The following is a list of the 591 communes of the Meurthe-et-Moselle department of Fr ...
moment hierarchy, each of which is a dispersionless integrable system: : A^n_ + A^_x + n A^ A^0_x =0. These arise as the consistency condition between : \lambda = p + \sum_^\infty A^n/p^, and the simplest two evolutions in the hierarchy are: : p_ + p p_x + A^0_x =0, : p_ + p^2 p_x + (p A^0+A^1)_x = 0, The dKP is recovered on setting : u = A^0, and eliminating the other moments, as well as identifying y=t_2 and t= t_3. If one sets A^n = h v^n, so that the countably many moments A^n are expressed in terms of just two functions, the classical
shallow water equations The shallow-water equations (SWE) are a set of hyperbolic partial differential equations (or parabolic if viscous shear is considered) that describe the flow below a pressure surface in a fluid (sometimes, but not necessarily, a free surface). ...
result: :h_y + (hv)_x=0, :v_y +v v_x + h_x=0. These may also be derived from considering slowly modulated wave train solutions of the nonlinear Schrodinger equation. Such 'reductions', expressing the moments in terms of finitely many dependent variables, are described by the Gibbons-Tsarev equation.


Dispersionless Korteweg–de Vries equation

The dispersionless Korteweg–de Vries equation (dKdVE) reads as : u_=uu_.\qquad (4) It is the dispersionless or quasiclassical limit of the Korteweg–de Vries equation. It is satisfied by t_2-independent solutions of the dKP system. It is also obtainable from the t_3-flow of the Benney hierarchy on setting : \lambda^2 = p^2 + 2A^0.


Dispersionless Novikov–Veselov equation

The dispersionless Novikov-Veselov equation is most commonly written as the following equation for a real-valued function v=v(x_1,x_2,t): : \begin & \partial_ v = \partial_( v w ) + \partial_( v \bar w ), \\ & \partial_ w = - 3 \partial_ v, \end where the following standard notation of complex analysis is used: \partial_ = \frac ( \partial_ - i \partial_ ) , \partial_ = \frac ( \partial_ + i \partial_ ) . The function w here is an auxiliary function, defined uniquely from v up to a holomorphic summand.


Multidimensional integrable dispersionless systems

See for systems with contact Lax pairs, and e.g., and references therein for other systems.


See also

*
Integrable systems In mathematics, integrability is a property of certain dynamical systems. While there are several distinct formal definitions, informally speaking, an integrable system is a dynamical system with sufficiently many conserved quantities, or first ...
*
Nonlinear Schrödinger equation In theoretical physics, the (one-dimensional) nonlinear Schrödinger equation (NLSE) is a nonlinear variation of the Schrödinger equation. It is a classical field equation whose principal applications are to the propagation of light in nonlin ...
*
Nonlinear systems In mathematics and science, a nonlinear system is a system in which the change of the output is not proportional to the change of the input. Nonlinear problems are of interest to engineers, biologists, physicists, mathematicians, and many other ...
*
Davey–Stewartson equation In fluid dynamics, the Davey–Stewartson equation (DSE) was introduced in a paper by to describe the evolution of a three-dimensional wave-packet on water of finite depth. It is a system of partial differential equations for a complex ( wave-am ...
*
Dispersive partial differential equation In mathematics, a dispersive partial differential equation or dispersive PDE is a partial differential equation that is dispersive. In this context, dispersion means that waves of different wavelength propagate at different phase velocities. ...
*
Kadomtsev–Petviashvili equation In mathematics and physics, the Kadomtsev–Petviashvili equation (often abbreviated as KP equation) is a partial differential equation to describe nonlinear wave motion. Named after Boris Borisovich Kadomtsev and Vladimir Iosifovich Petviash ...
* Korteweg–de Vries equation


References

* Kodama Y., Gibbons J. "Integrability of the dispersionless KP hierarchy", Nonlinear World 1, (1990). * Zakharov V.E. "Dispersionless limit of integrable systems in 2+1 dimensions", Singular Limits of Dispersive Waves, NATO ASI series, Volume 320, 165-174, (1994). * * * * * Dunajski M. "Solitons, instantons and twistors", Oxford University Press, 2010. * {{cite journal , arxiv=1401.2122 , doi=10.1007/s11005-017-1013-4 , title=New integrable (3+1)-dimensional systems and contact geometry , year=2018 , last1=Sergyeyev , first1=A. , s2cid=119159629 , journal=Letters in Mathematical Physics , volume=108 , issue=2 , pages=359–376 , bibcode=2018LMaPh.108..359S * Takebe T. "Lectures on Dispersionless Integrable Hierarchies", 2014, https://rikkyo.repo.nii.ac.jp/index.php?action=pages_view_main&active_action=repository_action_common_download&item_id=9046&item_no=1&attribute_id=22&file_no=1&page_id=13&block_id=49


External links


Ishimori_system
at the dispersive equations wiki Partial differential equations Integrable systems