Lax pair

The result can also be shown using the invariants ${\displaystyle \mathrm {tr} (L^{n})}$ for any ${\displaystyle n}$. These satisfy

$${\displaystyle {\frac {d}{dt}}\mathrm {tr} (L^{n})=0}$$

due to the Lax equation, and since the characteristic polynomial can be written in terms of these traces, the spectrum is preserved by the flow.[1]

The above property is the basis for the inverse scattering method. In this method, L and P act on a functional space (thus ψ = ψ(t,x)), and depend on an unknown function u(t,x) which is to be determined. It is generally assumed that u(0,x) is known, and that P does not depend on u in the scattering region where ${\displaystyle \Vert x\Vert \to \infty }$. The method then takes the following form:

1. Compute the spectrum of ${\displaystyle L(0)}$, giving ${\displaystyle \lambda }$ and ${\displaystyle \psi (0,x)}$,
2. In the scattering region where ${\displaystyle P}$ is known, propagate ${\displaystyle \psi }$ in time by using ${\displaystyle {\frac {\partial \psi }{\partial t}}(t,x)=P\psi (t,x)}$ with initial condition ${\displaystyle \psi (0,x)}$,
3. Knowing ${\displaystyle \psi }$ in the scattering region, compute ${\displaystyle L(t)}$ and/or ${\displaystyle u(t,x)}$.

If the Lax matrix additionally depends on a complex parameter ${\displaystyle z}$ (as is the case for say sine-Gordon), the equation

$${\displaystyle \det(wI-L(z))=0}$$

defines an algebraic curve in ${\displaystyle \mathbb {C} ^{2}}$ with coordinates ${\displaystyle w,z}$. By the isospectral property, this curve is preserved under time translation. This is the spectral curve. Such curves appear in the theory of Hitchin systems.[2]

The zero-curvature equations are described by a pair of matrix-valued functions ${\displaystyle A_{x}(x,t),A_{t}(x,t)}$, where the subscripts denote coordinate indices rather than derivatives. Often the ${\displaystyle (x,t)}$ dependence is through a single scalar function ${\displaystyle \varphi (x,t)}$ and its derivatives. The zero-curvature equation is then

$${\displaystyle \partial _{t}A_{x}-\partial _{x}A_{t}+[A_{x},A_{t}]=0.}$$

It is so called as it corresponds to the vanishing of the curvature tensor, which in this case is ${\displaystyle F_{\mu \nu }=[\partial _{\mu }-A_{\mu },\partial _{\nu }-A_{\nu }]=-\partial _{\mu }A_{\nu }+\partial _{\nu }A_{\mu }+[A_{\mu },A_{\nu }]}$. This differs from the conventional expression by some minus signs, which are ultimately unimportant.

For an eigensolution to the Lax operator ${\displaystyle L}$, one has

$${\displaystyle L\psi =\lambda \psi ,\psi _{t}+A\psi =0.}$$

If we instead enforce these, together with time independence of ${\displaystyle \lambda }$, instead the Lax equation arises as a consistency equation for an overdetermined system.

The Lax pair ${\displaystyle (L,P)}$ can be used to define the connection components ${\displaystyle (A_{x},A_{t})}$. When a PDE admits a zero-curvature representation but not a Lax equation representation, the connection components ${\displaystyle (A_{x},A_{t})}$ are referred to as the Lax pair, and the connection as a Lax connection.

The Korteweg–de Vries equation

${\displaystyle u_{t}=6uu_{x}-u_{xxx}.\,}$

can be reformulated as the Lax equation

${\displaystyle L_{t}=[P,L]\,}$

with

${\displaystyle L=-\partial _{x}^{2}+u\,}$ (a Sturm–Liouville operator)

${\displaystyle P=-4\partial _{x}^{3}+6u\partial _{x}+3u_{x}\,}$

where all derivatives act on all objects to the right. This accounts for the infinite number of first integrals of the KdV equation.

The previous example used an infinite dimensional Hilbert space. Examples are also possible with finite dimensional Hilbert spaces. These include Kovalevskaya top and the generalization to include an electric Field ${\displaystyle {\vec {h}}}$.[4]

${\displaystyle {\begin{aligned}L&={\begin{pmatrix}g_{1}+h_{2}&g_{2}+h_{1}&g_{3}&h_{3}\\g_{2}+h_{1}&-g_{1}+h_{2}&h_{3}&-g_{3}\\g_{3}&h_{3}&-g_{1}-h_{2}&g_{2}-h_{1}\\h_{3}&-g_{3}&g_{2}-h_{1}&g_{1}+h_{2}\\\end{pmatrix}}\lambda ^{-1}\\&+{\begin{pmatrix}0&0&-l_{2}&-l_{1}\\0&0&l_{1}&-l_{2}\\l_{2}&-l_{1}&-2\lambda &-2l_{3}\\l_{1}&l_{2}&2l_{3}&2\lambda \\\end{pmatrix}}\\P&={\frac {-1}{2}}{\begin{pmatrix}0&-2l_{3}&l_{2}&l_{1}\\2l_{3}&0&-l_{1}&l_{2}\\-l_{2}&l_{1}&2\lambda &2l_{3}+\gamma \\-l_{1}&-l_{2}&-2l_{3}&-2\lambda \\\end{pmatrix}}\end{aligned}}}$

In the Heisenberg picture of quantum mechanics, an observable A without explicit time t dependence satisfies

${\displaystyle {\frac {d}{dt}}A(t)={\frac {i}{\hbar }}[H,A(t)],}$

with H the Hamiltonian and ħ the reduced Planck constant. Aside from a factor, observables (without explicit time dependence) in this picture can thus be seen to form Lax pairs together with the Hamiltonian. The Schrödinger picture is then interpreted as the alternative expression in terms of isospectral evolution of these observables.

Further examples of systems of equations that can be formulated as a Lax pair include:

• Benjamin–Ono equation
• One-dimensional cubic non-linear Schrödinger equation
• Davey–Stewartson system
• Integrable systems with contact Lax pairs[5]
• Kadomtsev–Petviashvili equation
• Korteweg–de Vries equation
• KdV hierarchy
• Marchenko equation
• Modified Korteweg–de Vries equation
• Sine-Gordon equation
• Toda lattice
• Lagrange, Euler, and Kovalevskaya tops
• Belinski–Zakharov transform, in general relativity.

The last is remarkable, as it implies that both the Schwarzschild metric and the Kerr metric can be understood as solitons.