On tau functions associated with linear systems

О тау-функциях, связанных с линейными системами
Gordon Blower, Samantha L. Newsham
2012-07-09

Fredholm determinantsHankel integral operatorsLyapunov equationlinear systemstau functions
Let $(-A,B,C)$ be a linear system in continuous time $t>0$ with input and output space ${\bf C}$ and state space $H$. The function $ϕ_{(x)}(t)=Ce^{-(t+2x)A}B$ determines a Hankel integral operator $Γ_{ϕ_{(x)}}$ on $L^2((0, \infty ); {\bf C})$; if $Γ_{ϕ_{(x)}}$ is trace class, then the Fredholm determinant $τ(x)=\det (I+ Γ_{ϕ_{(x)}})$ defines the tau function of $(-A,B,C)$. Such tau functions arise in Tracy and Widom's theory of matrix models, where they describe the fundamental probability distributions of random matrix theory. Dyson considered such tau functions in the inverse spectral problem for Schrödinger's equation $-f''+uf=λf$, and derived the formula for the potential $u(x)=-2{{d^2}\over{dx^2}}\log τ(x)$ in the self-adjoint scattering case {\sl Commun. Math. Phys.} {\bf 47} (1976), 171--183. This paper introduces a operator function $R_x$ that satisfies Lyapunov's equation ${{dR_x}\over{dx}}=-AR_x-R_xA$ and $τ(x)=\det (I+R_x)$, without assumptions of self-adjointness. When $-A$ is sectorial, and $B,C$ are Hilbert--Schmidt, there exists a non-commutative differential ring ${\cal A}$ of operators in $H$ and a differential ring homomorphism $\lfloor\,\,\rfloor :{\cal A}\rightarrow {\bf C}[u,u', \dots ]$ such that $u=-4\lfloor A\rfloor$, which provides a substitute for the multiplication rules for Hankel operators considered by Pöppe, and McKean {\sl Cent. Eur. J. Math.} {\bf 9} (2011), 205--243. The paper obtains conditions on $(-A,B,C)$ for Schrödinger's equation with meromorphic $u$ to be integrable by quadratures. Special results apply to the linear systems associated with scattering $u$, periodic $u$ and elliptic $u$. The paper constructs a family of solutions to the Kadomtsev--Petviashivili differential equations, and proves that certain families of tau functions satisfy Fay's identities.\par
1
For sectorial −A with Hilbert–Schmidt B and C, it constructs a noncommutative differential ring and homomorphism yielding u = −4⌊A⌋, replacing Hankel-operator multiplication rules.
2
It constructs families of Kadomtsev–Petviashvili solutions and proves that certain tau-function families satisfy Fay identities.
3
It derives conditions under which Schrödinger equations with meromorphic potentials are integrable by quadratures, including scattering, periodic, and elliptic potentials.
4
It introduces an operator function R_x satisfying the Lyapunov equation dR_x/dx = −AR_x − R_xA, with tau(x) = det(I + R_x), without assuming self-adjointness.
5
The paper defines tau functions as Fredholm determinants of Hankel operators generated by continuous-time linear systems.

Tau functions and associated linear systems, including their Hankel operators and Schrödinger potentials

Determinant representations, differential-algebraic structure, integrability, and identities of these tau functions, including their connection to meromorphic Schrödinger potentials, KP solutions, and Fay identities

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2012-07-09
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Gordon Blower
Samantha L. Newsham
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