Proof of Well-Posedness of the Hamilton-Jacobi Equation of the Controlled Heat Equation with Square-Integrable White Noise on the Torus
corollarycor:white-noise-heat-hamilton-jacobi-well-posed-torus-2026aThe hypotheses of the abstract well-posedness theorem on a Hilbert triple are checked one by one against the data lemma for the Sobolev triple: infinite dimension, the zero nonlinearity, the contraction minus the identity, the square-summable trigonometric white noise, and the bounded uniformly continuous running cost.
Each result cited is universally quantified over the data in its own statement, and is applied here to the Sobolev triple of order , the enumeration and the data named in the present statement. Let be the zero map, , and the map , as in The Data of the Hamilton-Jacobi Equation of the Heat Equation with Square-Integrable White Noise on the Torus: the Noise, the Nonlinearities and the Drift, whose noise sequence and whose triple are those of the present statement.
We apply Well-Posedness for a Viscous Hamilton-Jacobi Equation with a Monotone Nonlinearity on a Hilbert Triple with its Hilbert triple taken to be , whose standing separability hypothesis Hilbert Triples: Standing Notation and Background §separable holds by The Negative-Order Sobolev Triple of the Torus: a Diagonal Hilbert Triple whose Form Operator Is One Minus the Laplacian §triple. Its hypotheses are met, one by one, as follows.
1. , as a vector space over , is not finite-dimensional, by The Data of the Hamilton-Jacobi Equation of the Heat Equation with Square-Integrable White Noise on the Torus: the Noise, the Nonlinearities and the Drift §not-finite-dimensional.
2. The number of that theorem is taken to be , which satisfies , and satisfies ; is a modulus of continuity; and is bounded in absolute value by and satisfies for all . These are hypotheses of the present statement.
3. is a monotone nonlinearity for , by The Data of the Hamilton-Jacobi Equation of the Heat Equation with Square-Integrable White Noise on the Torus: the Noise, the Nonlinearities and the Drift §zero-nonlinearity.
4. The number of that theorem is taken to be , which is nonnegative, and is Lipschitz with constant from to itself, by The Data of the Hamilton-Jacobi Equation of the Heat Equation with Square-Integrable White Noise on the Torus: the Noise, the Nonlinearities and the Drift §lipschitz.
5. The numbers and satisfy and , by hypothesis.
6. The sequence is square-summable in , by The Data of the Hamilton-Jacobi Equation of the Heat Equation with Square-Integrable White Noise on the Torus: the Noise, the Nonlinearities and the Drift §noise, and is the trace along , as fixed in the present statement.
Claim 1. By items 1 to 6 every hypothesis of Well-Posedness for a Viscous Hamilton-Jacobi Equation with a Monotone Nonlinearity on a Hilbert Triple is satisfied by the present data, with in the role of , with the zero map, and with and . The function displayed in that theorem for these data has value at , and by claim 1 of Elementary Identities in a Vector Space and claim 2 of that lemma; so it is the function of The Hamilton-Jacobi Equation of the Controlled Heat Equation with Square-Integrable White Noise on the Torus §operator, displayed in the present statement. That theorem records that is a second-order equation operator on relative to that is degenerate elliptic, by A Viscous Hamilton-Jacobi Operator with a Monotone Nonlinearity Satisfies the Second-Order Comparison Hypotheses §operator. This proves claim 1.
Claim 2. By Well-Posedness for a Viscous Hamilton-Jacobi Equation with a Monotone Nonlinearity on a Hilbert Triple §existence there is a function that is a viscosity solution of on , satisfies for every with the quotient of by the nonzero , which that theorem records as nonnegative, and is uniformly continuous on with respect to and the metric of Real Hilbert Spaces: Standing Notation and Background §numbers. By Well-Posedness for a Viscous Hamilton-Jacobi Equation with a Monotone Nonlinearity on a Hilbert Triple §well-posedness this is continuous on , and any viscosity solution of on that is continuous on and satisfies for every , for some , agrees with at every point of . These are the assertions of claim 2.
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Prerequisites
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