Skew multiples of self-adjoint operators are m-dissipative #
Multiplication by a nonzero purely imaginary scalar c turns a self-adjoint partial linear map
A on a complex Hilbert space into an m-dissipative real partial linear map: the quadratic form
of c • A is purely imaginary, so its real restriction is dissipative, and the range condition,
surjectivity of 1 - c • A, is the surjectivity of the nonreal shift c⁻¹ - A of A, since
1 - c • A = c • (c⁻¹ - A). Together with the density of the domain of a self-adjoint operator
(IsSelfAdjoint.dense_domain), this is the hypothesis set of the Lumer--Phillips theorem; at
c = ± i it produces the two contraction semigroups whose gluing is the unitary group e^{itA}.
Main results #
LinearPMap.IsFormalAdjoint.isDissipative_smul_restrictScalars: for a symmetricAand a purely imaginaryc, the real restriction ofc • Ais dissipative.IsSelfAdjoint.one_smul_sub_smul_restrictScalars_surjective: for self-adjointAand nonrealc,1 - c • Ais surjective.IsSelfAdjoint.isMDissipative_smul_restrictScalars: for self-adjointAand a nonzero purely imaginaryc, the real restriction ofc • Ais m-dissipative.
The statements are in the simp-normal form c • A.restrictScalars ℝ of
LinearPMap.restrictScalars_smul.
References #
- K.-J. Engel and R. Nagel, One-Parameter Semigroups for Linear Evolution Equations, Theorem II.3.24 (Stone's theorem) and the surrounding discussion.
- A. Pazy, Semigroups of Linear Operators and Applications to Partial Differential Equations, Theorem 1.10.8.
The real restriction of a purely imaginary multiple of a formally self-adjoint (symmetric) partial linear map is dissipative: its real quadratic form vanishes.
The range condition for a nonreal multiple c • A of a self-adjoint partial linear map:
1 - c • A = c • (c⁻¹ - A) is surjective because the nonreal shift c⁻¹ - A is.
c • A is m-dissipative for self-adjoint A and nonzero purely imaginary c. The real
restriction of c • A is dissipative, because its quadratic form is purely imaginary, and
1 - c • A is surjective, because the nonreal shift c⁻¹ - A is.