Phase shifts of a complex-linear strongly continuous semigroup #
For a C₀-semigroup S acting by complex-linear operators on a complex Banach space and a real
number b, the phase shift is the semigroup
(S.phaseShift hS b) t = exp (-i b t) • S t.
Unlike the exponential shift t ↦ exp (-omega t) • S t of
TauCeti/Analysis/Semigroups/ExponentialShift.lean, which damps the semigroup and moves its
growth exponent, a phase shift multiplies by a unimodular scalar: it preserves every growth
bound (omega, M) exactly, and it subtracts i b from the generator. Composing the two shifts
realizes t ↦ exp (-lambda t) • S t for an arbitrary complex lambda.
This is the device that moves a spectral parameter parallel to the imaginary axis. Since the
Laplace-transform resolvent of a C₀-semigroup is a real-variable construction, it only ever
produces real points of the resolvent set; the phase shift converts a real point for the shifted
semigroup into the point lambda = mu + i b for S, which is how the complex resolvent set of
the complex generator is reached in
TauCeti/Analysis/Semigroups/Resolvent/Complex.lean.
Main definitions and results #
TauCeti.Semigroups.StronglyContinuousSemigroup.phaseShift: the semigroupt ↦ exp (-i b t) • S t.TauCeti.Semigroups.StronglyContinuousSemigroup.IsComplexLinear.phaseShiftandTauCeti.Semigroups.StronglyContinuousSemigroup.HasGrowthBound.phaseShift: a phase shift is again complex linear, and has the same growth bounds.TauCeti.Semigroups.StronglyContinuousSemigroup.phaseShift_domain: a phase shift does not change the generator domain.TauCeti.Semigroups.StronglyContinuousSemigroup.complexGenerator_phaseShift: the complex generator oft ↦ exp (-i b t) • S tisA - i b.
References #
- K.-J. Engel and R. Nagel, One-Parameter Semigroups for Linear Evolution Equations, Section II.2.2 (rescaled semigroups).
The phase shift of a complex-linear C₀-semigroup by b : ℝ: the semigroup
t ↦ exp (-i b t) • S t.
Equations
Instances For
The native nonnegative-time operator of a phase shift.
Pointwise form of StronglyContinuousSemigroup.phaseShift_apply.
Real-time form of a phase-shifted operator at nonnegative times.
Pointwise real-time form of a phase-shifted operator at nonnegative times.
A phase shift is again complex linear.
The zero phase shift is the original semigroup.
Successive phase shifts add their parameters.
A phase shift multiplies by a unimodular scalar, so it preserves every growth bound.
The generator of a phase shift #
A phase shift does not change the generator domain.
The generator of a phase-shifted semigroup acts as A - i b.
The generator of a phase shift. The complex generator of t ↦ exp (-i b t) • S t is
A - i b, where A is the complex generator of S.