Laurent operators on circle L² #
A Laurent operator is multiplication by an essentially bounded symbol on L² of the circle;
in the Fourier basis e_n = exp (2πinx/T) it has the bi-infinite Toeplitz matrix of the Fourier
coefficients of its symbol. Concretely, ⟪e_m, e_n b⟫ = b̂(m - n) for every b ∈ L²
(TauCeti.inner_fourierBasis_multiplicationOperator_fourierLp). This file characterizes Laurent
operators in two ways.
TauCeti.eLpNorm_top_le_of_forall_mem_span_fourier: the multiplier criterion. If a measurable functionasatisfies‖a q‖_p ≤ C ‖q‖_pfor every trigonometric polynomialq, for some1 ≤ p < ∞, thenais essentially bounded with‖a‖∞ ≤ C. No integrability ofais assumed.TauCeti.commute_multiplicationOperator_fourierLp_one_iff: a bounded operator on circleL²commutes with the bilateral shift, multiplication bye_1, if and only if it is the multiplication operator of an essentially bounded symbol.
For the second statement, an operator W commuting with the bilateral shift sends e_n to
e_n b with b = W e_0 (TauCeti.apply_fourierBasis_of_commute), hence sends every
trigonometric polynomial q to b q (TauCeti.coeFn_apply_toLp_of_commute). Since
‖b q‖₂ ≤ ‖W‖ ‖q‖₂, the multiplier criterion makes b essentially bounded, and W agrees
with multiplication by b on the dense span of the Fourier basis.
These are the characterizations of bounded Laurent matrices through which Toeplitz operators on the Hardy space are recognized, as in the Brown–Halmos theorem. See A. Brown and P. R. Halmos, Algebraic properties of Toeplitz operators, J. Reine Angew. Math. 213 (1964), and A. Böttcher and B. Silbermann, Analysis of Toeplitz Operators, second edition, §2.
Multiplier criterion on the circle. If multiplication by a measurable function a on
the circle satisfies ‖a q‖_p ≤ C ‖q‖_p for every trigonometric polynomial q, for some
exponent 1 ≤ p < ∞, then a is essentially bounded by C.
The matrix coefficient ⟪e_m, e_n b⟫ of multiplication by the Fourier monomial e_n is the
Fourier coefficient b̂(m - n).
An operator on circle L² commuting with the bilateral shift, multiplication by e_1, sends
each Fourier mode e_n to e_n b, where b = W e_0.
An operator on circle L² commuting with the bilateral shift, multiplication by e_1,
multiplies every trigonometric polynomial q by b = W e_0.
Commutant of the bilateral shift. A bounded operator on circle L² commutes with the
bilateral shift, multiplication by the Fourier monomial e_1, if and only if it is
multiplication by an essentially bounded symbol.