Commutants of operators

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Let HH be a Hilbert space over the field K\mathbb {K}, and A∈L(H)A \in \mathcal{L}(H) be such that AB=BAA B = B A for all B∈L(H)B \in \mathcal{L}(H). Prove that A=γIA = \gamma I for some γ∈K\gamma \in \mathbb {K}.

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If A∈B(H)A \in \mathcal{B}(\mathcal{H}) and AT=TAAT=TA for every compact operator TT, show that AA is a multiple of the identity operator.

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Suppose TT is a compact normal operator on a C\mathbb {C}-Hilbert space such that dim⁡ker⁡(T−λ)≤1\dim \ker (T-\lambda ) \leq 1 for all λ\lambda in C\mathbb {C}. Show that if A∈B(H)A \in \mathcal{B}(\mathcal{H}) and AT=TAAT=TA, then A=ϕ(T)A = \phi (T) for some ϕ\phi in l∞(C)l^{\infty }(\mathbb {C}).

Definition 7.10 (context): Denote by l∞(C)l^{\infty }(\mathbb {C}) all the bounded functions ϕ:C→C\phi : \mathbb {C} \rightarrow \mathbb {C}. If TT is a compact normal operator satisfying T=∑n=1∞λnPnT = \sum_{n=1}^{\infty } \lambda_{n} P_{n} (7.7), define ϕ(T):H→H\phi (T): \mathcal{H} \rightarrow \mathcal{H} by

ϕ(T)=∑n=1∞ϕ(λn)Pn+ϕ(0)P0, \phi (T) = \sum _{n=1}^{\infty } \phi (\lambda _{n}) P_{n} + \phi (0) P_{0},

where P0P_{0} is the projection of H\mathcal{H} onto ker⁡T\ker T.

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Prove a converse to Exercise 8: if TT is a compact normal operator such that {A∈B(H):AT=TA}={ϕ(T):ϕ∈l∞(C)}\left\{ A \in \mathcal{B}(\mathcal{H}): AT=TA\right\} = \left\{ \phi (T): \phi \in l^{\infty }(\mathbb {C})\right\}, then dim⁡ker⁡(T−λ)≤1\dim \ker (T-\lambda ) \leq 1 for all λ\lambda in C\mathbb {C}.

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Let TT be a compact normal operator and show that dim⁡ker⁡(T−λ)≤1\dim \ker (T-\lambda ) \leq 1 for all λ\lambda in C\mathbb {C} if and only if there is a vector hh in H\mathcal{H} such that {p(T)h:p is a polynomial in one variable}\left\{ p(T)h: p \text{ is a polynomial in one variable}\right\} is dense in H\mathcal{H}. (Such a vector hh is called a cyclic vector for TT.)

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If λ∈C\lambda \in \mathbb {C}, let δλ\delta_{\lambda } be the unit point mass at λ\lambda; that is, δλ\delta_{\lambda } is the measure on C\mathbb {C} such that δλ(Δ)=1\delta_{\lambda }(\Delta ) = 1 if λ∈Δ\lambda \in \Delta and δλ(Δ)=0\delta_{\lambda }(\Delta ) = 0 if λ∉Δ\lambda \notin \Delta. If {λ1,λ2,…}\left\{ \lambda_{1}, \lambda_{2}, \ldots \right\} is a bounded sequence of distinct complex numbers and {αn}\left\{ \alpha_{n}\right\} is a sequence of real numbers with αn>0\alpha_{n} > 0 and ∑nαn<∞\sum_{n} \alpha_{n} < \infty, let μ=∑n=1∞αnδλn\mu = \sum_{n=1}^{\infty } \alpha_{n} \delta_{\lambda_{n}}; so μ\mu is a finite measure. If ϕ∈l∞(C)\phi \in l^{\infty }(\mathbb {C}), let MϕM_{\phi } be the multiplication operator on L2(μ)L^{2}(\mu ). Define T:L2(μ)→L2(μ)T: L^{2}(\mu ) \rightarrow L^{2}(\mu ) by (Tf)(λn)=λnf(λn)(Tf)(\lambda_{n}) = \lambda_{n} f(\lambda_{n}). Prove:

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(a)

TT is a normal operator;

(b)

TT has a cyclic vector (see Exercise 10);

(c)

if A∈B(H)A \in \mathcal{B}(\mathcal{H}) and AT=TAAT=TA, then A=MϕA = M_{\phi } for some ϕ\phi in l∞(C)l^{\infty }(\mathbb {C});

(d)

TT is compact if and only if λn→0\lambda_{n} \rightarrow 0;

(e)

if TT is compact, find all of the cyclic vectors for TT;

(f)

if TT is compact, find the decomposition (7.7) for TT.

The commutant of the bilateral shift is the set of all multiplications.

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Remark.
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The commutant of an operator (or of a set of operators) is the set of all operators that commute with it (or with each operator in the set). The bilateral shift WW can be viewed as multiplication by e1e_1 on L2L^{2} of the unit circle. Here en(z)=zne_n(z) = z^n (n=0,±1,±2,…n = 0, \pm 1, \pm 2, \ldots) whenever ∣z∣=1\left|z\right| = 1, and L2L^2 is formed with normalized Lebesgue measure.

The commutant of the unilateral shift is the set of all restrictions to H2\mathbf{H}^2 of multiplications by multipliers in H∞\mathbf{H}^{\infty }.

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Remark.
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The commutant of an operator (or of a set of operators) is the set of all operators that commute with it (or with each operator in the set). The unilateral shift is the restriction of the bilateral shift WW to H2\mathbf{H}^2, where H2\mathbf{H}^2 is the closed span in L2L^2 of the unit circle of the functions ene_n, n=0,1,2,…n = 0, 1, 2, \ldots (with en(z)=zne_n(z) = z^n), and H∞\mathbf{H}^{\infty } is the set of essentially bounded functions in H2\mathbf{H}^2. If the bilateral shift is regarded as a multiplication (by e1e_1 on L2L^2), then its commutant is the set of all multiplications on the same L2L^2 (Problem 146). If, however, the multiplier itself is in H2\mathbf{H}^2 (and hence in H∞\mathbf{H}^{\infty }), then H2\mathbf{H}^2 is invariant under the induced multiplication (cf. Problem 34), and the restriction of that multiplication to H2\mathbf{H}^2 makes sense.

Every operator that commutes with the unilateral shift is the limit (strong operator topology) of a sequence of polynomials in the unilateral shift.

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Prove that every continuous operator in S(Rn)S(\mathbb {R}^{n}) that commutes with the operators MkM_k, 1≤k≤n1\leq k\leq n, (see Problem 580) is the operator of multiplication by a function.

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Prove that every continuous operator in S(Rn)S(\mathbb {R}^{n}) that commutes with the operators MkM_k and DkD_k, 1≤k≤n1\leq k\leq n, (see Problem 580) is a scalar operator.

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Let SS be some set of operators in a linear space LL. Let S′S' be the collection of operators in LL that commute with all the operators in SS. For what operators AA does the equality A(A)′=A(A)\mathfrak A(A)'=\mathfrak A(A) hold?

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In the space of 2n×2n2n\times 2n matrices find a subspace of dimension 1+n21+n^2 consisting of pairwise commuting matrices.

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Let AA be the operator on L2([(0,∞),dx])L^{2}\left({[(0,\infty ),dx]}\right) given by the formula Af(x)=∫0∞[f(y)/(x+y)] dyAf(x)=\int_0^\infty [f(y)/(x+y)]\, dy. Prove that AA commutes with the dilation operators L(a):f(x)↦f(ax)L(a):f(x)\mapsto f(ax).

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Suppose that BB and CC are bounded selfadjoint operators that commute. Prove that there exists a bounded selfadjoint operator AA such that BB and CC are functions of AA.

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Let AA be a selfadjoint operator with simple spectrum. Prove that every bounded operator BB that commutes with AA is a function of AA.

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Prove that any family of pairwise commuting bounded selfadjoint operators on a separable Hilbert space can be simultaneously reduced to the form of multiplication by a function.

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References

[BCK+24] Brayman V.B., Chaikovskyi A.V., Konstantinov O.Y., Kukush A.G., Mishura Y.S., Nesterenko O.N. Functional Analysis and Operator Theory. Springer, 2024.
[Con07] Conway J.B. A Course in Functional Analysis. 2nd ed., Springer, 2007.
[Hal82] Halmos P.R. A Hilbert Space Problem Book. 2nd ed., Springer-Verlag, 1982.
[KiGv88] Kirillov A.A., Gvishiani A.D. Теоремы и задачи функционального анализа. 2-е изд., Наука, 1988.