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Proof of Finite Direct Sums of a Complex Hilbert Space: the Hilbert Structure, Coordinate Inclusions, Block Entries of Bounded Operators and Commutation with Diagonal Operators

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· 13,569 chars · 20 deps · depth 13 Reason: Proof of the finite direct sum lemma.

The Hilbert structure of HmH^m is checked componentwise, completeness coming from componentwise limits; the coordinate projection is shown to be the adjoint of each inclusion, and the block-entry formulas, the converse, and the diagonal-operator statements then follow from the identity that the sum of the inclusions composed with their adjoints is the identity.

Proof

For ζ∈Hm\zeta\in H^{m} and k∈[m]k\in[m], ζk\zeta_{k} is the kk-th component of ζ\zeta; by definition of the operations, (ζ+ζ′)k=ζk+ζk′(\zeta+\zeta')_{k}=\zeta_{k}+\zeta'_{k} and (λζ)k=λζk(\lambda\zeta)_{k}=\lambda\zeta_{k} for ζ,ζ′∈Hm\zeta,\zeta'\in H^{m} and λ∈C\lambda\in\mathbb{C}, and two elements of HmH^{m} are equal when all their components are equal. For k∈[m]k\in[m] let πk:Hm→H\pi_{k}:H^{m}\to H be the map ζ↦ζk\zeta\mapsto\zeta_{k}; it is linear by the preceding formulas.

1. (Hilbert structure) Vector space. Each condition of Vector Space over a Field for HmH^{m}, read in the kk-th component, is the same condition for HH; the tuple all of whose components are 00 is a zero vector of HmH^{m}, and (−ζ1,…,−ζm)(-\zeta_{1},\dots,-\zeta_{m}) is an additive inverse of ζ\zeta. So HmH^{m} is a complex vector space.

Inner product. Let ζ,ζ′,ζ′′∈Hm\zeta,\zeta',\zeta''\in H^{m} and λ∈C\lambda\in\mathbb{C}. By condition 1 of Complex Inner Product Space for HH and claim 4 of Properties of Finite Sums,

⟨ζ,ζ′⟩Hm=∑k=1m⟨ζk′,ζk⟩H‾=∑k=1m⟨ζk′,ζk⟩H‾=⟨ζ′,ζ⟩Hm‾.\langle\zeta,\zeta'\rangle_{H^{m}}=\sum_{k=1}^{m}\overline{\langle\zeta'_{k},\zeta_{k}\rangle_{H}}=\overline{\sum_{k=1}^{m}\langle\zeta'_{k},\zeta_{k}\rangle_{H}}=\overline{\langle\zeta',\zeta\rangle_{H^{m}}}.

By conditions 2 and 3 of Complex Inner Product Space for HH and claims 2 and 3 of Properties of Finite Sums,

⟨ζ,ζ′+ζ′′⟩Hm=∑k=1m(⟨ζk,ζk′⟩H+⟨ζk,ζk′′⟩H)=⟨ζ,ζ′⟩Hm+⟨ζ,ζ′′⟩Hm,⟨ζ,λζ′⟩Hm=∑k=1mλ⟨ζk,ζk′⟩H=λ⟨ζ,ζ′⟩Hm.\langle\zeta,\zeta'+\zeta''\rangle_{H^{m}}=\sum_{k=1}^{m}\bigl(\langle\zeta_{k},\zeta'_{k}\rangle_{H}+\langle\zeta_{k},\zeta''_{k}\rangle_{H}\bigr)=\langle\zeta,\zeta'\rangle_{H^{m}}+\langle\zeta,\zeta''\rangle_{H^{m}},\qquad\langle\zeta,\lambda\zeta'\rangle_{H^{m}}=\sum_{k=1}^{m}\lambda\langle\zeta_{k},\zeta'_{k}\rangle_{H}=\lambda\langle\zeta,\zeta'\rangle_{H^{m}}.

The summands ⟨ζk,ζk⟩H=∥ζk∥H2\langle\zeta_{k},\zeta_{k}\rangle_{H}=\lVert\zeta_{k}\rVert_{H}^{2} of ⟨ζ,ζ⟩Hm\langle\zeta,\zeta\rangle_{H^{m}} are nonnegative real numbers. Since R⊆C\mathbb{R}\subseteq\mathbb{C} is closed under addition, the map σ:[m]→C\sigma:[m]\to\mathbb{C} of Finite Sum Notation in a Field, formed in C\mathbb{C} for these summands, takes real values: the set of j∈Nj\in\mathbb{N} such that j∉[m]j\notin[m] or σ(j)∈R\sigma(j)\in\mathbb{R} contains 11 and, with jj, contains S(j)S(j) (if S(j)∈[m]S(j)\in[m] then j∈[m]j\in[m] and σ(S(j))=σ(j)+∥ζS(j)∥H2\sigma(S(j))=\sigma(j)+\lVert\zeta_{S(j)}\rVert_{H}^{2}), so it is N\mathbb{N} by Principle of Induction for the Natural Numbers; by the uniqueness in Existence and Uniqueness of Iterates of a Binary Operation it is then also the map formed in R\mathbb{R}, so ⟨ζ,ζ⟩Hm\langle\zeta,\zeta\rangle_{H^{m}} is the finite sum of the ∥ζk∥H2\lVert\zeta_{k}\rVert_{H}^{2} in R\mathbb{R}. By claim 5 of Properties of Finite Sums it is nonnegative, and if it is 00 then ∥ζk∥H2=0\lVert\zeta_{k}\rVert_{H}^{2}=0 for every k∈[m]k\in[m], so ζk=0\zeta_{k}=0 by claim 4 of Elementary Properties of a Complex Inner Product, that is, ζ=0\zeta=0. Hence ⟨⋅,⋅⟩Hm\langle\cdot,\cdot\rangle_{H^{m}} is an inner product, and by Norm Induced by a Complex Inner Product

∥ζ∥Hm2=⟨ζ,ζ⟩Hm=∑k=1m∥ζk∥H2.\lVert\zeta\rVert_{H^{m}}^{2}=\langle\zeta,\zeta\rangle_{H^{m}}=\sum_{k=1}^{m}\lVert\zeta_{k}\rVert_{H}^{2}.

Consequently, by claim 6 of Properties of Finite Sums and claim 2 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field,

∥ζk∥H≤∥ζ∥Hmfor all ζ∈Hm and k∈[m].(1.1)\lVert\zeta_{k}\rVert_{H}\le\lVert\zeta\rVert_{H^{m}}\qquad\text{for all }\zeta\in H^{m}\text{ and }k\in[m].\tag{1.1}

Completeness. Let (ζ(n))n∈N(\zeta^{(n)})_{n\in\mathbb{N}} be a Cauchy sequence in HmH^{m} and let k∈[m]k\in[m]. The kk-th component of ζ(n)−ζ(p)\zeta^{(n)}-\zeta^{(p)} is ζk(n)−ζk(p)\zeta^{(n)}_{k}-\zeta^{(p)}_{k}, so by (1.1) ∥ζk(n)−ζk(p)∥H≤∥ζ(n)−ζ(p)∥Hm\lVert\zeta^{(n)}_{k}-\zeta^{(p)}_{k}\rVert_{H}\le\lVert\zeta^{(n)}-\zeta^{(p)}\rVert_{H^{m}} for all n,p∈Nn,p\in\mathbb{N}, and (ζk(n))n∈N(\zeta^{(n)}_{k})_{n\in\mathbb{N}} is a Cauchy sequence in HH. Since HH is a complex Hilbert space, it is complete, so this sequence converges to some ζk∈H\zeta_{k}\in H, which is unique by Uniqueness of Limits in a Metric Space. Let ζ=(ζ1,…,ζm)∈Hm\zeta=(\zeta_{1},\dots,\zeta_{m})\in H^{m}.

Let ε>0\varepsilon>0 and put δ=ε/(4m)\delta=\varepsilon/(4m). First choose N∈NN\in\mathbb{N} with ∥ζ(n)−ζ(p)∥Hm<δ\lVert\zeta^{(n)}-\zeta^{(p)}\rVert_{H^{m}}<\delta for all n,p≥Nn,p\ge N. Let n≥Nn\ge N and k∈[m]k\in[m]. Next choose Nk∈NN_{k}\in\mathbb{N} with ∥ζk(p)−ζk∥H<δ\lVert\zeta^{(p)}_{k}-\zeta_{k}\rVert_{H}<\delta for all p≥Nkp\ge N_{k}, and let pp be the larger of NN and NkN_{k} (claim 3 of Properties of the Order on the Natural Numbers). By the triangle inequality (claim 2 of The Induced Norm is a Norm, and Induces a Metric) and (1.1),

∥ζk(n)−ζk∥H≤∥ζk(n)−ζk(p)∥H+∥ζk(p)−ζk∥H<2δ,\lVert\zeta^{(n)}_{k}-\zeta_{k}\rVert_{H}\le\lVert\zeta^{(n)}_{k}-\zeta^{(p)}_{k}\rVert_{H}+\lVert\zeta^{(p)}_{k}-\zeta_{k}\rVert_{H}<2\delta,

so ∥ζk(n)−ζk∥H2<4δ2\lVert\zeta^{(n)}_{k}-\zeta_{k}\rVert_{H}^{2}<4\delta^{2} by claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. The kk-th component of ζ(n)−ζ\zeta^{(n)}-\zeta is ζk(n)−ζk\zeta^{(n)}_{k}-\zeta_{k}; by the norm formula, claims 2, 3 and 5 of Properties of Finite Sums (applied to the nonnegative differences 4δ2−∥ζk(n)−ζk∥H24\delta^{2}-\lVert\zeta^{(n)}_{k}-\zeta_{k}\rVert_{H}^{2}) and the recursion in claim 1 of that lemma (which gives ∑k=1m4δ2=4mδ2\sum_{k=1}^{m}4\delta^{2}=4m\delta^{2}),

∥ζ(n)−ζ∥Hm2=∑k=1m∥ζk(n)−ζk∥H2≤4mδ2=ε24m<ε2,\lVert\zeta^{(n)}-\zeta\rVert_{H^{m}}^{2}=\sum_{k=1}^{m}\lVert\zeta^{(n)}_{k}-\zeta_{k}\rVert_{H}^{2}\le4m\delta^{2}=\frac{\varepsilon^{2}}{4m}<\varepsilon^{2},

so ∥ζ(n)−ζ∥Hm<ε\lVert\zeta^{(n)}-\zeta\rVert_{H^{m}}<\varepsilon by claim 1 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field. As n≥Nn\ge N was arbitrary, (ζ(n))(\zeta^{(n)}) converges to ζ\zeta. Hence HmH^{m} is complete, and it is a complex Hilbert space.

Two remarks. From now on we use the following facts. (R1) For a map j↦ξ(j)j\mapsto\xi^{(j)} from [n][n] to HmH^{m} and k∈[m]k\in[m], the kk-th component of ∑j=1nξ(j)\sum_{j=1}^{n}\xi^{(j)} is ∑j=1nξk(j)\sum_{j=1}^{n}\xi^{(j)}_{k}, by claim 4 of Properties of Finite Sums of Vectors applied to the linear map πk\pi_{k}. (R2) Let V,W,UV,W,U be among HH and HmH^{m}. For fixed v∈Vv\in V the map R↦RvR\mapsto Rv from L(V,W)\mathcal{L}(V,W) to WW is linear, because sums and scalar multiples in L(V,W)\mathcal{L}(V,W) are formed pointwise; and for fixed P∈L(W,U)P\in\mathcal{L}(W,U) and P′∈L(U,V)P'\in\mathcal{L}(U,V) the maps R↦PRR\mapsto PR and R↦RP′R\mapsto RP' are linear, because composition distributes over sums and commutes with scalar multiples (Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations). So, by claim 4 of Properties of Finite Sums of Vectors, finite sums in L(V,W)\mathcal{L}(V,W) may be evaluated termwise at vv and composed termwise with PP and P′P'.

2. (Coordinate inclusions) Let k,l∈[m]k,l\in[m]. For v,w∈Hv,w\in H and λ∈C\lambda\in\mathbb{C}, the tuples ιk(v+λw)\iota_{k}(v+\lambda w) and ιkv+λιkw\iota_{k}v+\lambda\iota_{k}w both have kk-th component v+λwv+\lambda w and all other components 00, so ιk\iota_{k} is linear. By the norm formula of claim 1 and claim 7 of Properties of Finite Sums (the summands with index j≠kj\ne k are ∥0∥H2=0\lVert0\rVert_{H}^{2}=0), ∥ιkv∥Hm2=∥v∥H2\lVert\iota_{k}v\rVert_{H^{m}}^{2}=\lVert v\rVert_{H}^{2}, so ∥ιkv∥Hm=∥v∥H\lVert\iota_{k}v\rVert_{H^{m}}=\lVert v\rVert_{H} by claim 3 of Monotonicity of Squaring on the Nonnegative Elements of an Ordered Field and 11 is a bound for ιk\iota_{k}; thus ιk∈L(H,Hm)\iota_{k}\in\mathcal{L}(H,H^{m}).

For ζ∈Hm\zeta\in H^{m} and v∈Hv\in H, claim 3 of Elementary Properties of a Complex Inner Product makes the summands with index j≠kj\ne k of ⟨ζ,ιkv⟩Hm\langle\zeta,\iota_{k}v\rangle_{H^{m}} equal to ⟨ζj,0⟩H=0\langle\zeta_{j},0\rangle_{H}=0, so by claim 7 of Properties of Finite Sums

⟨ζ,ιkv⟩Hm=⟨ζk,v⟩H=⟨πkζ,v⟩H.\langle\zeta,\iota_{k}v\rangle_{H^{m}}=\langle\zeta_{k},v\rangle_{H}=\langle\pi_{k}\zeta,v\rangle_{H}.

Thus the linear map πk\pi_{k} is an adjoint of ιk\iota_{k}, and by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique ιk∗=πk\iota_{k}^{*}=\pi_{k}, that is, ιk∗ζ=ζk\iota_{k}^{*}\zeta=\zeta_{k}; also ιk∗∈L(Hm,H)\iota_{k}^{*}\in\mathcal{L}(H^{m},H) by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint, as HH is a complex Hilbert space. Hence ιk∗ιlv=(ιlv)k\iota_{k}^{*}\iota_{l}v=(\iota_{l}v)_{k} is vv if k=lk=l and 00 if k≠lk\ne l, so ιk∗ιl=IH\iota_{k}^{*}\iota_{l}=I_{H} if k=lk=l and ιk∗ιl=0\iota_{k}^{*}\iota_{l}=0 if k≠lk\ne l. Finally let ζ∈Hm\zeta\in H^{m} and j∈[m]j\in[m]. By (R2) and (R1), the jj-th component of (∑k=1mιkιk∗)ζ=∑k=1mιkζk\bigl(\sum_{k=1}^{m}\iota_{k}\iota_{k}^{*}\bigr)\zeta=\sum_{k=1}^{m}\iota_{k}\zeta_{k} is ∑k=1m(ιkζk)j\sum_{k=1}^{m}(\iota_{k}\zeta_{k})_{j}, whose summands with k≠jk\ne j are 00; by claim 7 of Properties of Finite Sums of Vectors it equals ζj\zeta_{j}. Hence ∑k=1mιkιk∗=IHm\sum_{k=1}^{m}\iota_{k}\iota_{k}^{*}=I_{H^{m}}.

3. (Block entries) By claim 1, HmH^{m} is a complex Hilbert space, so every T∈L(Hm)T\in\mathcal{L}(H^{m}) has an adjoint T∗∈L(Hm)T^{*}\in\mathcal{L}(H^{m}) by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint; and Tkl=ιk∗Tιl∈L(H)T_{kl}=\iota_{k}^{*}T\iota_{l}\in\mathcal{L}(H) by claim 2 and Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations. Let S,T∈L(Hm)S,T\in\mathcal{L}(H^{m}), ζ,ζ′∈Hm\zeta,\zeta'\in H^{m} and k,l∈[m]k,l\in[m].

Components. By claim 2 and (R2),

(Tζ)k=ιk∗T(∑j=1mιjιj∗)ζ=∑j=1mιk∗Tιjιj∗ζ=∑j=1mTkjζj.(T\zeta)_{k}=\iota_{k}^{*}T\Bigl(\sum_{j=1}^{m}\iota_{j}\iota_{j}^{*}\Bigr)\zeta=\sum_{j=1}^{m}\iota_{k}^{*}T\iota_{j}\iota_{j}^{*}\zeta=\sum_{j=1}^{m}T_{kj}\zeta_{j}.

Inner products. By the definition of ⟨⋅,⋅⟩Hm\langle\cdot,\cdot\rangle_{H^{m}}, the formula just proved and claim 5 of Properties of Finite Sums of Vectors,

⟨ζ,Tζ′⟩Hm=∑k=1m⟨ζk,∑j=1mTkjζj′⟩H=∑k=1m∑j=1m⟨ζk,Tkjζj′⟩H.\langle\zeta,T\zeta'\rangle_{H^{m}}=\sum_{k=1}^{m}\Bigl\langle\zeta_{k},\sum_{j=1}^{m}T_{kj}\zeta'_{j}\Bigr\rangle_{H}=\sum_{k=1}^{m}\sum_{j=1}^{m}\langle\zeta_{k},T_{kj}\zeta'_{j}\rangle_{H}.

Adjoints. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-calculus, ιl\iota_{l} is the adjoint of ιl∗\iota_{l}^{*}, and, applying the rule for composites twice, Tlk=ιl∗(Tιk)T_{lk}=\iota_{l}^{*}(T\iota_{k}) has the adjoint (Tιk)∗ιl=ιk∗T∗ιl(T\iota_{k})^{*}\iota_{l}=\iota_{k}^{*}T^{*}\iota_{l}. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique, (Tlk)∗=ιk∗T∗ιl=(T∗)kl(T_{lk})^{*}=\iota_{k}^{*}T^{*}\iota_{l}=(T^{*})_{kl}.

Products. By claim 2 and (R2),

(ST)kl=ιk∗S(∑j=1mιjιj∗)Tιl=∑j=1m(ιk∗Sιj)(ιj∗Tιl)=∑j=1mSkjTjl.(ST)_{kl}=\iota_{k}^{*}S\Bigl(\sum_{j=1}^{m}\iota_{j}\iota_{j}^{*}\Bigr)T\iota_{l}=\sum_{j=1}^{m}(\iota_{k}^{*}S\iota_{j})(\iota_{j}^{*}T\iota_{l})=\sum_{j=1}^{m}S_{kj}T_{jl}.

Converse. Let (Akl)k,l∈[m](A_{kl})_{k,l\in[m]} be a family in L(H)\mathcal{L}(H) and T=∑k=1m∑l=1mιkAklιl∗T=\sum_{k=1}^{m}\sum_{l=1}^{m}\iota_{k}A_{kl}\iota_{l}^{*}, an element of the complex vector space L(Hm)\mathcal{L}(H^{m}) by Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations. Let p,q∈[m]p,q\in[m]. By (R2), Tpq=∑k=1m∑l=1mιp∗ιkAklιl∗ιqT_{pq}=\sum_{k=1}^{m}\sum_{l=1}^{m}\iota_{p}^{*}\iota_{k}A_{kl}\iota_{l}^{*}\iota_{q}. For fixed kk, the summands with l≠ql\ne q vanish since ιl∗ιq=0\iota_{l}^{*}\iota_{q}=0 by claim 2, so by claim 7 of Properties of Finite Sums of Vectors the inner sum is ιp∗ιkAkq\iota_{p}^{*}\iota_{k}A_{kq}; in the same way, since ιp∗ιk=0\iota_{p}^{*}\iota_{k}=0 for k≠pk\ne p and ιp∗ιp=IH\iota_{p}^{*}\iota_{p}=I_{H}, the outer sum is ApqA_{pq}. So Tpq=ApqT_{pq}=A_{pq}. If also T′∈L(Hm)T'\in\mathcal{L}(H^{m}) satisfies Tkl′=AklT'_{kl}=A_{kl} for all k,l∈[m]k,l\in[m], then by the component formula (T′ζ)k=∑j=1mAkjζj=(Tζ)k(T'\zeta)_{k}=\sum_{j=1}^{m}A_{kj}\zeta_{j}=(T\zeta)_{k} for all ζ∈Hm\zeta\in H^{m} and k∈[m]k\in[m], so T′=TT'=T.

4. (Diagonal operators) Let A∈L(H)A\in\mathcal{L}(H), ζ∈Hm\zeta\in H^{m} and j∈[m]j\in[m]. By (R2), (R1) and claim 2, the jj-th component of (∑k=1mιkAιk∗)ζ\bigl(\sum_{k=1}^{m}\iota_{k}A\iota_{k}^{*}\bigr)\zeta is ∑k=1m(ιkAζk)j\sum_{k=1}^{m}(\iota_{k}A\zeta_{k})_{j}, whose summands with k≠jk\ne j are 00, so by claim 7 of Properties of Finite Sums of Vectors it equals Aζj=(A(m)ζ)jA\zeta_{j}=(A^{(m)}\zeta)_{j}. Hence

A(m)=∑k=1mιkAιk∗,A^{(m)}=\sum_{k=1}^{m}\iota_{k}A\iota_{k}^{*},

which lies in L(Hm)\mathcal{L}(H^{m}) by claim 2 and Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §operations. Let Dkl=AD_{kl}=A if k=lk=l and Dkl=0D_{kl}=0 if k≠lk\ne l. For fixed kk the summands ιkDklιl∗\iota_{k}D_{kl}\iota_{l}^{*} with l≠kl\ne k are 00, so by claim 7 of Properties of Finite Sums of Vectors ∑k=1m∑l=1mιkDklιl∗=A(m)\sum_{k=1}^{m}\sum_{l=1}^{m}\iota_{k}D_{kl}\iota_{l}^{*}=A^{(m)}, and the converse part of claim 3 gives (A(m))kl=Dkl(A^{(m)})_{kl}=D_{kl} for all k,l∈[m]k,l\in[m].

Adjoint. By Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint, A∗∈L(H)A^{*}\in\mathcal{L}(H), so by what was just shown (A∗)(m)∈L(Hm)(A^{*})^{(m)}\in\mathcal{L}(H^{m}) has the entry A∗A^{*} at (k,k)(k,k) and 00 at (k,l)(k,l) with k≠lk\ne l. The zero map is its own adjoint, since ⟨0w,v⟩=0=⟨w,0v⟩\langle0w,v\rangle=0=\langle w,0v\rangle by claim 3 of Elementary Properties of a Complex Inner Product, so by the adjoint formula of claim 3 and Bounded Linear Maps between Complex Inner Product Spaces: the Least Bound, Operations, the Underlying Real Structure, Adjoints, Completeness and the Quadratic-Form Bound §adjoint-unique, ((A(m))∗)kl=((A(m))lk)∗((A^{(m)})^{*})_{kl}=((A^{(m)})_{lk})^{*} is A∗A^{*} if k=lk=l and 00 if k≠lk\ne l. By the uniqueness in the converse part of claim 3, (A(m))∗=(A∗)(m)(A^{(m)})^{*}=(A^{*})^{(m)}.

Commutation. Let T∈L(Hm)T\in\mathcal{L}(H^{m}) and k,l∈[m]k,l\in[m]. By the product formula of claim 3, (TA(m))kl=∑j=1mTkj(A(m))jl(TA^{(m)})_{kl}=\sum_{j=1}^{m}T_{kj}(A^{(m)})_{jl} and (A(m)T)kl=∑j=1m(A(m))kjTjl(A^{(m)}T)_{kl}=\sum_{j=1}^{m}(A^{(m)})_{kj}T_{jl}; the summands with j≠lj\ne l, respectively j≠kj\ne k, are composites with the zero map and hence 00, so by claim 7 of Properties of Finite Sums of Vectors

(TA(m))kl=TklA,(A(m)T)kl=ATkl.(TA^{(m)})_{kl}=T_{kl}A,\qquad(A^{(m)}T)_{kl}=AT_{kl}.

If TA(m)=A(m)TTA^{(m)}=A^{(m)}T, then these entries agree, so TklT_{kl} commutes with AA for all k,l∈[m]k,l\in[m]. Conversely, if TklA=ATklT_{kl}A=AT_{kl} for all k,l∈[m]k,l\in[m], then TA(m)TA^{(m)} and A(m)TA^{(m)}T have the same entries and are equal by the uniqueness in the converse part of claim 3.

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