Original text: CC0 1.0. Prerequisite proofs and component terms.

Finite domains, null directions, and support corners

OA-MOD-WS-01 — Conventions and exact inputs

Let M⊆B(H)M\subseteq B(H) be a concrete unital von Neumann algebra on any Hilbert space. Use the definitions of a weight φ\varphi, its finite cone FφF_\varphi, its finite left ideal nφ\mathfrak n_\varphi, its definition algebra mφ\mathfrak m_\varphi, and its null left ideal NφN_\varphi from OA-MOD-WG-002 through OA-MOD-WG-005. Inner products are linear in the first variable.

OA-MOD-WS-02 and OA-MOD-WS-03 allow an arbitrary weight. All later weight assertions explicitly assume normality, in the sense of preservation of bounded increasing positive suprema.

The proofs use the finite-domain algebra from WG-003, bounded inverse order, monotone nets, support cutoffs and topology facts from OA-MOD-BK-03 through OA-MOD-BK-06, and the finite-cutoff characterization of semifiniteness from WG-008. These are bounded-operator and Hilbert prerequisites; no modular theorem or spatial derivative is used.

For clarity, the concrete sigma-strong topology is given by the seminorms x⟼(∑n≥1∥xξn∥2)1/2,∑n∥ξn∥2<∞. x\longmapsto\left(\sum_{n\geq1}\|x\xi_n\|^2\right)^{1/2}, \qquad \sum_n\|\xi_n\|^2<\infty. A norm-bounded strongly convergent net converges in this topology: make the tail uniformly small by the common norm bound, and use strong convergence for the remaining finitely many vectors. This does not assume that HH has a countable basis. We use the corresponding square-summable vector-pair definition of the ultraweak topology from BK-03.

OA-MOD-WS-02 — The projection of the finite domain

Theorem. For every weight φ\varphi, there is a unique projection e∈Me\in M such that nφ‾ SOT=nφ‾ σ-strong=nφ‾ ultraweak=Me. \overline{\mathfrak n_\varphi}^{\,\mathrm{SOT}} =\overline{\mathfrak n_\varphi}^{\,\sigma\text{-strong}} =\overline{\mathfrak n_\varphi}^{\,\mathrm{ultraweak}} =M e. Moreover, mφ‾ SOT=mφ‾ σ-strong=mφ‾ ultraweak=eMe. \overline{\mathfrak m_\varphi}^{\,\mathrm{SOT}} =\overline{\mathfrak m_\varphi}^{\,\sigma\text{-strong}} =\overline{\mathfrak m_\varphi}^{\,\mathrm{ultraweak}} =eMe. The closures are taken inside MM. Every a∈Fφa\in F_\varphi satisfies a=eaea=eae. In particular, φ\varphi is semifinite if and only if e=1e=1.

Proof. Direct FφF_\varphi by its positive order; addition gives a common upper bound. For each a∈Fφa\in F_\varphi, put ua=a(1+a)−1. u_a=a(1+a)^{-1}. As in WG-008, these are increasing finite positive contractions. Let e∈Me\in M be their strong supremum. At this stage ee is only known to be a positive contraction.

Fix a∈Fφa\in F_\varphi. All tat a, t>0t>0, are indices, and the bounded support-cutoff theorem gives uta↑s(a). u_{ta}\uparrow s(a). Thus e≥s(a)e\geq s(a). A positive contraction dominating a projection acts as the identity on its range: if q≤e≤1q\leq e\leq1, then q(1−e)q=0,(1−e)1/2q=0, q(1-e)q=0,\qquad (1-e)^{1/2}q=0, so eq=qeq=q.

Let KK be the closed linear span of the ranges of all a∈Fφa\in F_\varphi. The preceding observation shows that ee is the identity on KK. Every uau_a vanishes on K⊥K^\perp, and therefore its strong limit ee does as well. Hence e=PKe=P_K is a projection. It follows that a=eaea=eae for every finite positive aa.

If x∈nφx\in\mathfrak n_\varphi, then x∗x∈Fφx^*x\in F_\varphi, and ∥x(1−e)ξ∥2=⟨x∗x(1−e)ξ,(1−e)ξ⟩=0. \|x(1-e)\xi\|^2 =\langle x^*x(1-e)\xi,(1-e)\xi\rangle=0. Thus x=xex=xe. Conversely, if x=xex=xe, then ua∈nφu_a\in\mathfrak n_\varphi, since ua2≤uau_a^2\leq u_a and its weight is finite. The left-ideal property gives xua∈nφx u_a\in\mathfrak n_\varphi. These operators are norm bounded and converge strongly to xe=xxe=x, hence sigma-strongly and ultraweakly as well.

The set Me={x∈M:x=xe}Me=\{x\in M:x=xe\} is closed in each stated topology: fixed right multiplication is continuous in each, and the defining equality is closed. This proves the three left-ideal closure identities. Uniqueness also follows: Me=Me′Me=Me' for projections implies e=ee′e=ee' and e′=e′ee'=e'e, and taking adjoints yields both projection inequalities.

Since mφ=span⁡CFφ\mathfrak m_\varphi=\operatorname{span}_{\mathbb C}F_\varphi, it lies in eMeeMe. For x∈eMex\in eMe, uaxua=ua∗(xua)∈mφ. u_a x u_a=u_a^*(x u_a)\in\mathfrak m_\varphi. Both factors in the last product belong to nφ\mathfrak n_\varphi. The operators uaxuau_a x u_a are norm bounded and converge strongly to exe=xexe=x. The same topology arguments prove all three definition-algebra closure identities. Semifiniteness, defined by ultraweak density of mφ\mathfrak m_\varphi, is consequently equivalent to eMe=MeMe=M, or e=1e=1. □\square

The projection ee need not be central. The proof does not turn the finite left ideal into a two-sided ideal.

OA-MOD-WS-03 — A semifinite restriction exists before normality

Proposition. With ee as above, the restriction of φ\varphi to (eMe)+(eMe)_+ is a semifinite weight. If φ\varphi is normal, so is this restriction. For a∈M+a\in M_+, a≠eae⟹φ(a)=+∞. a\ne eae\quad\Longrightarrow\quad\varphi(a)=+\infty.

Proof. Every finite positive element of MM belongs to eMeeMe, by WS-02. Hence the finite cone of the restricted weight is exactly FφF_\varphi, now viewed inside the corner. Its complex span is ultraweakly dense in eMeeMe, again by WS-02. This is precisely semifiniteness of the restriction. Increasing positive suprema in the corner agree with those in MM, so normality is inherited. Finally, if φ(a)<∞\varphi(a)<\infty, then a∈Fφa\in F_\varphi and a=eaea=eae; taking the contrapositive gives the assertion. □\square

The implication is about all finite elements. It does not say that every positive element of eMeeMe has finite weight.

OA-MOD-WS-04 — Normality produces a largest null projection

Assume from now on that φ\varphi is normal.

Theorem. There is a largest projection f∈Mf\in M with φ(f)=0\varphi(f)=0. It satisfies f≤ef\leq e, and Nφ=Mf. N_\varphi=M f. For a∈M+a\in M_+, the following are equivalent: φ(a)=0,s(a)≤f,a=faf. \varphi(a)=0,\qquad s(a)\leq f,\qquad a=faf.

Proof. If a≥0a\geq0 and φ(a)=0\varphi(a)=0, its cutoff vt=ta(1+ta)−1 v_t=t a(1+t a)^{-1} satisfies 0≤vt≤ta0\leq v_t\leq t a, and hence φ(vt)=0\varphi(v_t)=0. The cutoffs increase to s(a)s(a). Normality yields φ(s(a))=0\varphi(s(a))=0.

If projections q1,q2q_1,q_2 have weight zero, then q1+q2q_1+q_2 has weight zero, so s(q1+q2)s(q_1+q_2) does also. This support is their join: its kernel is ker⁡q1∩ker⁡q2\ker q_1\cap\ker q_2, as follows from ⟨(q1+q2)ξ,ξ⟩=∥q1ξ∥2+∥q2ξ∥2. \langle(q_1+q_2)\xi,\xi\rangle =\|q_1\xi\|^2+\|q_2\xi\|^2. Therefore finite joins of null projections are null. Their increasing net has a strong supremum f∈Mf\in M. A bounded strong limit of increasing projections is a projection: it fixes the range of every net member and vanishes on the orthogonal complement of the closed union of their ranges. Normality gives φ(f)=0\varphi(f)=0. By construction every null projection lies below ff, so it is the largest one.

If φ(a)=0\varphi(a)=0, the first paragraph gives s(a)≤fs(a)\leq f, or equivalently a=fafa=faf. Conversely, a=faf≥0a=faf\geq0 implies a≤∥a∥fa\leq\|a\|f, hence φ(a)=0\varphi(a)=0. This proves the positive-cone assertions. Since ff itself is finite, WS-02 gives f=efef=efe, so f≤ef\leq e.

If x∈Nφx\in N_\varphi, apply the positive-cone assertion to x∗xx^*x. It gives x(1−f)=0x(1-f)=0, or x=xfx=xf. Conversely, x=xfx=xf implies x∗x≤∥x∥2fx^*x\leq\|x\|^2f, so x∈Nφx\in N_\varphi. Hence Nφ=MfN_\varphi=Mf. □\square

The resulting null ideal is ultraweakly and strongly closed. Normality is essential to this conclusion; WS-08 contains a nonnormal counterexample.

OA-MOD-WS-05 — Removing null directions without subtracting infinities

Put r=1−fr=1-f.

Theorem. For every a∈M+a\in M_+, φ(a)=φ(rar). \varphi(a)=\varphi(rar). The restriction of φ\varphi to rMrrMr is faithful and normal. It is not automatically semifinite.

Proof. We first record an inequality that remains valid for infinite energies. For arbitrary x,y∈Mx,y\in M and ε>0\varepsilon>0, (x+y)∗(x+y)≤(1+ε)x∗x+(1+ε−1)y∗y. (x+y)^*(x+y) \leq(1+\varepsilon)x^*x+(1+\varepsilon^{-1})y^*y. It follows by expanding the positivity of (ε1/2x−ε−1/2y)∗(ε1/2x−ε−1/2y)(\varepsilon^{1/2}x-\varepsilon^{-1/2}y)^* (\varepsilon^{1/2}x-\varepsilon^{-1/2}y). If y∈Nφy\in N_\varphi, monotonicity and additivity imply φ((x+y)∗(x+y))≤(1+ε)φ(x∗x). \varphi((x+y)^*(x+y)) \leq(1+\varepsilon)\varphi(x^*x). Applying the same inequality to x=(x+y)−yx=(x+y)-y gives the reverse comparison with the same factor. If either weight is infinite, the comparisons force both to be infinite. If they are finite, letting ε\varepsilon decrease to zero proves equality. No difference of infinite numbers is taken.

For a positive aa, choose x=a1/2rx=a^{1/2}r and y=a1/2fy=a^{1/2}f. Since y∈Mf=Nφy\in Mf=N_\varphi, the preceding equality gives φ(a)=φ((x+y)∗(x+y))=φ(x∗x)=φ(rar). \varphi(a)=\varphi((x+y)^*(x+y)) =\varphi(x^*x)=\varphi(rar).

If a∈(rMr)+a\in(rMr)_+ has weight zero, WS-04 gives a=fafa=faf. Because also a=rara=rar and fr=0fr=0, we obtain a=0a=0. This is faithfulness. Normality is inherited under restriction. No semifiniteness conclusion follows solely from removing the null ideal; the everywhere-infinite example in WS-08 has r=1r=1 and is not semifinite. □\square

We call rr the null-carrier projection to keep it distinct from the support convention in the next statement.

OA-MOD-WS-06 — The faithful semifinite support corner

Theorem. Let φ\varphi be a normal weight, let e,fe,f be the projections constructed above, and put p=e−f. p=e-f. Then pp is a projection, and the restriction φp\varphi_p to pMppMp is normal, semifinite and faithful. On all of M+M_+, the exact reconstruction rule is φ(a)={φp(pap),a=eae,+∞,a≠eae. \varphi(a)= \begin{cases} \varphi_p(pap),&a=eae,\\ +\infty,&a\ne eae. \end{cases} For a normal semifinite weight, e=1e=1, so p=1−fp=1-f and φ(a)=φp(pap)(a∈M+). \varphi(a)=\varphi_p(pap)\qquad(a\in M_+).

Proof. We know f≤ef\leq e, hence p=e−f=e(1−f)=(1−f)ep=e-f=e(1-f)=(1-f)e is a projection. It lies under r=1−fr=1-f, so the restriction is faithful by WS-05 and normal by restriction.

Use the increasing finite positive contractions uau_a from WS-02. The compressions puapp u_a p increase strongly to pp, are positive contractions in the corner, and have finite weight. Indeed, ua=euaeu_a=e u_a e, so puap=ruar,φ(puap)=φ(ua)<∞ p u_a p=r u_a r,\qquad \varphi(pu_ap)=\varphi(u_a)<\infty by WS-05. WG-008 applied inside pMppMp, whose identity is pp, proves semifiniteness. This argument also covers the zero corner.

For a=eaea=eae, one has rar=paprar=pap, so WS-05 gives the finite-corner formula, whether its value is finite or infinite. For a≠eaea\ne eae, WS-03 gives the other line. Finally, semifiniteness is equivalent to e=1e=1, by WS-02. □\square

We use support of the normal weight for p=e−fp=e-f when following the stated Takesaki convention. If a discussion instead defines support as the complement of the maximal null projection, its projection is rr. The convention must be checked before treating results about arbitrary normal weights as identical. For the normal semifinite numerator in spatial derivative theory, the two conventions agree and WS-06 supplies the required support-corner reduction.

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