TheoremBase

Proof

Preliminaries. (P1) For every clock label aa, every jj, and 0≤t≤t′≤T0\le t\le t'\le T: 0≤Aja(t′)−Aja(t)≤Ba(t′−t)0\le A_j^{a}(t')-A_j^{a}(t)\le B_a(t'-t). Indeed, by condition 2 of Solution of the Controlled N-Agent Dynamics the consumed time Aja(t)A_j^{a}(t) is the Lebesgue integral over the compact interval [0,t][0,t] of an integrand with values in [0,Ba][0,B_a], and the increment over (t,t′](t,t'] is the integral of that integrand over the complementary piece by additivity of the integral over disjoint measurable sets, hence lies in [0,Ba(t′−t)][0,B_a(t'-t)] by monotonicity. In particular Aja(t)≤Bat≤BaTA_j^{a}(t)\le B_at\le B_aT, and the frontier A∨,aA^{\vee,a} is nondecreasing with At′∨,a≤At∨,a+Ba(t′−t)A^{\vee,a}_{t'}\le A^{\vee,a}_t+B_a(t'-t), the bound passing through the finite maximum. (P2) Each Aja(t)A_j^{a}(t) is Ftsys,j\mathcal{F}^{\mathrm{sys},j}_t-measurable by part (iv) of Existence, Uniqueness, and Regularity for the Controlled N-Agent Dynamics, so At∨,aA^{\vee,a}_t is Ft\mathbb{F}_t-measurable; evaluations of the clock paths at random levels are random variables by claim 1 of Predictable-Window Moment Identities for the Homogeneous Poisson Process. Also Fs⊆Fw\mathbb{F}_s\subseteq\mathbb{F}_w for s≤ws\le w, each (Ftsys,j)t(\mathcal{F}^{\mathrm{sys},j}_t)_t being a filtration. (P3) It suffices to prove the claims for bounded ZZ: for Z:Ω→[0,∞]Z:\Omega\to[0,\infty] apply the bounded case to Z∧nZ\wedge n and let n→∞n\to\infty by the Monotone Convergence Theorem.

Claim 1. Fix tt, the label aa, pp, and ZZ with 0≤Z≤ζ0\le Z\le\zeta; fix a natural mm and put δ=2−m\delta=2^{-m}, θq=qδ\theta_q=q\delta. Let QQ be the least natural with θQ≥Vˉ\theta_Q\ge\bar{V} and partition Ω\Omega into F0={v=0}F_0=\{v=0\} and Fq={θq−1<v≤θq}F_q=\{\theta_{q-1}<v\le\theta_q\} for q=1,…,Qq=1,\dots,Q (using 0≤v≤Vˉ0\le v\le\bar{V}). Fix qq and write θ\theta for θq\theta_q, with θ=0\theta=0 when q=0q=0.

Apply Level-Revealed Conditioning for Jointly Driven Solutions of the Controlled N-Agent Dynamics at time r:=tr:=t with caps ca:=θc_a:=\theta for the label aa and cb:=Bbtc_b:=B_bt for every label b≠ab\neq a. By (P1) the constraints for the labels b≠ab\neq a hold surely, so the event CC there equals ⋂j{Aja(t)≤θ}\bigcap_j\{A_j^{a}(t)\le\theta\}, and Fq⊆CF_q\subseteq C because Aja(t)≤At∨,a≤v≤θA_j^{a}(t)\le A^{\vee,a}_t\le v\le\theta on FqF_q. Its claim 1 gives C^∈Hq\hat{C}\in\mathcal{H}_q (the capped σ\sigma-algebra there) with P(C△C^)=0P(C\triangle\hat{C})=0, and its claim 2, applied to the Ft\mathbb{F}_t-measurable nonnegative maps Wq:=Z1FqW_q:=Z\mathbf{1}_{F_q}, vv, and λ\lambda, gives Hq\mathcal{H}_q-measurable W^q,v^q,λ^q\hat{W}_q,\hat{v}_q,\hat{\lambda}_q agreeing with them almost surely on CC. Set λq:=(v+λ−θ)+\lambda_q:=(v+\lambda-\theta)^{+} and λq†:=(((v^q∧Vˉ)+(λ^q∧Λˉ)−θ)+)∧Λˉ\lambda^{\dagger}_q:=\bigl(((\hat{v}_q\wedge\bar{V})+(\hat{\lambda}_q\wedge\bar{\Lambda})-\theta)^{+}\bigr)\wedge\bar{\Lambda}, an Hq\mathcal{H}_q-measurable variable with values in [0,Λˉ][0,\bar{\Lambda}].

Pathwise split. On FqF_q, with I:=Yv+λa−YvaI:=Y^{a}_{v+\lambda}-Y^{a}_{v}, Dq:=Y(v+λ)∧θa−YvaD_q:=Y^{a}_{(v+\lambda)\wedge\theta}-Y^{a}_{v}, and Gq:=Yθ+λqa−YθaG_q:=Y^{a}_{\theta+\lambda_q}-Y^{a}_{\theta}: if v+λ≥θv+\lambda\ge\theta then (v+λ)∧θ=θ(v+\lambda)\wedge\theta=\theta, θ+λq=v+λ\theta+\lambda_q=v+\lambda, and I=Dq+GqI=D_q+G_q by concatenation at the level θ\theta; if v+λ<θv+\lambda<\theta then λq=0\lambda_q=0, Gq=0G_q=0, Dq=ID_q=I. In all cases I=Dq+GqI=D_q+G_q with Dq,Gq≥0D_q,G_q\ge0.

Central term. First, (W^q∧ζ)1C^=Wq(\hat{W}_q\wedge\zeta)\mathbf{1}_{\hat{C}}=W_q almost surely: the two agree almost surely on CC (where W^q=Wq≤ζ\hat{W}_q=W_q\le\zeta and 1C^=1\mathbf{1}_{\hat{C}}=1 almost surely), and almost surely off CC both vanish (WqW_q vanishes off FqF_q and Fq⊆CF_q\subseteq C, so Wq=0W_q=0 off CC; and 1C^=0\mathbf{1}_{\hat{C}}=0 almost surely off CC). Second, λq†=λq\lambda^{\dagger}_q=\lambda_q almost surely on Fq⊇{Wq>0}F_q\supseteq\{W_q>0\}: almost surely on Fq⊆CF_q\subseteq C one has v^q=v≤Vˉ\hat{v}_q=v\le\bar{V} and λ^q=λ≤Λˉ\hat{\lambda}_q=\lambda\le\bar{\Lambda}, so the inner truncations do not act, and on FqF_q, v≤θv\le\theta gives λq≤λ≤Λˉ\lambda_q\le\lambda\le\bar{\Lambda}, so the outer truncation does not act either. Hence the integrands of E[WqGq p]\mathbb{E}[W_qG_q^{\,p}] and E[(W^q∧ζ)1C^ (Yθ+λq†a−Yθa)p]\mathbb{E}\bigl[(\hat{W}_q\wedge\zeta)\mathbf{1}_{\hat{C}}\,(Y^{a}_{\theta+\lambda^{\dagger}_q}-Y^{a}_{\theta})^{p}\bigr] agree almost surely, and the expectations coincide. Now apply claim 2 of Predictable-Window Moment Identities for the Homogeneous Poisson Process to the clock YaY^{a} with the data: level θ\theta, bounds Vˉ′:=θ\bar{V}':=\theta and Λˉ\bar{\Lambda}; σ\sigma-algebra G:=Hq\mathcal{G}:=\mathcal{H}_q, which is independent of σ(Yθ+sa−Yθa:s≥0)\sigma(Y^{a}_{\theta+s}-Y^{a}_{\theta}:s\ge0) by claim 3 of Level-Revealed Conditioning for Jointly Driven Solutions of the Controlled N-Agent Dynamics; window bottom the constant θ\theta; window length λq†\lambda^{\dagger}_q; multiplier (W^q∧ζ)1C^(\hat{W}_q\wedge\zeta)\mathbf{1}_{\hat{C}}. This yields E[WqGq p]=E[(W^q∧ζ)1C^ μp(λq†)]=E[Wq μp(λq)]\mathbb{E}[W_qG_q^{\,p}]=\mathbb{E}\bigl[(\hat{W}_q\wedge\zeta)\mathbf{1}_{\hat{C}}\,\mu_p(\lambda^{\dagger}_q)\bigr]=\mathbb{E}[W_q\,\mu_p(\lambda_q)]: in the last step the first factors agree almost surely, and where they are positive (a subset of FqF_q up to a null event) λq†=λq\lambda^{\dagger}_q=\lambda_q almost surely, so the integrands agree almost surely.

Error term. For reals x≥y≥0x\ge y\ge0, xp−yp=(x−y)(xp−1+⋯+yp−1)≤(x−y) p xp−1x^p-y^p=(x-y)(x^{p-1}+\dots+y^{p-1})\le(x-y)\,p\,x^{p-1}; with x=Ix=I, y=Gqy=G_q, and I≤Yˉ:=YVˉ+Λˉ+1aI\le\bar{Y}:=Y^{a}_{\bar{V}+\bar{\Lambda}+1} (path monotonicity, v+λ≤Vˉ+Λˉv+\lambda\le\bar{V}+\bar{\Lambda}), this gives 0≤E[WqIp]−E[WqGq p]≤p ζ E[1FqDqYˉ p−1]0\le\mathbb{E}[W_qI^{p}]-\mathbb{E}[W_qG_q^{\,p}]\le p\,\zeta\,\mathbb{E}[\mathbf{1}_{F_q}D_q\bar{Y}^{\,p-1}].

Assembly and limit. Summing over q=0,…,Qq=0,\dots,Q (the FqF_q partition Ω\Omega) and writing θ(m)(ω)\theta_{(m)}(\omega) for the cell top δ⌈v/δ⌉\delta\lceil v/\delta\rceil, λ(m):=(v+λ−θ(m))+\lambda_{(m)}:=(v+\lambda-\theta_{(m)})^{+}, and D(m):=Y(v+λ)∧θ(m)a−YvaD_{(m)}:=Y^{a}_{(v+\lambda)\wedge\theta_{(m)}}-Y^{a}_{v}: ∣E[Z Ip]−E[Z μp(λ(m))]∣≤p ζ E[D(m)Yˉ p−1].\bigl|\mathbb{E}[Z\,I^{p}]-\mathbb{E}[Z\,\mu_p(\lambda_{(m)})]\bigr|\le p\,\zeta\,\mathbb{E}[D_{(m)}\bar{Y}^{\,p-1}]. As m→∞m\to\infty: θ(m)↓v\theta_{(m)}\downarrow v (dyadic upper approximations), so λ(m)→λ\lambda_{(m)}\to\lambda pointwise and, by continuity and monotonicity of μp\mu_p (claim 4 of Predictable-Window Moment Identities for the Homogeneous Poisson Process) and the Dominated Convergence Theorem with the constant dominator ζμp(Λˉ)\zeta\mu_p(\bar{\Lambda}), E[Zμp(λ(m))]→E[Zμp(λ)]\mathbb{E}[Z\mu_p(\lambda_{(m)})]\to\mathbb{E}[Z\mu_p(\lambda)]. Also D(m)↓0D_{(m)}\downarrow0 pointwise: the levels (v+λ)∧θ(m)(v+\lambda)\wedge\theta_{(m)} decrease to vv, and YaY^{a} at levels decreasing to vv decreases to YvaY^{a}_{v} by right-continuity (property 3 of Counting Path and Its Jump Times, as in claim 1 of Predictable-Window Moment Identities for the Homogeneous Poisson Process); with D(m)Yˉ p−1≤Yˉ pD_{(m)}\bar{Y}^{\,p-1}\le\bar{Y}^{\,p} and E[Yˉ p]=μp(Vˉ+Λˉ+1)<∞\mathbb{E}[\bar{Y}^{\,p}]=\mu_p(\bar{V}+\bar{\Lambda}+1)<\infty, dominated convergence gives E[D(m)Yˉ p−1]→0\mathbb{E}[D_{(m)}\bar{Y}^{\,p-1}]\to0. Since E[ZIp]\mathbb{E}[ZI^{p}] does not depend on mm, E[Z Ip]=E[Z μp(λ)]\mathbb{E}[Z\,I^{p}]=\mathbb{E}[Z\,\mu_p(\lambda)].

The window-event identity is proved by the same split, using ∣1{I≥1}−1{Gq≥1}∣≤Dq|\mathbf{1}\{I\ge1\}-\mathbf{1}\{G_q\ge1\}|\le D_q pointwise (if I≥1I\ge1 and Gq=0G_q=0 then Dq=I≥1D_q=I\ge1, and Gq≤IG_q\le I), the central evaluation E[Wq1{Gq≥1}]=E[Wq(1−exp⁡(−λq))]\mathbb{E}[W_q\mathbf{1}\{G_q\ge1\}]=\mathbb{E}[W_q(1-\exp(-\lambda_q))] from claim 3 of Predictable-Window Moment Identities for the Homogeneous Poisson Process with the same almost-sure-equality bookkeeping as in the central term, and, in the limit, continuity of exp⁡\exp with dominator ζ\zeta for the central part together with E[Z D(m)]→0\mathbb{E}[Z\,D_{(m)}]\to0 for the error part, by the same dominated-convergence argument with dominator Yˉ\bar{Y} and E[Yˉ]=μ1(Vˉ+Λˉ+1)<∞\mathbb{E}[\bar{Y}]=\mu_1(\bar{V}+\bar{\Lambda}+1)<\infty. The final inequality follows from the pointwise bound 1−exp⁡(−λ)≤λ1-\exp(-\lambda)\le\lambda: for λ≥1\lambda\ge1 it is trivial, and for 0≤λ<10\le\lambda<1 the defining series and the geometric partial-sum bound give exp⁡(λ)≤∑kλk≤1/(1−λ)\exp(\lambda)\le\sum_k\lambda^k\le1/(1-\lambda), so exp⁡(−λ)≥1−λ\exp(-\lambda)\ge1-\lambda. The case p=1p=1 reads E[Z(Yv+λa−Yva)]=E[Zλ]\mathbb{E}[Z(Y^{a}_{v+\lambda}-Y^{a}_{v})]=\mathbb{E}[Z\lambda] since μ1(λ)=λ\mu_1(\lambda)=\lambda.

Claim 2. Assume ZZ bounded (P3). Write A∨:=A∨,aA^{\vee}:=A^{\vee,a} and λ∗:=As∨+Ba(w−s)−Aw∨\lambda^{*}:=A^{\vee}_s+B_a(w-s)-A^{\vee}_w; by (P1), 0≤λ∗≤Ba(w−s)0\le\lambda^{*}\le B_a(w-s) and Aw∨+λ∗=As∨+Ba(w−s)A^{\vee}_w+\lambda^{*}=A^{\vee}_s+B_a(w-s). Since As∨≤Aw∨≤As∨+Ba(w−s)A^{\vee}_s\le A^{\vee}_w\le A^{\vee}_s+B_a(w-s), the increments concatenate pathwise: YAw∨a−YAs∨a=[YAs∨+Ba(w−s)a−YAs∨a]−[YAw∨+λ∗a−YAw∨a],Y^{a}_{A^{\vee}_w}-Y^{a}_{A^{\vee}_s}=\bigl[Y^{a}_{A^{\vee}_s+B_a(w-s)}-Y^{a}_{A^{\vee}_s}\bigr]-\bigl[Y^{a}_{A^{\vee}_w+\lambda^{*}}-Y^{a}_{A^{\vee}_w}\bigr], both brackets being nonnegative integers bounded by YBaT+Ba(w−s)aY^{a}_{B_aT+B_a(w-s)}, which is integrable with expectation μ1(BaT+Ba(w−s))<∞\mu_1(B_aT+B_a(w-s))<\infty. Apply claim 1 with p=1p=1 twice: at time ss, with window bottom v:=As∨v:=A^{\vee}_s (Fs\mathbb{F}_s-measurable, ≥As∨,a\ge A^{\vee,a}_s, ≤BaT=:Vˉ\le B_aT=:\bar{V}), constant window length Ba(w−s)B_a(w-s), and multiplier ZZ, giving E[Z(YAs∨+Ba(w−s)a−YAs∨a)]=Ba(w−s) E[Z]\mathbb{E}\bigl[Z\bigl(Y^{a}_{A^{\vee}_s+B_a(w-s)}-Y^{a}_{A^{\vee}_s}\bigr)\bigr]=B_a(w-s)\,\mathbb{E}[Z]; and at time ww, with window bottom v:=Aw∨v:=A^{\vee}_w (Fw\mathbb{F}_w-measurable, ≥Aw∨,a\ge A^{\vee,a}_w, ≤Vˉ\le\bar{V}), window length λ∗\lambda^{*} (Fw\mathbb{F}_w-measurable, values in [0,Ba(w−s)][0,B_a(w-s)]), and multiplier ZZ (which is Fw\mathbb{F}_w-measurable by (P2)), giving E[Z(YAw∨+λ∗a−YAw∨a)]=E[Zλ∗]\mathbb{E}\bigl[Z\bigl(Y^{a}_{A^{\vee}_w+\lambda^{*}}-Y^{a}_{A^{\vee}_w}\bigr)\bigr]=\mathbb{E}[Z\lambda^{*}]. Subtracting (all terms finite), E[Z(YAw∨a−YAs∨a)]=E[Z(Ba(w−s)−λ∗)]=E[Z(Aw∨−As∨)].\mathbb{E}\bigl[Z\bigl(Y^{a}_{A^{\vee}_w}-Y^{a}_{A^{\vee}_s}\bigr)\bigr]=\mathbb{E}\bigl[Z\bigl(B_a(w-s)-\lambda^{*}\bigr)\bigr]=\mathbb{E}\bigl[Z\bigl(A^{\vee}_w-A^{\vee}_s\bigr)\bigr].

Claim 3. By induction on kk; the case k=1k=1 is claim 1, in both the power and the indicator form. Let k≥2k\ge2 and suppose the claim holds for every choice of k−1k-1 distinct labels. Fix the data of the claim, abbreviate In:=Yvn+λnan−YvnanI_n:=Y^{a_n}_{v_n+\lambda_n}-Y^{a_n}_{v_n}, and for each nn let fnf_n denote either x↦xpnx\mapsto x^{p_n} or x↦1{x≥1}x\mapsto\mathbf{1}\{x\ge1\}, with gn(λ)g_n(\lambda) the corresponding value μpn(λ)\mu_{p_n}(\lambda) or 1−exp⁡(−λ)1-\exp(-\lambda). By (P3) assume 0≤Z≤ζ0\le Z\le\zeta.

Run the cell decomposition of the claim 1 proof for the label a:=aka:=a_k and the window bottom v:=vkv:=v_k: for fixed natural mm, cells F0,…,FQF_0,\dots,F_Q with tops θ:=θq\theta:=\theta_q, and, for each qq, the application of Level-Revealed Conditioning for Jointly Driven Solutions of the Controlled N-Agent Dynamics at time tt with caps cak:=θc_{a_k}:=\theta and cb:=Bbtc_b:=B_bt for b≠akb\neq a_k, giving C⊇FqC\supseteq F_q, C^∈Hq\hat{C}\in\mathcal{H}_q, and Hq\mathcal{H}_q-measurable versions W^q\hat{W}_q of Wq:=Z1FqW_q:=Z\mathbf{1}_{F_q} and v^n,λ^n\hat{v}_n,\hat{\lambda}_n of vn,λnv_n,\lambda_n for all n≤kn\le k, agreeing with the unhatted maps almost surely on CC; and the quantities λq\lambda_q, λq†\lambda^{\dagger}_q, DqD_q, GqG_q built from vk,λk,v^k,λ^kv_k,\lambda_k,\hat{v}_k,\hat{\lambda}_k exactly as there.

Let Kq:=σ(Hq∪⋃n<kσ(Yuan:u≥0))\mathcal{K}_q:=\sigma\bigl(\mathcal{H}_q\cup\bigcup_{n<k}\sigma(Y^{a_n}_u:u\ge0)\bigr). Every generator of Kq\mathcal{K}_q lies in the σ\sigma-algebra Hak+\mathcal{H}^{+}_{a_k} of claim 3 of Level-Revealed Conditioning for Jointly Driven Solutions of the Controlled N-Agent Dynamics (for the caps above): the generators of Hq\mathcal{H}_q do, as shown there, and the full variable families of the clocks ana_n, n<kn<k, do since an≠aka_n\neq a_k. Hence σ(Yθ+sak−Yθak:s≥0)\sigma(Y^{a_k}_{\theta+s}-Y^{a_k}_{\theta}:s\ge0) is independent of Kq\mathcal{K}_q. Define, for n<kn<k, the counts I^n:=Y(v^n∧Vˉ)+(λ^n∧Λˉ)an−Yv^n∧Vˉan\hat{I}_n:=Y^{a_n}_{(\hat{v}_n\wedge\bar{V})+(\hat{\lambda}_n\wedge\bar{\Lambda})}-Y^{a_n}_{\hat{v}_n\wedge\bar{V}}; these are Kq\mathcal{K}_q-measurable by the final clause of claim 1 of Predictable-Window Moment Identities for the Homogeneous Poisson Process, applied with G0:=Kq\mathcal{G}_0:=\mathcal{K}_q (the evaluation levels are Hq\mathcal{H}_q-measurable and every variable YuanY^{a_n}_u is Kq\mathcal{K}_q-measurable); almost surely on CC the truncations do not act and I^n=In\hat{I}_n=I_n.

Apply claim 2 (respectively claim 3, for the indicator form of fkf_k) of Predictable-Window Moment Identities for the Homogeneous Poisson Process to the clock YakY^{a_k} with level θ\theta, σ\sigma-algebra G:=Kq\mathcal{G}:=\mathcal{K}_q, window bottom the constant θ\theta, window length λq†\lambda^{\dagger}_q, and the Kq\mathcal{K}_q-measurable [0,∞][0,\infty]-valued multiplier (W^q∧ζ) 1C^ ∏n<kfn(I^n)(\hat{W}_q\wedge\zeta)\,\mathbf{1}_{\hat{C}}\,\prod_{n<k}f_n(\hat{I}_n). By the almost-sure-equality bookkeeping of the claim 1 proof (extended by I^n=In\hat{I}_n=I_n almost surely on CC, both sides vanishing almost surely off CC), E[Wq fk(Gq)∏n<kfn(In)]=E[Wq gk(λq)∏n<kfn(In)].\mathbb{E}\Bigl[W_q\,f_k(G_q)\prod_{n<k}f_n(I_n)\Bigr]=\mathbb{E}\Bigl[W_q\,g_k(\lambda_q)\prod_{n<k}f_n(I_n)\Bigr]. The error of replacing fk(Ik)f_k(I_k) by fk(Gq)f_k(G_q) is bounded as in the claim 1 proof, with every estimate multiplied by ∏n<kfn(In)≤∏n<kYˉn pn\prod_{n<k}f_n(I_n)\le\prod_{n<k}\bar{Y}_n^{\,p_n}, where Yˉn:=YVˉ+Λˉ+1an\bar{Y}_n:=Y^{a_n}_{\bar{V}+\bar{\Lambda}+1}: in the power case by pkζ E[1FqDqYˉk pk−1∏n<kYˉn pn]p_k\zeta\,\mathbb{E}[\mathbf{1}_{F_q}D_q\bar{Y}_k^{\,p_k-1}\prod_{n<k}\bar{Y}_n^{\,p_n}], in the indicator case by ζ E[1FqDq∏n<kYˉn pn]\zeta\,\mathbb{E}[\mathbf{1}_{F_q}D_q\prod_{n<k}\bar{Y}_n^{\,p_n}]. The dominating product Yˉk pk∏n<kYˉn pn\bar{Y}_k^{\,p_k}\prod_{n<k}\bar{Y}_n^{\,p_n} is integrable with expectation ∏n≤kμpn(Vˉ+Λˉ+1)<∞\prod_{n\le k}\mu_{p_n}(\bar{V}+\bar{\Lambda}+1)<\infty: the variables Yˉ1,…,Yˉk\bar{Y}_1,\dots,\bar{Y}_k are functions of the variables of kk distinct clocks, whose σ\sigma-algebras form an independent family (hypothesis of Level-Revealed Conditioning for Jointly Driven Solutions of the Controlled N-Agent Dynamics), so each partial product ∏n≤jYˉn pn\prod_{n\le j}\bar{Y}_n^{\,p_n} is independent of Yˉj+1 pj+1\bar{Y}_{j+1}^{\,p_{j+1}} by part (a) of Grouping Lemma for Independent Random Variables together with Joint Distribution, Expectations, and Block Independence for Independent Random Variables --- functions of disjoint blocks of an independent family are independent --- and Expectation of a Product of Independent Random Variables applies inductively, each factor having finite expectation μpn(Vˉ+Λˉ+1)\mu_{p_n}(\bar{V}+\bar{\Lambda}+1) by claim 4 of Predictable-Window Moment Identities for the Homogeneous Poisson Process and claim 2 of Image Measures, Measures with Densities, and Change of Variables. Summing over qq and letting m→∞m\to\infty exactly as in the claim 1 proof --- the same pointwise limits λ(m)→λk\lambda_{(m)}\to\lambda_k and D(m)↓0D_{(m)}\downarrow0, with dominated convergence now using the integrable dominators ζ μpk(Λˉ)∏n<kYˉn pn\zeta\,\mu_{p_k}(\bar{\Lambda})\prod_{n<k}\bar{Y}_n^{\,p_n} in the power case, ζ∏n<kYˉn pn\zeta\prod_{n<k}\bar{Y}_n^{\,p_n} in the indicator case, and Yˉk pk∏n<kYˉn pn\bar{Y}_k^{\,p_k}\prod_{n<k}\bar{Y}_n^{\,p_n} for the error terms --- yields E[Z ∏n=1kfn(In)]=E[Z gk(λk)∏n=1k−1fn(In)].\mathbb{E}\Bigl[Z\,\prod_{n=1}^{k}f_n(I_n)\Bigr]=\mathbb{E}\Bigl[Z\,g_k(\lambda_k)\prod_{n=1}^{k-1}f_n(I_n)\Bigr]. The multiplier Z gk(λk)Z\,g_k(\lambda_k) is Ft\mathbb{F}_t-measurable and nonnegative (λk\lambda_k is Ft\mathbb{F}_t-measurable and gkg_k is Borel), so the induction hypothesis for the labels a1,…,ak−1a_1,\dots,a_{k-1} applies and gives E[Z∏n≤kfn(In)]=E[Z∏n≤kgn(λn)]\mathbb{E}[Z\prod_{n\le k}f_n(I_n)]=\mathbb{E}[Z\prod_{n\le k}g_n(\lambda_n)], completing the induction; the monotone reduction of (P3) removes the boundedness of ZZ.

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