TheoremBase

Proof

Throughout, the theorem refers to Existence, Uniqueness, Causality, and Measurability of the Open-Loop Aggregate Solution, and we use freely its claim 1: at every step k<Kk<K each t↦Ctc,(k)t\mapsto\mathsf{C}^{c,(k)}_t is nondecreasing and satisfies Cθkc,(k)=κkc\mathsf{C}^{c,(k)}_{\theta_k}=\kappa^{c}_k and ∣Ctc,(k)−Csc,(k)∣≤NB(t−s)|\mathsf{C}^{c,(k)}_t-\mathsf{C}^{c,(k)}_s|\le NB(t-s) for 0≤s≤t≤T0\le s\le t\le T (hence is continuous); λkc>κkc\lambda^{c}_k>\kappa^{c}_k; θk+1>θk\theta_{k+1}>\theta_k; Cθk+1c,(k)=λkc\mathsf{C}^{c,(k)}_{\theta_{k+1}}=\lambda^{c}_k for c∈Jkc\in\mathcal{J}_k; and the recursion stops at a finite index KK. Recall also that θk+1≤hkc\theta_{k+1}\le h^{c}_k for every label cc (by the definition θk+1=min⁡(T,min⁡chkc)\theta_{k+1}=\min(T,\min_ch^{c}_k)), and that κk+1c=Cθk+1c,(k)\kappa^{c}_{k+1}=\mathsf{C}^{c,(k)}_{\theta_{k+1}}. Two elementary facts about a counting path qq (Counting Path and Its Jump Times) are used: (F1) for a natural number jj, the set {t≥0:q(t)≥j}\{t\ge0:q(t)\ge j\} is, if nonempty, the interval [τj(q),∞)[\tau_j(q),\infty) — it is an up-set by monotonicity, contains its greatest lower bound τj(q)\tau_j(q) by right-continuity (q(τj)q(\tau_j) is the greatest lower bound of the values q(s)≥jq(s)\ge j, s>τjs>\tau_j), and so equals [τj(q),∞)[\tau_j(q),\infty); (F2) for a fixed step kk and label cc, the hitting time hkch^{c}_k is nondecreasing as a function of the next jump level it is computed from: if λ≤λ′\lambda\le\lambda' then {t∈[θk,T]:Ctc,(k)≥λ′}⊆{t∈[θk,T]:Ctc,(k)≥λ}\{t\in[\theta_k,T]:\mathsf{C}^{c,(k)}_t\ge\lambda'\}\subseteq\{t\in[\theta_k,T]:\mathsf{C}^{c,(k)}_t\ge\lambda\}, so the greatest lower bound of the former is at least that of the latter. Finally, since Cc,(k)\mathsf{C}^{c,(k)} is continuous and nondecreasing on [θk,T][\theta_k,T], the set {t∈[θk,T]:Ctc,(k)≥λkc}\{t\in[\theta_k,T]:\mathsf{C}^{c,(k)}_t\ge\lambda^{c}_k\} is, if nonempty, the interval [hkc,T][h^{c}_k,T] (its greatest lower bound hkch^{c}_k belongs to it by continuity, as the limit of a sequence in the set), so that (F3) Ctc,(k)<λkc\mathsf{C}^{c,(k)}_t<\lambda^{c}_k for t∈[θk,T]t\in[\theta_k,T] with t<hkct<h^{c}_k, and Chkcc,(k)≥λkc\mathsf{C}^{c,(k)}_{h^{c}_k}\ge\lambda^{c}_k when hkc≤Th^{c}_k\le T.

Step 1 (claim 1). Fix a label c=(σ,γ)c=(\sigma,\gamma). By the definition of the recursion consumed times, Crec,c\mathsf{C}^{\mathrm{rec},c} coincides on [θk,θk+1][\theta_k,\theta_{k+1}] with Cc,(k)\mathsf{C}^{c,(k)} for k<Kk<K and is constant equal to κKc\kappa^{c}_K on [θK,T][\theta_K,T]; on each such interval it is nondecreasing and NBNB-Lipschitz by claim 1 of the theorem, and the pieces agree at the junction times θk+1\theta_{k+1} (as noted in the theorem). Hence Crec,c\mathsf{C}^{\mathrm{rec},c} is nondecreasing on [0,T][0,T], and for s≤ts\le t lying in consecutive pieces [θk,θk+1][\theta_{k},\theta_{k+1}], …\dots, [θk′,θk′+1][\theta_{k'},\theta_{k'+1}] (and possibly the terminal piece [θK,T][\theta_K,T], on which the map is constant) the Lipschitz bound follows by adding the bounds over the pieces (the intermediate junction times θk+1,…,θk′\theta_{k+1},\dots,\theta_{k'} lying between ss and tt); C0rec,c=Cθ0c,(0)=κ0c=0\mathsf{C}^{\mathrm{rec},c}_0=\mathsf{C}^{c,(0)}_{\theta_0}=\kappa^{c}_0=0. For k<Kk<K, κk+1c=Cθk+1c,(k)≥Cθkc,(k)=κkc\kappa^{c}_{k+1}=\mathsf{C}^{c,(k)}_{\theta_{k+1}}\ge\mathsf{C}^{c,(k)}_{\theta_k}=\kappa^{c}_k by monotonicity, and by induction Ctrec,c≤κi+1c≤κk+1c\mathsf{C}^{\mathrm{rec},c}_t\le\kappa^{c}_{i+1}\le\kappa^{c}_{k+1} for t∈[θi,θi+1]t\in[\theta_i,\theta_{i+1}] and i≤ki\le k, which gives Ctrec,c≤κk+1c\mathsf{C}^{\mathrm{rec},c}_t\le\kappa^{c}_{k+1} on [0,θk+1][0,\theta_{k+1}]. For t∈[0,θk]t\in[0,\theta_k] this yields Ctrec,c≤κkc<λkc\mathsf{C}^{\mathrm{rec},c}_t\le\kappa^{c}_k<\lambda^{c}_k, and for t∈[θk,θk+1)t\in[\theta_k,\theta_{k+1}) we have t<θk+1≤hkct<\theta_{k+1}\le h^{c}_k, so Ctrec,c=Ctc,(k)<λkc\mathsf{C}^{\mathrm{rec},c}_t=\mathsf{C}^{c,(k)}_t<\lambda^{c}_k by (F3); together, Ctrec,c<λkc\mathsf{C}^{\mathrm{rec},c}_t<\lambda^{c}_k on [0,θk+1)[0,\theta_{k+1}).

Now let k<Kk<K and c∈Jkc\in\mathcal{J}_k. Then κk+1c=Cθk+1c,(k)=λkc\kappa^{c}_{k+1}=\mathsf{C}^{c,(k)}_{\theta_{k+1}}=\lambda^{c}_k by claim 1 of the theorem. If x(k),σx^{(k),\sigma} were 00, the integrand 1(θk,T](s)Nx(k),σβ(σ,γ,x(k),as)\mathbf{1}_{(\theta_k,T]}(s)Nx^{(k),\sigma}\beta(\sigma,\gamma,x^{(k)},a_s) defining Cc,(k)\mathsf{C}^{c,(k)} would vanish identically, so Ctc,(k)=κkc<λkc\mathsf{C}^{c,(k)}_t=\kappa^{c}_k<\lambda^{c}_k for every tt (the integral of the zero function being 00 by the scalar rule of claim 1 of Linearity and Monotonicity of the Lebesgue Integral with scalar 00), contradicting Cθk+1c,(k)≥λkc\mathsf{C}^{c,(k)}_{\theta_{k+1}}\ge\lambda^{c}_k; hence x(k),σ>0x^{(k),\sigma}>0. Since θk+1∈[θk,T]\theta_{k+1}\in[\theta_k,T] and Cθk+1c,(k)≥λkc\mathsf{C}^{c,(k)}_{\theta_{k+1}}\ge\lambda^{c}_k, the time θk+1\theta_{k+1} belongs to the set whose greatest lower bound is hkch^{c}_k, so hkc≤θk+1h^{c}_k\le\theta_{k+1}; with θk+1≤hkc\theta_{k+1}\le h^{c}_k this gives θk+1=hkc\theta_{k+1}=h^{c}_k. Finally, the set {t∈[0,T]:Ctrec,c≥λkc}\{t\in[0,T]:\mathsf{C}^{\mathrm{rec},c}_t\ge\lambda^{c}_k\} contains θk+1\theta_{k+1} (as Cθk+1rec,c=Cθk+1c,(k)=λkc\mathsf{C}^{\mathrm{rec},c}_{\theta_{k+1}}=\mathsf{C}^{c,(k)}_{\theta_{k+1}}=\lambda^{c}_k) and contains no t<θk+1t<\theta_{k+1} (shown above), so its greatest lower bound is θk+1\theta_{k+1}.

Step 2 (claim 2). Assume no step k<Kk<K is a tie. We show by induction on k≤Kk\le K that x(k)∈GNx^{(k)}\in\mathbb{G}_N. For k=0k=0, x(0)=x0∈GNx^{(0)}=x_0\in\mathbb{G}_N. Let k<Kk<K with x(k)∈GNx^{(k)}\in\mathbb{G}_N. If Jk\mathcal{J}_k is empty, x(k+1)=x(k)x^{(k+1)}=x^{(k)}. Otherwise Jk={c}\mathcal{J}_k=\{c\} for a single label c=(σ,γ)c=(\sigma,\gamma), and x(k+1)=x(k)+vc/Nx^{(k+1)}=x^{(k)}+v_c/N, which differs from x(k)x^{(k)} only in the coordinates σ\sigma and γ\gamma: x(k+1),σ=x(k),σ−1/Nx^{(k+1),\sigma}=x^{(k),\sigma}-1/N and x(k+1),γ=x(k),γ+1/Nx^{(k+1),\gamma}=x^{(k),\gamma}+1/N. By Step 1, x(k),σ>0x^{(k),\sigma}>0, and Nx(k),σ∈N0Nx^{(k),\sigma}\in\mathbb{N}_0 by the definition of GN\mathbb{G}_N, so Nx(k),σ≥1Nx^{(k),\sigma}\ge1 and x(k+1),σ≥0x^{(k+1),\sigma}\ge0; thus all coordinates of x(k+1)x^{(k+1)} are nonnegative, they sum to 11 (the sum being unchanged), and NN times each is in N0\mathbb{N}_0; by the definition of the probability simplex and of GN\mathbb{G}_N, x(k+1)∈GNx^{(k+1)}\in\mathbb{G}_N. This completes the induction. The recursion stops at the index KK (claim 1 of the theorem) because θK=T\theta_K=T or x(K)∉GNx^{(K)}\notin\mathbb{G}_N; the second alternative is excluded, so θK=T\theta_K=T and x(K)∈GNx^{(K)}\in\mathbb{G}_N, i.e. the data are conflict-free.

Step 3 (the deleted path). Let c0c_0, uu and p−p^{-} be as in claim 3, and write q=pc0q=p^{c_0}, q−=p−,c0q^{-}=p^{-,c_0}. Since uu is a jump time of qq, q(u)>q(u−)q(u)>q(u-), and by the unit-jump property q(u)=q(u−)+1q(u)=q(u-)+1, both values being integers with difference in (0,1](0,1] (the value q(u−)q(u-) is the least upper bound of a nonempty set of elements of N0\mathbb{N}_0 bounded above by q(u)q(u), hence its maximum and in particular an integer, with q(u−)≥q(0)=0q(u-)\ge q(0)=0). We check that q−q^{-} is a counting path. q−(0)=q(0)=0q^{-}(0)=q(0)=0 (as u>0u>0), and q−(t)q^{-}(t) is an integer; it is nonnegative since for t<ut<u it equals q(t)≥0q(t)\ge0, and for t≥ut\ge u, q(t)≥q(u)=q(u−)+1≥1q(t)\ge q(u)=q(u-)+1\ge1. Monotonicity: for s≤ts\le t, if both are <u<u or both ≥u\ge u then q−(t)−q−(s)=q(t)−q(s)≥0q^{-}(t)-q^{-}(s)=q(t)-q(s)\ge0; if s<u≤ts<u\le t then q−(t)−q−(s)=q(t)−1−q(s)≥q(u)−1−q(u−)=0q^{-}(t)-q^{-}(s)=q(t)-1-q(s)\ge q(u)-1-q(u-)=0, using q(s)≤q(u−)q(s)\le q(u-) (the least upper bound over [0,u)[0,u)) and q(t)≥q(u)q(t)\ge q(u). Right-continuity at tt: the greatest lower bound of {q−(s):s>t}\{q^{-}(s):s>t\} equals that of {q(s):s>t}\{q(s):s>t\} minus the constant 1{t≥u}\mathbf{1}\{t\ge u\} when t≥ut\ge u (all s>ts>t then satisfy s≥us\ge u) and when t<ut<u (the values for s∈(t,u)s\in(t,u) already realise the greatest lower bound q(t)q(t) of {q(s):s>t}\{q(s):s>t\}, qq being nondecreasing, and every q−(s)q^{-}(s) with s>ts>t is at least q−(t)=q(t)q^{-}(t)=q(t) by the monotonicity just proved), so it equals q−(t)q^{-}(t). Unit jumps: for t≠ut\ne u the jump q−(t)−q−(t−)q^{-}(t)-q^{-}(t-) equals q(t)−q(t−)≤1q(t)-q(t-)\le1 (for t>ut>u the subtracted constant is the same on a left neighbourhood; for t<ut<u nothing is subtracted on [0,t][0,t]); at t=ut=u, q−(u−)=q(u−)q^{-}(u-)=q(u-) and q−(u)=q(u)−1=q(u−)q^{-}(u)=q(u)-1=q(u-), so the jump is 00. Hence q−q^{-} is a counting path, and q−=qq^{-}=q on [0,u)[0,u), q−=q−1q^{-}=q-1 on [u,∞)[u,\infty).

Consequently, for a consumed level κ<u\kappa<u and j=q(κ)+1=q−(κ)+1j=q(\kappa)+1=q^{-}(\kappa)+1: (a) q(u)≥q(u−)+1≥q(κ)+1=jq(u)\ge q(u-)+1\ge q(\kappa)+1=j, so τj(q)≤u\tau_j(q)\le u by (F1); (b) if τj(q)<u\tau_j(q)<u then τj(q−)=τj(q)\tau_j(q^{-})=\tau_j(q): indeed q−≤qq^{-}\le q gives {q−≥j}⊆{q≥j}\{q^{-}\ge j\}\subseteq\{q\ge j\} and so τj(q−)≥τj(q)\tau_j(q^{-})\ge\tau_j(q), while q−(τj(q))=q(τj(q))≥jq^{-}(\tau_j(q))=q(\tau_j(q))\ge j (by (F1), as τj(q)<u\tau_j(q)<u) gives τj(q−)≤τj(q)\tau_j(q^{-})\le\tau_j(q); (c) if τj(q)=u\tau_j(q)=u then τj(q−)>u\tau_j(q^{-})>u: for t∈[κ,u)t\in[\kappa,u), q−(t)=q(t)<jq^{-}(t)=q(t)<j (as t<τj(q)t<\tau_j(q), by (F1)), and q−(u)=q(u)−1=q(u−)q^{-}(u)=q(u)-1=q(u-), where q(u−)q(u-) is the least upper bound of the values q(t)q(t), t<ut<u, all of which are ≤j−1\le j-1 (for t<κt<\kappa by monotonicity, since q(κ)=j−1q(\kappa)=j-1; for t∈[κ,u)t\in[\kappa,u) as just shown), so q−(u)≤j−1<jq^{-}(u)\le j-1<j; thus no t≤ut\le u lies in {q−≥j}\{q^{-}\ge j\}, and by (F1) τj(q−)>u\tau_j(q^{-})>u (the set being [τj(q−),∞)[\tau_j(q^{-}),\infty) or empty, with τj(q−)=+∞\tau_j(q^{-})=+\infty in the latter case). In either case τj(q−)≥τj(q)\tau_j(q^{-})\ge\tau_j(q).

Step 4 (claim 3). Keep the notation of claim 3. We prove by induction on i∈{0,…,k}i\in\{0,\dots,k\} that the recursion for p−p^{-} performs step ii with θi−=θi\theta^{-}_i=\theta_i, x−(i)=x(i)x^{-(i)}=x^{(i)} and κi−,c=κic\kappa^{-,c}_i=\kappa^{c}_i for all cc, and that, for i<ki<k, also θi+1−=θi+1\theta^{-}_{i+1}=\theta_{i+1}, Ji−=Ji\mathcal{J}^{-}_i=\mathcal{J}_i, x−(i+1)=x(i+1)x^{-(i+1)}=x^{(i+1)} and κi+1−,c=κi+1c\kappa^{-,c}_{i+1}=\kappa^{c}_{i+1}. The initial data agree. Let i<ki<k and assume agreement at step ii; since i<k<Ki<k<K, the recursion for pp has not stopped at any index ≤i\le i, i.e. θi<T\theta_i<T and x(i)∈GNx^{(i)}\in\mathbb{G}_N, hence neither has the recursion for p−p^{-}, and both perform step ii. The functions Cc,(i)\mathsf{C}^{c,(i)} and C−,c,(i)\mathsf{C}^{-,c,(i)} coincide for every cc (their definition involves only κic\kappa^{c}_i, θi\theta_i, x(i)x^{(i)} and aa). For c≠c0c\ne c_0, p−,c=pcp^{-,c}=p^{c} gives λi−,c=λic\lambda^{-,c}_i=\lambda^{c}_i and hi−,c=hich^{-,c}_i=h^{c}_i. For c0c_0: κic0≤κkc0<λkc0=u\kappa^{c_0}_i\le\kappa^{c_0}_k<\lambda^{c_0}_k=u (Step 1 and claim 1 of the theorem), so Step 3 applies with κ=κic0\kappa=\kappa^{c_0}_i and j=q(κic0)+1j=q(\kappa^{c_0}_i)+1, for which λic0=τj(q)\lambda^{c_0}_i=\tau_j(q) and λi−,c0=τj(q−)\lambda^{-,c_0}_i=\tau_j(q^{-}): either λic0<u\lambda^{c_0}_i<u and λi−,c0=λic0\lambda^{-,c_0}_i=\lambda^{c_0}_i, in which case all quantities of step ii coincide; or λic0=u\lambda^{c_0}_i=u and λi−,c0>u\lambda^{-,c_0}_i>u. In the latter case c0∉Jic_0\notin\mathcal{J}_i, since otherwise κi+1c0=λic0=u\kappa^{c_0}_{i+1}=\lambda^{c_0}_i=u (Step 1), whereas κi+1c0≤κkc0<u\kappa^{c_0}_{i+1}\le\kappa^{c_0}_k<u; hence Cθi+1c0,(i)<λic0\mathsf{C}^{c_0,(i)}_{\theta_{i+1}}<\lambda^{c_0}_i, so θi+1<hic0\theta_{i+1}<h^{c_0}_i (if θi+1=hic0≤T\theta_{i+1}=h^{c_0}_i\le T, then Cθi+1c0,(i)≥λic0\mathsf{C}^{c_0,(i)}_{\theta_{i+1}}\ge\lambda^{c_0}_i by (F3)), and hi−,c0≥hic0>θi+1h^{-,c_0}_i\ge h^{c_0}_i>\theta_{i+1} by (F2). Since hic0>θi+1h^{c_0}_i>\theta_{i+1} and hi−,c0>θi+1h^{-,c_0}_i>\theta_{i+1}, the label c0c_0 may be dropped from both minima defining θi+1\theta_{i+1} and θi+1−\theta^{-}_{i+1}, and hi−,c=hich^{-,c}_i=h^{c}_i for c≠c0c\ne c_0; hence θi+1−=θi+1\theta^{-}_{i+1}=\theta_{i+1}. Then Ji−=Ji\mathcal{J}^{-}_i=\mathcal{J}_i: for c≠c0c\ne c_0 the membership conditions coincide, and c0c_0 belongs to neither (Cθi+1−,c0,(i)=Cθi+1c0,(i)<λic0<λi−,c0\mathsf{C}^{-,c_0,(i)}_{\theta_{i+1}}=\mathsf{C}^{c_0,(i)}_{\theta_{i+1}}<\lambda^{c_0}_i<\lambda^{-,c_0}_i). Hence x−(i+1)=x(i+1)x^{-(i+1)}=x^{(i+1)} and κi+1−,c=Cθi+1−,c,(i)=κi+1c\kappa^{-,c}_{i+1}=\mathsf{C}^{-,c,(i)}_{\theta_{i+1}}=\kappa^{c}_{i+1}, completing the induction.

At step kk (performed by both recursions, by the same argument): C−,c,(k)=Cc,(k)\mathsf{C}^{-,c,(k)}=\mathsf{C}^{c,(k)} for every cc; λk−,c=λkc\lambda^{-,c}_k=\lambda^{c}_k and hk−,c=hkch^{-,c}_k=h^{c}_k for c≠c0c\ne c_0; and for c0c_0, κkc0<u=λkc0=τj(q)\kappa^{c_0}_k<u=\lambda^{c_0}_k=\tau_j(q) with j=q(κkc0)+1j=q(\kappa^{c_0}_k)+1; since κk−,c0=κkc0<u\kappa^{-,c_0}_k=\kappa^{c_0}_k<u we have q−(κkc0)=q(κkc0)q^{-}(\kappa^{c_0}_k)=q(\kappa^{c_0}_k), so λk−,c0=τj(q−)\lambda^{-,c_0}_k=\tau_j(q^{-}), and by Step 3(c) λk−,c0>u\lambda^{-,c_0}_k>u, whence hk−,c0≥hkc0h^{-,c_0}_k\ge h^{c_0}_k by (F2). Since c′∈Jkc'\in\mathcal{J}_k, Step 1 gives hkc′=θk+1h^{c'}_k=\theta_{k+1}, so hk−,c′=θk+1h^{-,c'}_k=\theta_{k+1}; every other hk−,ch^{-,c}_k is at least θk+1\theta_{k+1} (equal to hkc≥θk+1h^{c}_k\ge\theta_{k+1} for c≠c0c\ne c_0, and hk−,c0≥hkc0≥θk+1h^{-,c_0}_k\ge h^{c_0}_k\ge\theta_{k+1}), and T≥θk+1T\ge\theta_{k+1}; therefore θk+1−=min⁡(T,min⁡chk−,c)=θk+1\theta^{-}_{k+1}=\min(T,\min_ch^{-,c}_k)=\theta_{k+1}. The recursion consumed times of p−p^{-} on [0,θk+1][0,\theta_{k+1}] are determined by the steps 0,…,k0,\dots,k (on [θi−,θi+1−][\theta^{-}_i,\theta^{-}_{i+1}] they equal C−,c,(i)\mathsf{C}^{-,c,(i)}), which coincide with those of pp; hence Ct−,rec,c=Ctrec,c\mathsf{C}^{-,\mathrm{rec},c}_t=\mathsf{C}^{\mathrm{rec},c}_t for all cc and t∈[0,θk+1]t\in[0,\theta_{k+1}]. In particular Cθk+1−,rec,c0=Cθk+1rec,c0=Cθk+1c0,(k)=λkc0=u\mathsf{C}^{-,\mathrm{rec},c_0}_{\theta_{k+1}}=\mathsf{C}^{\mathrm{rec},c_0}_{\theta_{k+1}}=\mathsf{C}^{c_0,(k)}_{\theta_{k+1}}=\lambda^{c_0}_k=u (claim 1 of the theorem, as c0∈Jkc_0\in\mathcal{J}_k). Finally, by Step 1 applied to c′∈Jkc'\in\mathcal{J}_k with v=λkc′v=\lambda^{c'}_k (a jump time of pc′p^{c'}: it is τj′(pc′)\tau_{j'}(p^{c'}) with j′=pc′(κkc′)+1≥1j'=p^{c'}(\kappa^{c'}_k)+1\ge1, is finite since c′∈Jkc'\in\mathcal{J}_k gives Cθk+1c′,(k)≥λkc′\mathsf{C}^{c',(k)}_{\theta_{k+1}}\ge\lambda^{c'}_k, is positive since pc′(τj′)≥j′≥1>0=pc′(0)p^{c'}(\tau_{j'})\ge j'\ge1>0=p^{c'}(0), and satisfies pc′(τj′)≥j′>pc′(τj′−)p^{c'}(\tau_{j'})\ge j'>p^{c'}(\tau_{j'}-), since by (F1) and the definition of τj′\tau_{j'} every value pc′(s)p^{c'}(s) with s<τj′s<\tau_{j'} satisfies pc′(s)<j′p^{c'}(s)<j', hence pc′(s)≤j′−1p^{c'}(s)\le j'-1 by integer-valuedness, so that the least upper bound pc′(τj′−)p^{c'}(\tau_{j'}-) is at most j′−1j'-1), θk+1\theta_{k+1} is the greatest lower bound of {t∈[0,T]:Ctrec,c′≥v}\{t\in[0,T]:\mathsf{C}^{\mathrm{rec},c'}_t\ge v\}: no t<θk+1t<\theta_{k+1} belongs to this set and θk+1\theta_{k+1} does. As C−,rec,c′\mathsf{C}^{-,\mathrm{rec},c'} agrees with Crec,c′\mathsf{C}^{\mathrm{rec},c'} on [0,θk+1][0,\theta_{k+1}], the same two facts hold for {t∈[0,T]:Ct−,rec,c′≥v}\{t\in[0,T]:\mathsf{C}^{-,\mathrm{rec},c'}_t\ge v\}, whose greatest lower bound is therefore θk+1\theta_{k+1} as well. ■\blacksquare

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