TheoremBase

Proof

Throughout, the stopping-time toolkit is cited by claim number, Dn={kT2−n:k∈{0,…,2n}}D_n=\{kT2^{-n}:k\in\{0,\dots,2^n\}\} is the nn-th dyadic grid, and σn,τn\sigma_n,\tau_n are the dyadic approximations from above of σ,τ\sigma,\tau (toolkit, claim 3). A real-valued function on Ω\Omega is called G\mathcal{G}-measurable, for a σ\sigma-algebra G⊆F\mathcal{G}\subseteq\mathcal{F}, when it is measurable with respect to G\mathcal{G} and the Borel σ\sigma-algebra of the real line. Every random variable UU with ∣U∣≤C|U|\le C everywhere is square-integrable (E[U2]≤C2\mathbb{E}[U^2]\le C^2 by monotonicity of the integral), hence integrable; this is used without further comment for all the bounded random variables below.

Step 0: two forms of right-continuity. Let ω∈Ω\omega\in\Omega be a point at which the path t↦Mt(ω)t\mapsto M_t(\omega) is right-continuous at every t∈[0,T)t\in[0,T) in the sense of the hypothesis (in particular, any ω∈Ω0\omega\in\Omega_0). The path is then right-continuous in the sequential sense of the toolkit: let t∈[0,T]t\in[0,T] and let (sj)(s_j) be a sequence in [t,T][t,T] converging to tt. If t=Tt=T then sj=Ts_j=T for all jj and there is nothing to prove. If t<Tt<T, given ε>0\varepsilon>0 choose η>0\eta>0 from the hypothesis; for all large jj we have t≤sj≤min⁡(t+η,T)t\le s_j\le\min(t+\eta,T), hence ∣Msj(ω)−Mt(ω)∣≤ε|M_{s_j}(\omega)-M_t(\omega)|\le\varepsilon. Conversely, if a path is right-continuous in the sequential sense at every point of [0,T][0,T], it is right-continuous at every t∈[0,T)t\in[0,T) in the sense of the hypothesis: otherwise there would be t∈[0,T)t\in[0,T), ε>0\varepsilon>0 and, for each j∈Nj\in\mathbb{N}, a point sj∈[t,min⁡(t+1/j,T)]s_j\in[t,\min(t+1/j,T)] with ∣Msj(ω)−Mt(ω)∣>ε|M_{s_j}(\omega)-M_t(\omega)|>\varepsilon, contradicting the sequential form along (sj)(s_j).

Step 1: measurability and convergence of the dyadic samples (claim (a)). Since the pair σ≤τ\sigma\le\tau in the statement is arbitrary, whatever is proved below for τ\tau (respectively for the pair σ≤τ\sigma\le\tau) holds for every stopping time ρ\rho (respectively every pair ρ≤ρ′\rho\le\rho') of (Ft)t∈[0,T](\mathcal{F}_t)_{t\in[0,T]}; claims (a) and (b) are used in that generality in Step 4. Fix nn. At every ω\omega exactly one of the sets {τn=d}\{\tau_n=d\}, d∈Dnd\in D_n, contains ω\omega, so pointwise

Mτn=∑d∈DnMd 1{τn=d}.M_{\tau_n}=\sum_{d\in D_n}M_d\,\mathbf{1}_{\{\tau_n=d\}} .

Each {τn=d}\{\tau_n=d\} lies in Fd⊆FT\mathcal{F}_d\subseteq\mathcal{F}_T (toolkit, claim 1) and each MdM_d is Fd\mathcal{F}_d-measurable, so MτnM_{\tau_n} is an FT\mathcal{F}_T-measurable random variable by claims 1--3 of the arithmetic lemma for measurable functions, with ∣Mτn∣≤K|M_{\tau_n}|\le K. For ω∈Ω0\omega\in\Omega_0, (τn(ω))n(\tau_n(\omega))_n is a sequence in [τ(ω),T][\tau(\omega),T] converging to τ(ω)\tau(\omega) (toolkit, claim 3), so Step 0 gives Mτn(ω)→Mτ(ω)M_{\tau_n}(\omega)\to M_\tau(\omega). Hence Mτn1Ω0→Mτ1Ω0M_{\tau_n}\mathbf{1}_{\Omega_0}\to M_\tau\mathbf{1}_{\Omega_0} at every point of Ω\Omega (both sides vanish off Ω0\Omega_0), and the limit is a random variable on (Ω,F,P)(\Omega,\mathcal{F},P) by claim 5 of the arithmetic lemma (1Ω0\mathbf{1}_{\Omega_0} being F\mathcal{F}-measurable as Ω0∈F\Omega_0\in\mathcal{F}), bounded by KK. The same applies to σ\sigma. If every path of MM is right-continuous at every t∈[0,T)t\in[0,T), then by Step 0 every path is right-continuous in the sequential sense, MM is adapted, so MM is progressively measurable by claim 2 of the progressive measurability toolkit, and MτM_\tau is Fτ\mathcal{F}_\tau-measurable by claim 4(ii) of the stopping-time toolkit. This proves (a).

Step 2: optional stopping on the dyadic grid. Fix nn and list DnD_n as t0<t1<⋯<t2nt_0<t_1<\dots<t_{2^n}. By toolkit claim 3, σn≤τn\sigma_n\le\tau_n pointwise. For every ω\omega, with σn(ω)=ti\sigma_n(\omega)=t_i and τn(ω)=ti′\tau_n(\omega)=t_{i'}, i≤i′i\le i', the indicator of {σn≤tk}∩{τn>tk}\{\sigma_n\le t_k\}\cap\{\tau_n>t_k\} at ω\omega equals 11 exactly for i≤k≤i′−1i\le k\le i'-1, so the telescoping identity

Mτn−Mσn=∑k=02n−1(Mtk+1−Mtk) 1{σn≤tk}1{τn>tk}M_{\tau_n}-M_{\sigma_n}=\sum_{k=0}^{2^n-1}\big(M_{t_{k+1}}-M_{t_k}\big)\,\mathbf{1}_{\{\sigma_n\le t_k\}}\mathbf{1}_{\{\tau_n>t_k\}}

holds pointwise (an empty sum when i=i′i=i'). Let D∈FσD\in\mathcal{F}_\sigma. Since σ≤σn\sigma\le\sigma_n, toolkit claim 3 gives D∈FσnD\in\mathcal{F}_{\sigma_n}, so D∩{σn≤tk}∈FtkD\cap\{\sigma_n\le t_k\}\in\mathcal{F}_{t_k} by the definition of the prior σ\sigma-algebra; and {τn>tk}∈Ftk\{\tau_n>t_k\}\in\mathcal{F}_{t_k} by toolkit claim 1. Hence Ak=D∩{σn≤tk}∩{τn>tk}∈FtkA_k=D\cap\{\sigma_n\le t_k\}\cap\{\tau_n>t_k\}\in\mathcal{F}_{t_k}, and the martingale property in averaged form of the martingale definition, for the times tk≤tk+1t_k\le t_{k+1}, gives E[Mtk+11Ak]=E[Mtk1Ak]\mathbb{E}[M_{t_{k+1}}\mathbf{1}_{A_k}]=\mathbb{E}[M_{t_k}\mathbf{1}_{A_k}]. Multiplying the telescoping identity by 1D\mathbf{1}_D, taking expectations (all terms are bounded random variables) and using linearity of the integral,

E[(Mτn−Mσn)1D]=∑k=02n−1(E[Mtk+11Ak]−E[Mtk1Ak])=0.\mathbb{E}\big[(M_{\tau_n}-M_{\sigma_n})\mathbf{1}_D\big]=\sum_{k=0}^{2^n-1}\Big(\mathbb{E}\big[M_{t_{k+1}}\mathbf{1}_{A_k}\big]-\mathbb{E}\big[M_{t_k}\mathbf{1}_{A_k}\big]\Big)=0 .

Step 3: passage to the limit (claim (b)). Put gn=(Mτn−Mσn)1Dg_n=(M_{\tau_n}-M_{\sigma_n})\mathbf{1}_D and fn=gn1Ω0f_n=g_n\mathbf{1}_{\Omega_0}. Both are random variables bounded by 2K2K everywhere and agree on Ω0\Omega_0, so E[fn]=E[gn]=0\mathbb{E}[f_n]=\mathbb{E}[g_n]=0 by claim 2 of the lemma on almost sure equality of bounded random variables and Step 2. By Step 1, fn→f=(Mτ−Mσ)1Ω01Df_n\to f=(M_\tau-M_\sigma)\mathbf{1}_{\Omega_0}\mathbf{1}_D at every point of Ω\Omega, and ∣fn∣≤2K|f_n|\le2K with the constant 2K2K integrable on the probability space. The dominated convergence theorem yields E[f]=lim⁡nE[fn]=0\mathbb{E}[f]=\lim_n\mathbb{E}[f_n]=0, which by linearity is the identity of (b). For the particular case take σ\sigma to be the constant 00 (a stopping time with σ≤τ\sigma\le\tau, toolkit claim 1) and D=ΩD=\Omega, which lies in Fσ=F0\mathcal{F}_\sigma=\mathcal{F}_0 by toolkit claim 2: then E[Mτ1Ω0]=E[M01Ω0]=E[M0]\mathbb{E}[M_\tau\mathbf{1}_{\Omega_0}]=\mathbb{E}[M_0\mathbf{1}_{\Omega_0}]=\mathbb{E}[M_0], the last equality again by claim 2 of the almost-sure-equality lemma. Finally, suppose every path of MM is right-continuous at every t∈[0,T)t\in[0,T). By Step 1, MσM_\sigma is Fσ\mathcal{F}_\sigma-measurable and MτM_\tau is a random variable, both bounded by KK, hence square-integrable; and for D∈FσD\in\mathcal{F}_\sigma,

E[Mτ1D]=E[Mτ1Ω01D]=E[Mσ1Ω01D]=E[Mσ1D],\mathbb{E}[M_\tau\mathbf{1}_D]=\mathbb{E}[M_\tau\mathbf{1}_{\Omega_0}\mathbf{1}_D]=\mathbb{E}[M_\sigma\mathbf{1}_{\Omega_0}\mathbf{1}_D]=\mathbb{E}[M_\sigma\mathbf{1}_D],

the outer equalities by the almost-sure-equality lemma and the middle one by (b). These are conditions (i)--(iii) of the definition of conditional expectation, so MσM_\sigma is a conditional expectation of MτM_\tau given Fσ\mathcal{F}_\sigma.

Step 4: the stopped process (claim (c)). Claims (a) and (b) are used here for arbitrary stopping times, as justified at the start of Step 1. Fix 0≤s≤t≤T0\le s\le t\le T and D∈FsD\in\mathcal{F}_s. Put σ′=min⁡(s,τ)\sigma'=\min(s,\tau) and τ′=min⁡(t,τ)\tau'=\min(t,\tau), stopping times by toolkit claim 1 with σ′≤τ′\sigma'\le\tau' pointwise, so that Msτ=Mσ′M^\tau_s=M_{\sigma'} and Mtτ=Mτ′M^\tau_t=M_{\tau'}. By Step 1 applied to σ′\sigma' and τ′\tau', both Mσ′1Ω0M_{\sigma'}\mathbf{1}_{\Omega_0} and Mτ′1Ω0M_{\tau'}\mathbf{1}_{\Omega_0} are random variables bounded by KK. Split DD into E1=D∩{τ≤s}E_1=D\cap\{\tau\le s\} and E2=D∩{τ>s}E_2=D\cap\{\tau>s\}; both lie in Fs\mathcal{F}_s ({τ≤s}\{\tau\le s\} by the definition of a stopping time, {τ>s}\{\tau>s\} by toolkit claim 1), so 1E1\mathbf{1}_{E_1} and 1E2\mathbf{1}_{E_2} are random variables and 1D=1E1+1E2\mathbf{1}_D=\mathbf{1}_{E_1}+\mathbf{1}_{E_2}. On E1E_1 we have min⁡(t,τ)=τ=min⁡(s,τ)\min(t,\tau)=\tau=\min(s,\tau), so Mτ′1Ω01E1=Mσ′1Ω01E1M_{\tau'}\mathbf{1}_{\Omega_0}\mathbf{1}_{E_1}=M_{\sigma'}\mathbf{1}_{\Omega_0}\mathbf{1}_{E_1} pointwise. By the splitting assertion of toolkit claim 2, E2∈Fσ′E_2\in\mathcal{F}_{\sigma'}, so claim (b) applied to the stopping times σ′≤τ′\sigma'\le\tau' and the event E2E_2 gives E[Mτ′1Ω01E2]=E[Mσ′1Ω01E2]\mathbb{E}[M_{\tau'}\mathbf{1}_{\Omega_0}\mathbf{1}_{E_2}]=\mathbb{E}[M_{\sigma'}\mathbf{1}_{\Omega_0}\mathbf{1}_{E_2}]. Adding the two contributions by linearity of the integral yields the identity of (c).

Suppose finally that every path of MM is right-continuous at every t∈[0,T)t\in[0,T). As in Step 1, MM is progressively measurable, so MτM^\tau is adapted by toolkit claim 4(i); ∣Mtτ(ω)∣=∣Mmin⁡(t,τ(ω))(ω)∣≤K|M^\tau_t(\omega)|=|M_{\min(t,\tau(\omega))}(\omega)|\le K for all t,ωt,\omega, so each MtτM^\tau_t is square-integrable; and for s≤ts\le t and D∈FsD\in\mathcal{F}_s the identity of (c) together with claim 2 of the almost-sure-equality lemma (applied on each side to remove the factor 1Ω0\mathbf{1}_{\Omega_0}) gives E[Mtτ1D]=E[Msτ1D]\mathbb{E}[M^\tau_t\mathbf{1}_D]=\mathbb{E}[M^\tau_s\mathbf{1}_D], the martingale property in averaged form. Thus MτM^\tau is a square-integrable martingale with respect to (Ft)t∈[0,T](\mathcal{F}_t)_{t\in[0,T]}, with time index restricted to [0,T][0,T]. By Step 0 every path of MM is right-continuous in the sequential sense, so by toolkit claim 4(iii) every path of MτM^\tau is right-continuous in the sequential sense, hence, by the converse direction of Step 0, right-continuous at every t∈[0,T)t\in[0,T) in the sense of the hypothesis. ■\blacksquare

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