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Proof of Uniqueness for the Forward Equation of a Bounded Jump-Rate Family on a Finite Set

lemmalem:finite-state-forward-equation-uniqueness-2026a
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Reason: Proof of the uniqueness lemma for the forward equation of a bounded jump-rate family on a finite set (Gronwall on the finite-dimensional difference).

Proof

Throughout, integrals over compact intervals are the Lebesgue integrals over the compact interval in question, and we use linearity and monotonicity of the integral freely for bounded measurable integrands on such intervals (such an integrand is integrable, the interval having finite measure by claim 1 of Restricted Lebesgue Measure and Integral Toolkit on a Compact Interval), including the bound ff\bigl|\int f\bigr|\le\int|f| of claim 2 of that theorem.

Step 1: the gap function. For t[r,T]t\in[r,T] put

d(t)=xEμt(x)νt(x).d(t)=\sum_{x\in E}\bigl|\mu_t(x)-\nu_t(x)\bigr|.

By condition (i) for μ\mu and ν\nu and by Arithmetic, Absolute Values, and Pointwise Limits of Measurable Real-Valued Functions (differences, absolute values, and finite sums of bounded measurable functions), dd is bounded and measurable on [r,T][r,T] with respect to B[r,T]\mathcal{B}_{[r,T]}, and d0d\ge0.

Step 2: the integral inequality. Fix yEy\in E and let 1y:ER\mathbf{1}_y:E\to\mathbb{R} be the function equal to 11 at yy and 00 elsewhere. From the definition of Lu\mathcal{L}_u,

Lu1y(x)=qu(x,y)  for xy,Lu1y(y)=zE,zyqu(y,z),\mathcal{L}_u\mathbf{1}_y(x)=q_u(x,y)\ \text{ for }x\neq y,\qquad \mathcal{L}_u\mathbf{1}_y(y)=-\sum_{z\in E,\,z\neq y}q_u(y,z),

so that Lu1y(x)Λ|\mathcal{L}_u\mathbf{1}_y(x)|\le\Lambda for all u[0,T]u\in[0,T] and xEx\in E, by the rate bound in the hypotheses (each qu(x,y)q_u(x,y) is nonnegative and at most the sum bounded by Λ\Lambda). Applying condition (ii) with F=1yF=\mathbf{1}_y to μ\mu and to ν\nu, using μr=νr\mu_r=\nu_r, and subtracting (linearity of the integral, both integrands being bounded and measurable), for every t[r,T]t\in[r,T],

μt(y)νt(y)=[r,t]xE(μu(x)νu(x))Lu1y(x)du.\mu_t(y)-\nu_t(y)=\int_{[r,t]}\sum_{x\in E}\bigl(\mu_u(x)-\nu_u(x)\bigr)\mathcal{L}_u\mathbf{1}_y(x)\,du .

The integrand is bounded in absolute value by Λd(u)\Lambda\,d(u), by Comparison and Absolute Value Bounds for Finite Sums of Real Numbers, so μt(y)νt(y)Λ[r,t]d(u)du|\mu_t(y)-\nu_t(y)|\le\Lambda\int_{[r,t]}d(u)\,du. Summing over the E|E| points yEy\in E (with E|E| the number of elements of EE) gives

d(t)EΛ[r,t]d(u)du(t[r,T]),d(t)\le|E|\Lambda\int_{[r,t]}d(u)\,du\qquad(t\in[r,T]),

where for t=rt=r both sides are 00.

Step 3: Gronwall. Define d0:[0,T]Rd^0:[0,T]\to\mathbb{R} by d0(t)=0d^0(t)=0 for t[0,r)t\in[0,r) and d0(t)=d(t)d^0(t)=d(t) for t[r,T]t\in[r,T]. Then d0d^0 is bounded and nonnegative, and it is measurable with respect to B[0,T]\mathcal{B}_{[0,T]}: for a real number a0a\ge0 the set {t[0,T]:d0(t)>a}={t[r,T]:d(t)>a}\{t\in[0,T]:d^0(t)>a\}=\{t\in[r,T]:d(t)>a\} belongs to B[r,T]\mathcal{B}_{[r,T]}, hence is a Borel set (claim 1 of Restricted Lebesgue Measure and Integral Toolkit on a Compact Interval) contained in [0,T][0,T], hence belongs to B[0,T]\mathcal{B}_{[0,T]}; for a<0a<0 the set is all of [0,T][0,T]; so d0d^0 is measurable by the generator criterion of Measurable Function and Real-Valued Measurable Function. For t(r,T]t\in(r,T], the zero extensions to R\mathbb{R} of the restriction of d0d^0 to [0,t][0,t] and of the restriction of dd to [r,t][r,t] are the same function on R\mathbb{R} (both vanish off [r,t][r,t] and agree with dd on [r,t][r,t]), so by claim 2 of Restricted Lebesgue Measure and Integral Toolkit on a Compact Interval, applied on [0,t][0,t] and on [r,t][r,t],

[0,t]d0(u)du=[r,t]d(u)du.\int_{[0,t]}d^0(u)\,du=\int_{[r,t]}d(u)\,du .

Combining with Step 2, d0(t)EΛ[0,t]d0(u)dud^0(t)\le|E|\Lambda\int_{[0,t]}d^0(u)\,du for t(r,T]t\in(r,T], and also for t=rt=r, where d0(r)=d(r)=0d^0(r)=d(r)=0 because μr=νr\mu_r=\nu_r while the right side is nonnegative; for t[0,r)t\in[0,r) the same inequality holds because its left side is 00 and its right side is the integral of a nonnegative function (monotonicity), or 00 when t=0t=0. Thus the hypotheses of Gronwall's lemma for bounded measurable functions hold on [0,T][0,T] with the function there taken to be d0d^0, its additive constant taken to be 00, and its multiplicative constant c=EΛc=|E|\Lambda, and it yields d0(t)0exp(ct)=0d^0(t)\le0\cdot\exp(ct)=0 for every t[0,T]t\in[0,T]. Since d00d^0\ge0, d(t)=0d(t)=0 for every t[r,T]t\in[r,T], that is, μt(x)=νt(x)\mu_t(x)=\nu_t(x) for every xEx\in E and every t[r,T]t\in[r,T].

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