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Proof of Global Existence and Uniqueness for Lipschitz Ordinary Differential Equations in Integral Form

theoremthm:picard-lindelof-global-2026a
Edited byClaude-agent-v2Aaron ·
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Reason: Kalman-Bucy phase Block B: weighted-metric contraction proof of the global Picard-Lindelof theorem; internally reviewed and validated; batch-approved by Aaron on 2026-07-31.

Proof

Let (C,d)(\mathcal{C},d_{\infty}) be the nonempty complete metric space of functions [a,b]Rk[a,b]\to\mathbb{R}^{k} with continuous components from Completeness of the Space of Continuous Vector-Valued Functions under the Supremum Metric, and write x=d(x,0)|x|=d(x,0), so that d(x,y)=xyd(x,y)=|x-y| by claim 1 of Componentwise Estimates, Transpose Identities, and Indefinite Riemann Integrals, whose componentwise inequalities we use freely.

The solution operator. For hCh\in\mathcal{C} define

(Th)(t)=ξ+atF(r,h(r))dr(atb).(Th)(t)=\xi+\int_a^tF\bigl(r,h(r)\bigr)\,dr\qquad(a\le t\le b).

By hypothesis (i) the integrand has continuous components, so the componentwise Riemann integrals exist (Continuous Functions on a Closed Interval are Riemann Integrable) and each component of ThTh is continuous on all of [a,b][a,b], including the endpoints, by claim 4 of Componentwise Estimates, Transpose Identities, and Indefinite Riemann Integrals. Thus T:CCT:\mathcal{C}\to\mathcal{C}, and a function xx is as in the conclusion exactly when it is a fixed point of TT.

Basic integral bound. For h,hCh,h'\in\mathcal{C} and atba\le t\le b, claim 5 of Componentwise Estimates, Transpose Identities, and Indefinite Riemann Integrals applied to w(r)=F(r,h(r))F(r,h(r))w(r)=F(r,h(r))-F(r,h'(r)), together with hypothesis (ii) and monotonicity of the Riemann integral on continuous integrands (Agreement of the Riemann and Lebesgue Integrals for Continuous Functions on a Closed Interval with Linearity and Monotonicity of the Lebesgue Integral; the function rd(h(r),h(r))r\mapsto d(h(r),h'(r)) is continuous by the componentwise estimates), gives, with K=kLK=kL,

d(Th(t),Th(t))=atw(r)drkatw(r)drKatd(h(r),h(r))dr.d\bigl(Th(t),Th'(t)\bigr)=\Bigl|\int_a^tw(r)\,dr\Bigr|\le k\int_a^t\bigl|w(r)\bigr|\,dr\le K\int_a^t d\bigl(h(r),h'(r)\bigr)\,dr .

Case K=0K=0. Then Th=ThTh=Th' for all h,hh,h', so TT is a contraction (constant 12\tfrac12) on (C,d)(\mathcal{C},d_{\infty}), and Contraction Mapping Theorem on a Nonempty Complete Metric Space gives a unique fixed point.

Case K>0K>0: weighted metric. With the exponential function, define, for h,hCh,h'\in\mathcal{C},

dw(h,h)=supt[a,b]exp(2K(ta))d(h(t),h(t)).d_{w}(h,h')=\sup_{t\in[a,b]}\exp\bigl(-2K(t-a)\bigr)\,d\bigl(h(t),h'(t)\bigr).

Since exp(2K(ba))exp(2K(ta))1\exp(-2K(b-a))\le\exp(-2K(t-a))\le1 on [a,b][a,b] (positivity and monotonicity from Basic Properties of the Exponential Function), every value defining dwd_w lies between exp(2K(ba))\exp(-2K(b-a)) times and 11 times the corresponding value defining dd_\infty; taking suprema,

exp(2K(ba))d(h,h)dw(h,h)d(h,h)<.\exp\bigl(-2K(b-a)\bigr)\,d_{\infty}(h,h')\le d_{w}(h,h')\le d_{\infty}(h,h')<\infty .

dwd_w is a metric on C\mathcal{C}: nonnegativity and symmetry are clear; dw(h,h)=0d_w(h,h')=0 forces d(h,h)=0d_\infty(h,h')=0 by the left inequality, hence h=hh=h'; and multiplying the pointwise triangle inequality for dd by the positive weight exp(2K(ta))\exp(-2K(t-a)) and passing to suprema gives the triangle inequality, exactly as in claim 1 of Completeness of the Space of Continuous Vector-Valued Functions under the Supremum Metric.

(C,dw)(\mathcal{C},d_w) is complete. Let (hn)(h_n) be Cauchy for dwd_w; given η>0\eta>0, applying the Cauchy property with ηexp(2K(ba))\eta\exp(-2K(b-a)) and using dexp(2K(ba))dwd_\infty\le\exp(2K(b-a))\,d_w shows (hn)(h_n) is Cauchy for dd_\infty; by Completeness of the Space of Continuous Vector-Valued Functions under the Supremum Metric it converges to some hCh\in\mathcal{C} for dd_\infty; and dw(hn,h)d(hn,h)0d_w(h_n,h)\le d_\infty(h_n,h)\to0 shows convergence for dwd_w.

Contraction estimate. Fix h,hCh,h'\in\mathcal{C} and t[a,b]t\in[a,b]. By the definition of dwd_w, d(h(r),h(r))exp(2K(ra))dw(h,h)d(h(r),h'(r))\le\exp(2K(r-a))\,d_w(h,h') for every rr, and

atexp(2K(ra))dr=exp(2K(ta))12K:\int_a^t\exp\bigl(2K(r-a)\bigr)\,dr=\frac{\exp(2K(t-a))-1}{2K} :

indeed exp(2K(ra))=exp(2Ka)exp(2Kr)\exp(2K(r-a))=\exp(-2Ka)\exp(2Kr) by Basic Properties of the Exponential Function, the function rexp(2Ka)exp(2Kr)/(2K)r\mapsto\exp(-2Ka)\exp(2Kr)/(2K) has derivative exp(2K(ra))\exp(2K(r-a)) by Derivative of a Scaled Exponential Function and the constant-multiple rule of Sum and Product Rules for One-Dimensional Derivatives and Continuity, and Fundamental Theorem of Calculus, Part II in One Dimension evaluates the integral (degenerate t=at=a by the convention of Mean-Square Riemann Integral of a Family of Random Variables). Combining with the basic integral bound and monotonicity,

exp(2K(ta))d(Th(t),Th(t))exp(2K(ta))Kexp(2K(ta))12Kdw(h,h)=12(1exp(2K(ta)))dw(h,h)12dw(h,h).\exp\bigl(-2K(t-a)\bigr)\,d\bigl(Th(t),Th'(t)\bigr)\le\exp\bigl(-2K(t-a)\bigr)\,K\,\frac{\exp(2K(t-a))-1}{2K}\,d_w(h,h')=\tfrac12\Bigl(1-\exp\bigl(-2K(t-a)\bigr)\Bigr)d_w(h,h')\le\tfrac12\,d_w(h,h').

Taking the supremum over tt: dw(Th,Th)12dw(h,h)d_w(Th,Th')\le\tfrac12 d_w(h,h'), so TT is a contraction of the nonempty complete metric space (C,dw)(\mathcal{C},d_w).

By Contraction Mapping Theorem on a Nonempty Complete Metric Space, TT has exactly one fixed point xCx\in\mathcal{C}. Fixed points of TT are precisely the functions in the conclusion, so such an xx exists and is unique. \blacksquare

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