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Proof of The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair

lemmalem:delta-envelopes-bounded-wasserstein-2026a
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· 5,615 chars · 13 deps · depth 33 Reason: Proof of the new envelope lemma for bounded functions and monotonicity in the weight.

Growth and the envelope bound follow from the lower bound of a coercive penalty and the bound clause of the envelope lemma; monotonicity follows because the upper envelope is the least upper semicontinuous majorant, and u minus delta' times the penalty lies below the upper semicontinuous function obtained from the delta-envelope by subtracting (delta'-delta) times the penalty. The lower statements follow by duality.

Proof

Each result cited is universally quantified over the data in its own statement, and is applied to the data named here. By Basic Properties of a Wasserstein-Coercive Penalty Pair §bounded-below fix e0Re_{0}\in\mathbb{R} with e0E(μ)e_{0}\le\mathcal{E}(\mu) for every μD\mu\in\mathcal{D}; by Basic Properties of a Wasserstein-Coercive Penalty Pair §lsc, E\mathcal{E} is lower semicontinuous on D\mathcal{D} relative to D\mathcal{D} in (P2(Rd),W2)(\mathcal{P}_{2}(\mathbb{R}^{d}),W_{2}). The set D\mathcal{D} contains the nonempty set DΣ\mathcal{D}_{\Sigma} (Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §pair, Penalty Pairs on the Wasserstein Space: the Penalty, Its Score, and Their Domains §nonempty), so it is nonempty. For positive δ\delta and μD\mu\in\mathcal{D}, multiplying e0E(μ)e_{0}\le\mathcal{E}(\mu) by the nonnegative δ\delta gives δe0δE(μ)\delta e_{0}\le\delta\,\mathcal{E}(\mu) (claim 5 of Elementary Arithmetic in an Ordered Field).

Claim 1. Suppose u(μ)bu(\mu)\le b for every μD\mu\in\mathcal{D}, and let δ\delta be positive. Put C=bδe0C=b-\delta e_{0}. For μD\mu\in\mathcal{D}, adding bδe0b-\delta e_{0} to both sides of δe0δE(μ)\delta e_{0}\le\delta\,\mathcal{E}(\mu) gives bC+δE(μ)b\le C+\delta\,\mathcal{E}(\mu), so u(μ)C+δE(μ)u(\mu)\le C+\delta\,\mathcal{E}(\mu). As δ\delta was arbitrary, uu has penalty-subordinate growth from above (Penalty-Subordinate Growth of a Function on the Penalty Domain §above). Suppose instead bu(μ)b\le u(\mu) for every μD\mu\in\mathcal{D}, and put C=bδe0C=-b-\delta e_{0}. For μD\mu\in\mathcal{D}, adding bδE(μ)b-\delta\,\mathcal{E}(\mu) to both sides of δe0δE(μ)\delta e_{0}\le\delta\,\mathcal{E}(\mu) gives CδE(μ)=b+δe0δE(μ)bu(μ)-C-\delta\,\mathcal{E}(\mu)=b+\delta e_{0}-\delta\,\mathcal{E}(\mu)\le b\le u(\mu), so uu has penalty-subordinate growth from below (Penalty-Subordinate Growth of a Function on the Penalty Domain §below).

Claim 2. Suppose u(μ)bu(\mu)\le b for every μD\mu\in\mathcal{D}. By Claim 1, uu has penalty-subordinate growth from above; since 0E(μ)=00\,\mathcal{E}(\mu)=0 (claim 1 of Zero Products and Elementary Identities in a Field), u(μ)b+0E(μ)u(\mu)\le b+0\,\mathcal{E}(\mu) for every μD\mu\in\mathcal{D}. Apply Basic Properties of the Delta-Envelopes on the Wasserstein Space §bound with C=bC=b and η=0\eta=0, for which 0ηδ0\le\eta\le\delta holds, E\mathcal{E} being lower semicontinuous on D\mathcal{D}: it gives uδ(μ)b(δ0)E(μ)=bδE(μ)u^{-}_{\delta}(\mu)\le b-(\delta-0)\,\mathcal{E}(\mu)=b-\delta\,\mathcal{E}(\mu) for every μD\mu\in\mathcal{D}. If instead bu(μ)b\le u(\mu) for every μD\mu\in\mathcal{D}, then uu has penalty-subordinate growth from below by Claim 1 and (b)0E(μ)=bu(μ)-(-b)-0\,\mathcal{E}(\mu)=b\le u(\mu); the second part of Basic Properties of the Delta-Envelopes on the Wasserstein Space §bound, with C=bC=-b and η=0\eta=0, gives b+δE(μ)uδ+(μ)b+\delta\,\mathcal{E}(\mu)\le u^{+}_{\delta}(\mu) for every μD\mu\in\mathcal{D}.

Claim 3, from above. Suppose uu has penalty-subordinate growth from above, and put κ=δδ\kappa=\delta'-\delta, positive by claim 1 of Elementary Order Arithmetic in an Ordered Field. The function E-\mathcal{E} on D\mathcal{D}, with value E(ν)-\mathcal{E}(\nu) at ν\nu, is upper semicontinuous on D\mathcal{D} relative to D\mathcal{D}: given νD\nu\in\mathcal{D} and a positive ε\varepsilon, the lower semicontinuity of E\mathcal{E} at ν\nu provides a positive radius within which E(ν)ε<E(ν)\mathcal{E}(\nu)-\varepsilon<\mathcal{E}(\nu'), which is E(ν)<E(ν)+ε-\mathcal{E}(\nu')<-\mathcal{E}(\nu)+\varepsilon by claim 4 of Elementary Order Arithmetic in an Ordered Field. By Basic Properties of the Delta-Envelopes on the Wasserstein Space §semicontinuity, uδu^{-}_{\delta} is upper semicontinuous on D\mathcal{D} and

u(ν)δE(ν)uδ(ν)(νD).u(\nu)-\delta\,\mathcal{E}(\nu)\le u^{-}_{\delta}(\nu)\qquad(\nu\in\mathcal{D}).

Let h:DRh:\mathcal{D}\to\mathbb{R} have value h(ν)=uδ(ν)+κ(E(ν))=uδ(ν)κE(ν)h(\nu)=u^{-}_{\delta}(\nu)+\kappa\bigl(-\mathcal{E}(\nu)\bigr)=u^{-}_{\delta}(\nu)-\kappa\,\mathcal{E}(\nu). By claims 2 and 1 of Sums and Nonnegative Multiples of Semicontinuous Functions, applied at every point of D\mathcal{D} with the nonnegative multiplier κ\kappa, hh is upper semicontinuous on D\mathcal{D} relative to D\mathcal{D}. For νD\nu\in\mathcal{D}, adding κE(ν)-\kappa\,\mathcal{E}(\nu) to both sides of the last display gives

u(ν)δE(ν)=(u(ν)δE(ν))κE(ν)h(ν).u(\nu)-\delta'\,\mathcal{E}(\nu)=\bigl(u(\nu)-\delta\,\mathcal{E}(\nu)\bigr)-\kappa\,\mathcal{E}(\nu)\le h(\nu).

The function uδEu-\delta'\mathcal{E} is bounded above near each point of D\mathcal{D} and uδu^{-}_{\delta'} is its upper semicontinuous envelope, by The Delta-Envelopes of a Function on the Penalty Domain Relative to a Penalty Pair §minus read with δ\delta'. So Properties of the Upper Semicontinuous Envelope §least, in the metric space (P2(Rd),W2)(\mathcal{P}_{2}(\mathbb{R}^{d}),W_{2}) with the nonempty subset D\mathcal{D}, the function uδEu-\delta'\mathcal{E} and the upper semicontinuous majorant hh, gives uδ(μ)h(μ)=uδ(μ)κE(μ)u^{-}_{\delta'}(\mu)\le h(\mu)=u^{-}_{\delta}(\mu)-\kappa\,\mathcal{E}(\mu) for every μD\mu\in\mathcal{D}; adding κE(μ)\kappa\,\mathcal{E}(\mu) to both sides is the claim.

Claim 3, from below. Suppose uu has penalty-subordinate growth from below. By Basic Properties of the Delta-Envelopes on the Wasserstein Space §duality, u-u has penalty-subordinate growth from above, (u)δ=uδ+(-u)^{-}_{\delta}=-u^{+}_{\delta} and (u)δ=uδ+(-u)^{-}_{\delta'}=-u^{+}_{\delta'} on D\mathcal{D}. The part from above, applied to u-u, gives uδ+(μ)+κE(μ)uδ+(μ)-u^{+}_{\delta'}(\mu)+\kappa\,\mathcal{E}(\mu)\le-u^{+}_{\delta}(\mu) for every μD\mu\in\mathcal{D}; adding uδ+(μ)+uδ+(μ)κE(μ)u^{+}_{\delta}(\mu)+u^{+}_{\delta'}(\mu)-\kappa\,\mathcal{E}(\mu) to both sides gives uδ+(μ)uδ+(μ)κE(μ)u^{+}_{\delta}(\mu)\le u^{+}_{\delta'}(\mu)-\kappa\,\mathcal{E}(\mu).

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