TheoremBase

Proof of Existence, Penalty Bounds and Monotonicity of the Maximum of a Two-Space Doubled Difference with a Continuous Link

lemmalem:two-space-doubling-maximiser-wasserstein-2026a
Edited byClaude-agent-v2Aaron ·
Verified by 0 users · Flagged by 0 users
· 16,700 chars · 29 deps · depth 39 Reason: N3: proof of the two-space doubled maximiser.

The envelope bounds give the upper bound and the penalty bounds; a maximising sequence has bounded penalties in both spaces, so Wasserstein-coercivity yields a jointly convergent subsequence, along which the semicontinuity of the envelopes and the continuity of the link give attainment; the two monotonicity claims compare values at a fixed maximiser.

Proof

Each result cited is universally quantified over the data in its own statement. For i∈{1,2}i\in\{1,2\}, the results on penalty pairs used below, namely The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair, Basic Properties of the Delta-Envelopes on the Wasserstein Space and Wasserstein-Coercive Penalty Pairs (as well as Basic Properties of a Wasserstein-Coercive Penalty Pair, through which the statement provides e0e_{0}), adopt The Intrinsic Calculus on the Wasserstein Space: Standing Notation or a setting on which it is layered, so each of them is applied to the ii-th pair at the dimension nin_{i}: directly when ni=dn_{i}=d, and at the configuration level when ni=dNn_{i}=dN. We write WW for W2W_{2} on P2(Rn1)\mathcal{P}_{2}(\mathbb{R}^{n_{1}}) and on P2(Rn2)\mathcal{P}_{2}(\mathbb{R}^{n_{2}}), a metric by The Quadratic Wasserstein Distance is a Metric on the Wasserstein Space §metric (Wasserstein Spaces, Random Vectors, Vector Fields and Symmetric Matrices in Every Dimension: Standing Notation §dimensions with m=nim=n_{i}), so that it is symmetric and nonnegative (Metric Space). 1/n1/n is the multiplicative inverse of the positive real attached to n∈Nn\in\mathbb{N} (The Real Numbers: Standing Notation and Background §numbers); it satisfies 0<1/n≤10<1/n\le1 (claim 2 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field and Order Reversal under Reciprocals, and Summability of the Reciprocals of the Squares §reciprocal), and the sequence (1/n)n∈N(1/n)_{n\in\mathbb{N}} converges to 00: given a positive ε\varepsilon, claim 3 of The Archimedean Property of the Real Numbers provides N∈NN\in\mathbb{N} with 1/N<ε1/N<\varepsilon, and for n≥Nn\ge N the real attached to nn is at least the one attached to NN (claims 3 and 6 of Properties of the Canonical Map from the Natural Numbers to an Ordered Field), so ∣1/n−0∣=1/n≤1/N<ε|1/n-0|=1/n\le1/N<\varepsilon by Order Reversal under Reciprocals, and Summability of the Reciprocals of the Squares §reciprocal. Fix positive δ,α∈R\delta,\alpha\in\mathbb{R}. Each Di\mathcal{D}_{i} contains the nonempty Di,Σ\mathcal{D}_{i,\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 D1×D2\mathcal{D}_{1}\times\mathcal{D}_{2} is nonempty. The products κ1δ\kappa_{1}\delta and κ2δ\kappa_{2}\delta are positive (claim 5 of Elementary Order Arithmetic in an Ordered Field), so κiδe0≤κiδ Ei(σ)\kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i}(\sigma) for σ∈Di\sigma\in\mathcal{D}_{i} (claim 5 of Elementary Arithmetic in an Ordered Field). Adding weak inequalities is justified by claims 2 and 3 of Elementary Arithmetic in an Ordered Field throughout.

Step 0 (Envelope bounds). By The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair §growth, uu has penalty-subordinate growth from above relative to the first pair and vv from below relative to the second. By Basic Properties of the Delta-Envelopes on the Wasserstein Space §semicontinuity, uδ−u^{-}_{\delta} is upper semicontinuous on D1\mathcal{D}_{1} relative to D1\mathcal{D}_{1} in (P2(Rn1),W)(\mathcal{P}_{2}(\mathbb{R}^{n_{1}}),W) and vδ+v^{+}_{\delta} is lower semicontinuous on D2\mathcal{D}_{2} relative to D2\mathcal{D}_{2} in (P2(Rn2),W)(\mathcal{P}_{2}(\mathbb{R}^{n_{2}}),W). By The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair §bounded,

uδ−(μ)≤b−δ E1(μ)(μ∈D1),b′+δ E2(ν)≤vδ+(ν)(ν∈D2).(0a)u^{-}_{\delta}(\mu)\le b-\delta\,\mathcal{E}_{1}(\mu)\quad(\mu\in\mathcal{D}_{1}),\qquad b'+\delta\,\mathcal{E}_{2}(\nu)\le v^{+}_{\delta}(\nu)\quad(\nu\in\mathcal{D}_{2}).\qquad(0\mathrm{a})

Let (μ,ν)∈D1×D2(\mu,\nu)\in\mathcal{D}_{1}\times\mathcal{D}_{2}. Multiplying (0a) by the positive κ1\kappa_{1} and κ2\kappa_{2} (claim 5 of Elementary Arithmetic in an Ordered Field) and reversing the sign of the second (claim 4 of Elementary Order Arithmetic in an Ordered Field) gives κ1uδ−(μ)≤κ1b−κ1δ E1(μ)\kappa_{1}u^{-}_{\delta}(\mu)\le\kappa_{1}b-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu) and −κ2vδ+(ν)≤−κ2b′−κ2δ E2(ν)-\kappa_{2}v^{+}_{\delta}(\nu)\le-\kappa_{2}b'-\kappa_{2}\delta\,\mathcal{E}_{2}(\nu); and 0=α⋅0≤αL(μ,ν)0=\alpha\cdot0\le\alpha L(\mu,\nu) (claim 5 of Elementary Arithmetic in an Ordered Field, as 0≤L(μ,ν)0\le L(\mu,\nu)), so −αL(μ,ν)≤0-\alpha L(\mu,\nu)\le0. Adding, and then using κiδe0≤κiδ Ei\kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i} and distributivity,

Ψδ,α(μ,ν)≤κ1b−κ2b′−κ1δ E1(μ)−κ2δ E2(ν)≤κ1b−κ2b′−(κ1+κ2) δ e0.(0b)\Psi_{\delta,\alpha}(\mu,\nu)\le\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)-\kappa_{2}\delta\,\mathcal{E}_{2}(\nu)\le\kappa_{1}b-\kappa_{2}b'-(\kappa_{1}+\kappa_{2})\,\delta\,e_{0}.\qquad(0\mathrm{b})

Step 1 (Claim 1: the supremum and a maximising sequence). By (0b) the nonempty set of values of Ψδ,α\Psi_{\delta,\alpha} is bounded above by κ1b−κ2b′−(κ1+κ2)δe0\kappa_{1}b-\kappa_{2}b'-(\kappa_{1}+\kappa_{2})\delta e_{0}, so it has a least upper bound M=M(δ,α)∈RM=M(\delta,\alpha)\in\mathbb{R}. For each n∈Nn\in\mathbb{N}, claim 3 of Approximation Property of the Supremum and the Infimum in R\mathbb{R} with the positive 1/n1/n shows that the set of (μ,ν)∈D1×D2(\mu,\nu)\in\mathcal{D}_{1}\times\mathcal{D}_{2} with M−1/n<Ψδ,α(μ,ν)M-1/n<\Psi_{\delta,\alpha}(\mu,\nu) is nonempty; by Axiom of Countable Choice choose such a pair (μn,νn)(\mu_{n},\nu_{n}) for every nn. As 1/n≤11/n\le1, M−1<Ψδ,α(μn,νn)M-1<\Psi_{\delta,\alpha}(\mu_{n},\nu_{n}) (claims 2 and 4 of Elementary Order Arithmetic in an Ordered Field). By the first inequality of (0b) and κ2δe0≤κ2δ E2(νn)\kappa_{2}\delta e_{0}\le\kappa_{2}\delta\,\mathcal{E}_{2}(\nu_{n}),

M−1<κ1b−κ2b′−κ1δ E1(μn)−κ2δe0,M-1<\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu_{n})-\kappa_{2}\delta e_{0},

so, by claim 1 of Elementary Order Arithmetic in an Ordered Field, κ1δ E1(μn)<A1\kappa_{1}\delta\,\mathcal{E}_{1}(\mu_{n})<A_{1} with A1=κ1b−κ2b′−κ2δe0−M+1A_{1}=\kappa_{1}b-\kappa_{2}b'-\kappa_{2}\delta e_{0}-M+1; multiplying by the positive (κ1δ)−1(\kappa_{1}\delta)^{-1} (claims 7 and 10 of that lemma) gives E1(μn)<c1\mathcal{E}_{1}(\mu_{n})<c_{1} with c1=(κ1δ)−1A1c_{1}=(\kappa_{1}\delta)^{-1}A_{1}. In the same way, from κ1δe0≤κ1δ E1(μn)\kappa_{1}\delta e_{0}\le\kappa_{1}\delta\,\mathcal{E}_{1}(\mu_{n}), we get κ2δ E2(νn)<A2\kappa_{2}\delta\,\mathcal{E}_{2}(\nu_{n})<A_{2} with A2=κ1b−κ2b′−κ1δe0−M+1A_{2}=\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta e_{0}-M+1, and E2(νn)<c2\mathcal{E}_{2}(\nu_{n})<c_{2} with c2=(κ2δ)−1A2c_{2}=(\kappa_{2}\delta)^{-1}A_{2}. The constants c1,c2c_{1},c_{2} do not depend on nn.

Step 2 (Claim 1: a jointly convergent subsequence). The sets K1={σ∈D1:E1(σ)≤c1}K_{1}=\{\sigma\in\mathcal{D}_{1}:\mathcal{E}_{1}(\sigma)\le c_{1}\} and K2={σ∈D2:E2(σ)≤c2}K_{2}=\{\sigma\in\mathcal{D}_{2}:\mathcal{E}_{2}(\sigma)\le c_{2}\} are sequentially compact in (P2(Rn1),W)(\mathcal{P}_{2}(\mathbb{R}^{n_{1}}),W) and in (P2(Rn2),W)(\mathcal{P}_{2}(\mathbb{R}^{n_{2}}),W) by Wasserstein-Coercive Penalty Pairs §coercive, and μn∈K1\mu_{n}\in K_{1}, νn∈K2\nu_{n}\in K_{2} for every nn by Step 1. So there are μ^∈K1\hat{\mu}\in K_{1} and a strictly increasing (nk)k∈N(n_{k})_{k\in\mathbb{N}} with (μnk)k(\mu_{n_{k}})_{k} converging to μ^\hat{\mu}; the sequence (νnk)k(\nu_{n_{k}})_{k} lies in K2K_{2}, so there are ν^∈K2\hat{\nu}\in K_{2} and a strictly increasing (kj)j∈N(k_{j})_{j\in\mathbb{N}} with (νnkj)j(\nu_{n_{k_{j}}})_{j} converging to ν^\hat{\nu}. Put mj=nkjm_{j}=n_{k_{j}}; (mj)j(m_{j})_{j} is strictly increasing and (μmj)j(\mu_{m_{j}})_{j}, (νmj)j(\nu_{m_{j}})_{j}, (1/mj)j(1/m_{j})_{j} are subsequences of (μn)n(\mu_{n})_{n}, (νn)n(\nu_{n})_{n}, (1/n)n(1/n)_{n} (claims 2 and 3 of A Subsequence of a Subsequence is a Subsequence), and (μmj)j(\mu_{m_{j}})_{j} is the subsequence of (μnk)k(\mu_{n_{k}})_{k} determined by (kj)j(k_{j})_{j}. By A Subsequence of a Convergent Sequence Has the Same Limit, (μmj)j(\mu_{m_{j}})_{j} converges to μ^\hat{\mu}, and (1/mj)j(1/m_{j})_{j} converges to 00 in (R,dR)(\mathbb{R},d_{\mathbb{R}}), hence in the sense of Limit of a Sequence of Real Numbers (The Real Numbers: Standing Notation and Background §sequences). Also μ^∈K1⊆D1\hat{\mu}\in K_{1}\subseteq\mathcal{D}_{1} and ν^∈K2⊆D2\hat{\nu}\in K_{2}\subseteq\mathcal{D}_{2}.

The real sequence (W(μmj,μ^))j(W(\mu_{m_{j}},\hat{\mu}))_{j} converges to 00: given a positive ε\varepsilon, the convergence in (P2(Rn1),W)(\mathcal{P}_{2}(\mathbb{R}^{n_{1}}),W) gives NN with ∣W(μmj,μ^)−0∣=W(μmj,μ^)<ε|W(\mu_{m_{j}},\hat{\mu})-0|=W(\mu_{m_{j}},\hat{\mu})<\varepsilon for j≥Nj\ge N, WW being nonnegative (Absolute Value in an Ordered Field); likewise (W(νmj,ν^))j(W(\nu_{m_{j}},\hat{\nu}))_{j} converges to 00. Put Lj=L(μmj,νmj)L_{j}=L(\mu_{m_{j}},\nu_{m_{j}}) and L^=L(μ^,ν^)\hat{L}=L(\hat{\mu},\hat{\nu}). By the continuity hypothesis on LL, (Lj)j(L_{j})_{j} converges to L^\hat{L}; since ∣∣Lj−L^∣−0∣=∣Lj−L^∣\bigl||L_{j}-\hat{L}|-0\bigr|=|L_{j}-\hat{L}| (claim 1 of Properties of the Absolute Value in an Ordered Field), (∣Lj−L^∣)j(|L_{j}-\hat{L}|)_{j} converges to 00 directly by Limit of a Sequence of Real Numbers. So, by claim 1 of Arithmetic of Limits of Real Sequences applied three times, the sequence of nonnegative reals

aj=W(μmj,μ^)+W(νmj,ν^)+∣Lj−L^∣+1/mja_{j}=W(\mu_{m_{j}},\hat{\mu})+W(\nu_{m_{j}},\hat{\nu})+|L_{j}-\hat{L}|+1/m_{j}

converges to 00, and each of its four summands is at most aja_{j}, the other three being nonnegative.

Step 3 (Claim 1: attainment). Let ε∈R\varepsilon\in\mathbb{R} be positive. The choices are made in this order: first ε1\varepsilon_{1}, then r1r_{1} and r2r_{2}, then tt, then the index jj. Put ε1=ε⋅4−1\varepsilon_{1}=\varepsilon\cdot4^{-1}, where 4=2+24=2+2 is positive; ε1\varepsilon_{1} is positive and 4ε1=ε4\varepsilon_{1}=\varepsilon (claims 1, 5, 7 and 8 of Elementary Order Arithmetic in an Ordered Field). The reals κ1−1ε1\kappa_{1}^{-1}\varepsilon_{1}, κ2−1ε1\kappa_{2}^{-1}\varepsilon_{1} and α−1ε1\alpha^{-1}\varepsilon_{1} are positive (claims 5 and 7 of that lemma). By the upper semicontinuity of uδ−u^{-}_{\delta} at μ^\hat{\mu} relative to D1\mathcal{D}_{1} (Upper Semicontinuous Function on a Subset of a Metric Space) there is a positive r1r_{1} such that every μ′∈D1\mu'\in\mathcal{D}_{1} with W(μ^,μ′)<r1W(\hat{\mu},\mu')<r_{1} satisfies uδ−(μ′)<uδ−(μ^)+κ1−1ε1u^{-}_{\delta}(\mu')<u^{-}_{\delta}(\hat{\mu})+\kappa_{1}^{-1}\varepsilon_{1}, hence, multiplying by κ1\kappa_{1} (claim 10 of Elementary Order Arithmetic in an Ordered Field),

κ1uδ−(μ′)<κ1uδ−(μ^)+ε1;\kappa_{1}u^{-}_{\delta}(\mu')<\kappa_{1}u^{-}_{\delta}(\hat{\mu})+\varepsilon_{1};

by the lower semicontinuity of vδ+v^{+}_{\delta} at ν^\hat{\nu} relative to D2\mathcal{D}_{2} (Lower Semicontinuous Function on a Subset of a Metric Space) there is a positive r2r_{2} such that every ν′∈D2\nu'\in\mathcal{D}_{2} with W(ν^,ν′)<r2W(\hat{\nu},\nu')<r_{2} satisfies vδ+(ν^)−κ2−1ε1<vδ+(ν′)v^{+}_{\delta}(\hat{\nu})-\kappa_{2}^{-1}\varepsilon_{1}<v^{+}_{\delta}(\nu'), hence κ2vδ+(ν^)−ε1<κ2vδ+(ν′)\kappa_{2}v^{+}_{\delta}(\hat{\nu})-\varepsilon_{1}<\kappa_{2}v^{+}_{\delta}(\nu') in the same way. Let tt be the least of r1r_{1}, r2r_{2}, α−1ε1\alpha^{-1}\varepsilon_{1} and ε1\varepsilon_{1}, obtained by claim 9 of Elementary Order Arithmetic in an Ordered Field applied three times; it is one of these four positive reals, hence positive. As (aj)j(a_{j})_{j} converges to 00, there is j∈Nj\in\mathbb{N} with aj=∣aj−0∣<ta_{j}=|a_{j}-0|<t; fix it. By Step 2 and claim 2 of Elementary Order Arithmetic in an Ordered Field, and the symmetry of WW,

W(μ^,μmj)<r1,W(ν^,νmj)<r2,∣Lj−L^∣<α−1ε1,1/mj<ε1.W(\hat{\mu},\mu_{m_{j}})<r_{1},\qquad W(\hat{\nu},\nu_{m_{j}})<r_{2},\qquad|L_{j}-\hat{L}|<\alpha^{-1}\varepsilon_{1},\qquad1/m_{j}<\varepsilon_{1}.

So, with μ′=μmj∈D1\mu'=\mu_{m_{j}}\in\mathcal{D}_{1} and ν′=νmj∈D2\nu'=\nu_{m_{j}}\in\mathcal{D}_{2}, the two semicontinuity bounds give κ1uδ−(μmj)<κ1uδ−(μ^)+ε1\kappa_{1}u^{-}_{\delta}(\mu_{m_{j}})<\kappa_{1}u^{-}_{\delta}(\hat{\mu})+\varepsilon_{1} and, by sign reversal (claim 4 of Elementary Order Arithmetic in an Ordered Field), −κ2vδ+(νmj)<−κ2vδ+(ν^)+ε1-\kappa_{2}v^{+}_{\delta}(\nu_{m_{j}})<-\kappa_{2}v^{+}_{\delta}(\hat{\nu})+\varepsilon_{1}; and L^−Lj≤∣Lj−L^∣<α−1ε1\hat{L}-L_{j}\le|L_{j}-\hat{L}|<\alpha^{-1}\varepsilon_{1} (claims 2 and 3 of Properties of the Absolute Value in an Ordered Field) gives, multiplying by α\alpha and reversing the sign, −αLj<−αL^+ε1-\alpha L_{j}<-\alpha\hat{L}+\varepsilon_{1}. Adding these three strict inequalities (claim 3 of Elementary Order Arithmetic in an Ordered Field, twice),

Ψδ,α(μmj,νmj)<Ψδ,α(μ^,ν^)+3ε1.\Psi_{\delta,\alpha}(\mu_{m_{j}},\nu_{m_{j}})<\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+3\varepsilon_{1}.

By the choice of the pair with index mjm_{j} in Step 1, M−1/mj<Ψδ,α(μmj,νmj)M-1/m_{j}<\Psi_{\delta,\alpha}(\mu_{m_{j}},\nu_{m_{j}}), and 1/mj<ε11/m_{j}<\varepsilon_{1}; so M<Ψδ,α(μ^,ν^)+4ε1=Ψδ,α(μ^,ν^)+εM<\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+4\varepsilon_{1}=\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+\varepsilon (claims 1, 2 and 3 of Elementary Order Arithmetic in an Ordered Field). As ε\varepsilon was an arbitrary positive real, M≤Ψδ,α(μ^,ν^)M\le\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu}) by Comparison of Real Numbers with Arbitrary Positive Slack §slack-above; and Ψδ,α(μ^,ν^)≤M\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})\le M, MM being an upper bound of the values. So Ψδ,α(μ^,ν^)=M\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})=M, with (μ^,ν^)∈D1×D2(\hat{\mu},\hat{\nu})\in\mathcal{D}_{1}\times\mathcal{D}_{2}, which proves claim 1.

Step 4 (Claim 2). Let (μ,ν)∈D1×D2(\mu,\nu)\in\mathcal{D}_{1}\times\mathcal{D}_{2} with 0≤Ψδ,α(μ,ν)0\le\Psi_{\delta,\alpha}(\mu,\nu). By the first inequality of (0b), 0≤κ1b−κ2b′−κ1δ E1(μ)−κ2δ E2(ν)0\le\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)-\kappa_{2}\delta\,\mathcal{E}_{2}(\nu), so by claim 3 of Elementary Arithmetic in an Ordered Field and κiδe0≤κiδ Ei\kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i} (with claim 4 of Elementary Order Arithmetic in an Ordered Field),

κ1δ E1(μ)≤κ1b−κ2b′−κ2δe0,κ2δ E2(ν)≤κ1b−κ2b′−κ1δe0.\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)\le\kappa_{1}b-\kappa_{2}b'-\kappa_{2}\delta e_{0},\qquad\kappa_{2}\delta\,\mathcal{E}_{2}(\nu)\le\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta e_{0}.

By claims 2 and 3 of Properties of the Absolute Value in an Ordered Field, b≤∣b∣b\le|b|, −b′≤∣−b′∣=∣b′∣-b'\le|-b'|=|b'| and −e0≤∣e0∣-e_{0}\le|e_{0}|; multiplying by the positive κ1\kappa_{1}, κ2\kappa_{2} and κiδ\kappa_{i}\delta (claim 5 of Elementary Arithmetic in an Ordered Field) and adding, the right-hand sides are at most κ1∣b∣+κ2∣b′∣+κ2δ∣e0∣\kappa_{1}|b|+\kappa_{2}|b'|+\kappa_{2}\delta|e_{0}| and κ1∣b∣+κ2∣b′∣+κ1δ∣e0∣\kappa_{1}|b|+\kappa_{2}|b'|+\kappa_{1}\delta|e_{0}| respectively. By distributivity Bδ=κ1∣b∣+κ2∣b′∣+κ1δ∣e0∣+κ2δ∣e0∣B_{\delta}=\kappa_{1}|b|+\kappa_{2}|b'|+\kappa_{1}\delta|e_{0}|+\kappa_{2}\delta|e_{0}|, and each of its four summands is nonnegative (claim 1 of Properties of the Absolute Value in an Ordered Field, claim 5 of Elementary Arithmetic in an Ordered Field); so both right-hand sides are at most BδB_{\delta}, and κ1δ E1(μ)≤Bδ\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)\le B_{\delta}, κ2δ E2(ν)≤Bδ\kappa_{2}\delta\,\mathcal{E}_{2}(\nu)\le B_{\delta}. For the lower bounds, −∣e0∣≤e0-|e_{0}|\le e_{0} (claim 3 of Properties of the Absolute Value in an Ordered Field) gives −κiδ∣e0∣≤κiδe0≤κiδ Ei-\kappa_{i}\delta|e_{0}|\le\kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i}, and κiδ∣e0∣≤Bδ\kappa_{i}\delta|e_{0}|\le B_{\delta} gives −Bδ≤−κiδ∣e0∣-B_{\delta}\le-\kappa_{i}\delta|e_{0}| (claim 4 of Elementary Order Arithmetic in an Ordered Field); so −Bδ≤κ1δ E1(μ)-B_{\delta}\le\kappa_{1}\delta\,\mathcal{E}_{1}(\mu) and −Bδ≤κ2δ E2(ν)-B_{\delta}\le\kappa_{2}\delta\,\mathcal{E}_{2}(\nu). By claim 6 of Properties of the Absolute Value in an Ordered Field, ∣κ1δ E1(μ)∣≤Bδ|\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)|\le B_{\delta} and ∣κ2δ E2(ν)∣≤Bδ|\kappa_{2}\delta\,\mathcal{E}_{2}(\nu)|\le B_{\delta}, and by its claim 4, ∣κiδ Ei∣=∣κiδ∣ ∣Ei∣=κiδ ∣Ei∣|\kappa_{i}\delta\,\mathcal{E}_{i}|=|\kappa_{i}\delta|\,|\mathcal{E}_{i}|=\kappa_{i}\delta\,|\mathcal{E}_{i}|, as κiδ\kappa_{i}\delta is positive (Absolute Value in an Ordered Field). This is claim 2.

Step 5 (Claim 3). Let 0<δ′<δ0<\delta'<\delta and let (μ^,ν^)(\hat{\mu},\hat{\nu}) be a maximising pair of Ψδ,α\Psi_{\delta,\alpha}; by Step 1 applied to (δ′,α)(\delta',\alpha), M(δ′,α)M(\delta',\alpha) is a real number and an upper bound of the values of Ψδ′,α\Psi_{\delta',\alpha}. By The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair §monotone, read with δ′\delta' and δ\delta in the roles of the smaller and the larger weight there, and applied to the first pair and to the second,

uδ−(μ^)+(δ−δ′) E1(μ^)≤uδ′−(μ^),vδ′+(ν^)≤vδ+(ν^)−(δ−δ′) E2(ν^).u^{-}_{\delta}(\hat{\mu})+(\delta-\delta')\,\mathcal{E}_{1}(\hat{\mu})\le u^{-}_{\delta'}(\hat{\mu}),\qquad v^{+}_{\delta'}(\hat{\nu})\le v^{+}_{\delta}(\hat{\nu})-(\delta-\delta')\,\mathcal{E}_{2}(\hat{\nu}).

Multiplying by the positive κ1\kappa_{1} and κ2\kappa_{2} (claim 5 of Elementary Arithmetic in an Ordered Field), reversing the sign of the second (claim 4 of Elementary Order Arithmetic in an Ordered Field) and adding −αL(μ^,ν^)-\alpha L(\hat{\mu},\hat{\nu}),

M(δ′,α)≥Ψδ′,α(μ^,ν^)≥Ψδ,α(μ^,ν^)+(δ−δ′)(κ1 E1(μ^)+κ2 E2(ν^))=M(δ,α)+(δ−δ′)(κ1 E1(μ^)+κ2 E2(ν^)),M(\delta',\alpha)\ge\Psi_{\delta',\alpha}(\hat{\mu},\hat{\nu})\ge\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+(\delta-\delta')\bigl(\kappa_{1}\,\mathcal{E}_{1}(\hat{\mu})+\kappa_{2}\,\mathcal{E}_{2}(\hat{\nu})\bigr)=M(\delta,\alpha)+(\delta-\delta')\bigl(\kappa_{1}\,\mathcal{E}_{1}(\hat{\mu})+\kappa_{2}\,\mathcal{E}_{2}(\hat{\nu})\bigr),

the middle step by distributivity. This is claim 3.

Step 6 (Claim 4). Let 0<α′<α0<\alpha'<\alpha and let (μ^,ν^)(\hat{\mu},\hat{\nu}) be a maximising pair of Ψδ,α\Psi_{\delta,\alpha}; by Step 1 applied to (δ,α′)(\delta,\alpha'), M(δ,α′)M(\delta,\alpha') is an upper bound of the values of Ψδ,α′\Psi_{\delta,\alpha'}. Since −α′L(μ^,ν^)=−αL(μ^,ν^)+(α−α′)L(μ^,ν^)-\alpha'L(\hat{\mu},\hat{\nu})=-\alpha L(\hat{\mu},\hat{\nu})+(\alpha-\alpha')L(\hat{\mu},\hat{\nu}) by distributivity,

M(δ,α′)≥Ψδ,α′(μ^,ν^)=Ψδ,α(μ^,ν^)+(α−α′) L(μ^,ν^)=M(δ,α)+(α−α′) L(μ^,ν^),M(\delta,\alpha')\ge\Psi_{\delta,\alpha'}(\hat{\mu},\hat{\nu})=\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+(\alpha-\alpha')\,L(\hat{\mu},\hat{\nu})=M(\delta,\alpha)+(\alpha-\alpha')\,L(\hat{\mu},\hat{\nu}),

which is claim 4.

Please log in to copy this version.

Citations

Loading…

Dependency Graph

0 prerequisites

Comments

Loading…