Each result cited is universally quantified over the data in its own statement. For i ∈ { 1 , 2 } i\in\{1,2\} i ∈ { 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 e 0 e_{0} e 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 i i i -th pair at the dimension n i n_{i} n i : directly when n i = d n_{i}=d n i = d , and at the configuration level when n i = d N n_{i}=dN n i = d N . We write W W W for W 2 W_{2} W 2 on P 2 ( R n 1 ) \mathcal{P}_{2}(\mathbb{R}^{n_{1}}) P 2 ( R n 1 ) and on P 2 ( R n 2 ) \mathcal{P}_{2}(\mathbb{R}^{n_{2}}) P 2 ( 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 = n i m=n_{i} m = n i ), so that it is symmetric and nonnegative (Metric Space ). 1 / n 1/n 1/ n is the multiplicative inverse of the positive real attached to n ∈ N n\in\mathbb{N} n ∈ N (The Real Numbers: Standing Notation and Background §numbers ); it satisfies 0 < 1 / n ≤ 1 0<1/n\le1 0 < 1/ n ≤ 1 (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}} ( 1/ n ) n ∈ N converges to 0 0 0 : given a positive ε \varepsilon ε , claim 3 of The Archimedean Property of the Real Numbers provides N ∈ N N\in\mathbb{N} N ∈ N with 1 / N < ε 1/N<\varepsilon 1/ N < ε , and for n ≥ N n\ge N n ≥ N the real attached to n n n is at least the one attached to N N N (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 ∣1/ n − 0∣ = 1/ n ≤ 1/ N < ε by Order Reversal under Reciprocals, and Summability of the Reciprocals of the Squares §reciprocal . Fix positive δ , α ∈ R \delta,\alpha\in\mathbb{R} δ , α ∈ R . Each D i \mathcal{D}_{i} D i contains the nonempty D i , Σ \mathcal{D}_{i,\Sigma} D i , Σ (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 D 1 × D 2 \mathcal{D}_{1}\times\mathcal{D}_{2} D 1 × D 2 is nonempty. The products κ 1 δ \kappa_{1}\delta κ 1 δ and κ 2 δ \kappa_{2}\delta κ 2 δ are positive (claim 5 of Elementary Order Arithmetic in an Ordered Field ), so κ i δ e 0 ≤ κ i δ E i ( σ ) \kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i}(\sigma) κ i δ e 0 ≤ κ i δ E i ( σ ) for σ ∈ D i \sigma\in\mathcal{D}_{i} σ ∈ 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 , u u u has penalty-subordinate growth from above relative to the first pair and v v v from below relative to the second. By Basic Properties of the Delta-Envelopes on the Wasserstein Space §semicontinuity , u δ − u^{-}_{\delta} u δ − is upper semicontinuous on D 1 \mathcal{D}_{1} D 1 relative to D 1 \mathcal{D}_{1} D 1 in ( P 2 ( R n 1 ) , W ) (\mathcal{P}_{2}(\mathbb{R}^{n_{1}}),W) ( P 2 ( R n 1 ) , W ) and v δ + v^{+}_{\delta} v δ + is lower semicontinuous on D 2 \mathcal{D}_{2} D 2 relative to D 2 \mathcal{D}_{2} D 2 in ( P 2 ( R n 2 ) , W ) (\mathcal{P}_{2}(\mathbb{R}^{n_{2}}),W) ( P 2 ( R n 2 ) , W ) . By The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair §bounded ,
u δ − ( μ ) ≤ b − δ E 1 ( μ ) ( μ ∈ D 1 ) , b ′ + δ E 2 ( ν ) ≤ v δ + ( ν ) ( ν ∈ D 2 ) . ( 0 a ) 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}) u δ − ( μ ) ≤ b − δ E 1 ( μ ) ( μ ∈ D 1 ) , b ′ + δ E 2 ( ν ) ≤ v δ + ( ν ) ( ν ∈ D 2 ) . ( 0 a )
Let ( μ , ν ) ∈ D 1 × D 2 (\mu,\nu)\in\mathcal{D}_{1}\times\mathcal{D}_{2} ( μ , ν ) ∈ D 1 × D 2 . Multiplying (0a) by the positive κ 1 \kappa_{1} κ 1 and κ 2 \kappa_{2} κ 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 κ 1 u δ − ( μ ) ≤ κ 1 b − κ 1 δ E 1 ( μ ) \kappa_{1}u^{-}_{\delta}(\mu)\le\kappa_{1}b-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu) κ 1 u δ − ( μ ) ≤ κ 1 b − κ 1 δ E 1 ( μ ) and − κ 2 v δ + ( ν ) ≤ − κ 2 b ′ − κ 2 δ E 2 ( ν ) -\kappa_{2}v^{+}_{\delta}(\nu)\le-\kappa_{2}b'-\kappa_{2}\delta\,\mathcal{E}_{2}(\nu) − κ 2 v δ + ( ν ) ≤ − κ 2 b ′ − κ 2 δ E 2 ( ν ) ; and 0 = α ⋅ 0 ≤ α L ( μ , ν ) 0=\alpha\cdot0\le\alpha L(\mu,\nu) 0 = α ⋅ 0 ≤ αL ( μ , ν ) (claim 5 of Elementary Arithmetic in an Ordered Field , as 0 ≤ L ( μ , ν ) 0\le L(\mu,\nu) 0 ≤ L ( μ , ν ) ), so − α L ( μ , ν ) ≤ 0 -\alpha L(\mu,\nu)\le0 − αL ( μ , ν ) ≤ 0 . Adding, and then using κ i δ e 0 ≤ κ i δ E i \kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i} κ i δ e 0 ≤ κ i δ E i and distributivity,
Ψ δ , α ( μ , ν ) ≤ κ 1 b − κ 2 b ′ − κ 1 δ E 1 ( μ ) − κ 2 δ E 2 ( ν ) ≤ κ 1 b − κ 2 b ′ − ( κ 1 + κ 2 ) δ e 0 . ( 0 b ) \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}) Ψ δ , α ( μ , ν ) ≤ κ 1 b − κ 2 b ′ − κ 1 δ E 1 ( μ ) − κ 2 δ E 2 ( ν ) ≤ κ 1 b − κ 2 b ′ − ( κ 1 + κ 2 ) δ e 0 . ( 0 b )
Step 1 (Claim 1: the supremum and a maximising sequence). By (0b) the nonempty set of values of Ψ δ , α \Psi_{\delta,\alpha} Ψ δ , α is bounded above by κ 1 b − κ 2 b ′ − ( κ 1 + κ 2 ) δ e 0 \kappa_{1}b-\kappa_{2}b'-(\kappa_{1}+\kappa_{2})\delta e_{0} κ 1 b − κ 2 b ′ − ( κ 1 + κ 2 ) δ e 0 , so it has a least upper bound M = M ( δ , α ) ∈ R M=M(\delta,\alpha)\in\mathbb{R} M = M ( δ , α ) ∈ R . For each n ∈ N n\in\mathbb{N} n ∈ N , claim 3 of Approximation Property of the Supremum and the Infimum in R \mathbb{R} R with the positive 1 / n 1/n 1/ n shows that the set of ( μ , ν ) ∈ D 1 × D 2 (\mu,\nu)\in\mathcal{D}_{1}\times\mathcal{D}_{2} ( μ , ν ) ∈ D 1 × D 2 with M − 1 / n < Ψ δ , α ( μ , ν ) M-1/n<\Psi_{\delta,\alpha}(\mu,\nu) M − 1/ n < Ψ δ , α ( μ , ν ) is nonempty; by Axiom of Countable Choice choose such a pair ( μ n , ν n ) (\mu_{n},\nu_{n}) ( μ n , ν n ) for every n n n . As 1 / n ≤ 1 1/n\le1 1/ n ≤ 1 , M − 1 < Ψ δ , α ( μ n , ν n ) M-1<\Psi_{\delta,\alpha}(\mu_{n},\nu_{n}) M − 1 < Ψ δ , α ( μ n , ν n ) (claims 2 and 4 of Elementary Order Arithmetic in an Ordered Field ). By the first inequality of (0b) and κ 2 δ e 0 ≤ κ 2 δ E 2 ( ν n ) \kappa_{2}\delta e_{0}\le\kappa_{2}\delta\,\mathcal{E}_{2}(\nu_{n}) κ 2 δ e 0 ≤ κ 2 δ E 2 ( ν n ) ,
M − 1 < κ 1 b − κ 2 b ′ − κ 1 δ E 1 ( μ n ) − κ 2 δ e 0 , M-1<\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu_{n})-\kappa_{2}\delta e_{0}, M − 1 < κ 1 b − κ 2 b ′ − κ 1 δ E 1 ( μ n ) − κ 2 δ e 0 ,
so, by claim 1 of Elementary Order Arithmetic in an Ordered Field , κ 1 δ E 1 ( μ n ) < A 1 \kappa_{1}\delta\,\mathcal{E}_{1}(\mu_{n})<A_{1} κ 1 δ E 1 ( μ n ) < A 1 with A 1 = κ 1 b − κ 2 b ′ − κ 2 δ e 0 − M + 1 A_{1}=\kappa_{1}b-\kappa_{2}b'-\kappa_{2}\delta e_{0}-M+1 A 1 = κ 1 b − κ 2 b ′ − κ 2 δ e 0 − M + 1 ; multiplying by the positive ( κ 1 δ ) − 1 (\kappa_{1}\delta)^{-1} ( κ 1 δ ) − 1 (claims 7 and 10 of that lemma) gives E 1 ( μ n ) < c 1 \mathcal{E}_{1}(\mu_{n})<c_{1} E 1 ( μ n ) < c 1 with c 1 = ( κ 1 δ ) − 1 A 1 c_{1}=(\kappa_{1}\delta)^{-1}A_{1} c 1 = ( κ 1 δ ) − 1 A 1 . In the same way, from κ 1 δ e 0 ≤ κ 1 δ E 1 ( μ n ) \kappa_{1}\delta e_{0}\le\kappa_{1}\delta\,\mathcal{E}_{1}(\mu_{n}) κ 1 δ e 0 ≤ κ 1 δ E 1 ( μ n ) , we get κ 2 δ E 2 ( ν n ) < A 2 \kappa_{2}\delta\,\mathcal{E}_{2}(\nu_{n})<A_{2} κ 2 δ E 2 ( ν n ) < A 2 with A 2 = κ 1 b − κ 2 b ′ − κ 1 δ e 0 − M + 1 A_{2}=\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta e_{0}-M+1 A 2 = κ 1 b − κ 2 b ′ − κ 1 δ e 0 − M + 1 , and E 2 ( ν n ) < c 2 \mathcal{E}_{2}(\nu_{n})<c_{2} E 2 ( ν n ) < c 2 with c 2 = ( κ 2 δ ) − 1 A 2 c_{2}=(\kappa_{2}\delta)^{-1}A_{2} c 2 = ( κ 2 δ ) − 1 A 2 . The constants c 1 , c 2 c_{1},c_{2} c 1 , c 2 do not depend on n n n .
Step 2 (Claim 1: a jointly convergent subsequence). The sets K 1 = { σ ∈ D 1 : E 1 ( σ ) ≤ c 1 } K_{1}=\{\sigma\in\mathcal{D}_{1}:\mathcal{E}_{1}(\sigma)\le c_{1}\} K 1 = { σ ∈ D 1 : E 1 ( σ ) ≤ c 1 } and K 2 = { σ ∈ D 2 : E 2 ( σ ) ≤ c 2 } K_{2}=\{\sigma\in\mathcal{D}_{2}:\mathcal{E}_{2}(\sigma)\le c_{2}\} K 2 = { σ ∈ D 2 : E 2 ( σ ) ≤ c 2 } are sequentially compact in ( P 2 ( R n 1 ) , W ) (\mathcal{P}_{2}(\mathbb{R}^{n_{1}}),W) ( P 2 ( R n 1 ) , W ) and in ( P 2 ( R n 2 ) , W ) (\mathcal{P}_{2}(\mathbb{R}^{n_{2}}),W) ( P 2 ( R n 2 ) , W ) by Wasserstein-Coercive Penalty Pairs §coercive , and μ n ∈ K 1 \mu_{n}\in K_{1} μ n ∈ K 1 , ν n ∈ K 2 \nu_{n}\in K_{2} ν n ∈ K 2 for every n n n by Step 1. So there are μ ^ ∈ K 1 \hat{\mu}\in K_{1} μ ^ ∈ K 1 and a strictly increasing ( n k ) k ∈ N (n_{k})_{k\in\mathbb{N}} ( n k ) k ∈ N with ( μ n k ) k (\mu_{n_{k}})_{k} ( μ n k ) k converging to μ ^ \hat{\mu} μ ^ ; the sequence ( ν n k ) k (\nu_{n_{k}})_{k} ( ν n k ) k lies in K 2 K_{2} K 2 , so there are ν ^ ∈ K 2 \hat{\nu}\in K_{2} ν ^ ∈ K 2 and a strictly increasing ( k j ) j ∈ N (k_{j})_{j\in\mathbb{N}} ( k j ) j ∈ N with ( ν n k j ) j (\nu_{n_{k_{j}}})_{j} ( ν n k j ) j converging to ν ^ \hat{\nu} ν ^ . Put m j = n k j m_{j}=n_{k_{j}} m j = n k j ; ( m j ) j (m_{j})_{j} ( m j ) j is strictly increasing and ( μ m j ) j (\mu_{m_{j}})_{j} ( μ m j ) j , ( ν m j ) j (\nu_{m_{j}})_{j} ( ν m j ) j , ( 1 / m j ) j (1/m_{j})_{j} ( 1/ m j ) j are subsequences of ( μ n ) n (\mu_{n})_{n} ( μ n ) n , ( ν n ) n (\nu_{n})_{n} ( ν n ) n , ( 1 / n ) n (1/n)_{n} ( 1/ n ) n (claims 2 and 3 of A Subsequence of a Subsequence is a Subsequence ), and ( μ m j ) j (\mu_{m_{j}})_{j} ( μ m j ) j is the subsequence of ( μ n k ) k (\mu_{n_{k}})_{k} ( μ n k ) k determined by ( k j ) j (k_{j})_{j} ( k j ) j . By A Subsequence of a Convergent Sequence Has the Same Limit , ( μ m j ) j (\mu_{m_{j}})_{j} ( μ m j ) j converges to μ ^ \hat{\mu} μ ^ , and ( 1 / m j ) j (1/m_{j})_{j} ( 1/ m j ) j converges to 0 0 0 in ( R , d R ) (\mathbb{R},d_{\mathbb{R}}) ( R , d R ) , hence in the sense of Limit of a Sequence of Real Numbers (The Real Numbers: Standing Notation and Background §sequences ). Also μ ^ ∈ K 1 ⊆ D 1 \hat{\mu}\in K_{1}\subseteq\mathcal{D}_{1} μ ^ ∈ K 1 ⊆ D 1 and ν ^ ∈ K 2 ⊆ D 2 \hat{\nu}\in K_{2}\subseteq\mathcal{D}_{2} ν ^ ∈ K 2 ⊆ D 2 .
The real sequence ( W ( μ m j , μ ^ ) ) j (W(\mu_{m_{j}},\hat{\mu}))_{j} ( W ( μ m j , μ ^ ) ) j converges to 0 0 0 : given a positive ε \varepsilon ε , the convergence in ( P 2 ( R n 1 ) , W ) (\mathcal{P}_{2}(\mathbb{R}^{n_{1}}),W) ( P 2 ( R n 1 ) , W ) gives N N N with ∣ W ( μ m j , μ ^ ) − 0 ∣ = W ( μ m j , μ ^ ) < ε |W(\mu_{m_{j}},\hat{\mu})-0|=W(\mu_{m_{j}},\hat{\mu})<\varepsilon ∣ W ( μ m j , μ ^ ) − 0∣ = W ( μ m j , μ ^ ) < ε for j ≥ N j\ge N j ≥ N , W W W being nonnegative (Absolute Value in an Ordered Field ); likewise ( W ( ν m j , ν ^ ) ) j (W(\nu_{m_{j}},\hat{\nu}))_{j} ( W ( ν m j , ν ^ ) ) j converges to 0 0 0 . Put L j = L ( μ m j , ν m j ) L_{j}=L(\mu_{m_{j}},\nu_{m_{j}}) L j = L ( μ m j , ν m j ) and L ^ = L ( μ ^ , ν ^ ) \hat{L}=L(\hat{\mu},\hat{\nu}) L ^ = L ( μ ^ , ν ^ ) . By the continuity hypothesis on L L L , ( L j ) j (L_{j})_{j} ( L j ) j converges to L ^ \hat{L} L ^ ; since ∣ ∣ L j − L ^ ∣ − 0 ∣ = ∣ L j − L ^ ∣ \bigl||L_{j}-\hat{L}|-0\bigr|=|L_{j}-\hat{L}| ∣ L j − L ^ ∣ − 0 = ∣ L j − L ^ ∣ (claim 1 of Properties of the Absolute Value in an Ordered Field ), ( ∣ L j − L ^ ∣ ) j (|L_{j}-\hat{L}|)_{j} ( ∣ L j − L ^ ∣ ) j converges to 0 0 0 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
a j = W ( μ m j , μ ^ ) + W ( ν m j , ν ^ ) + ∣ L j − L ^ ∣ + 1 / m j a_{j}=W(\mu_{m_{j}},\hat{\mu})+W(\nu_{m_{j}},\hat{\nu})+|L_{j}-\hat{L}|+1/m_{j} a j = W ( μ m j , μ ^ ) + W ( ν m j , ν ^ ) + ∣ L j − L ^ ∣ + 1/ m j
converges to 0 0 0 , and each of its four summands is at most a j a_{j} a j , the other three being nonnegative.
Step 3 (Claim 1: attainment). Let ε ∈ R \varepsilon\in\mathbb{R} ε ∈ R be positive. The choices are made in this order: first ε 1 \varepsilon_{1} ε 1 , then r 1 r_{1} r 1 and r 2 r_{2} r 2 , then t t t , then the index j j j . Put ε 1 = ε ⋅ 4 − 1 \varepsilon_{1}=\varepsilon\cdot4^{-1} ε 1 = ε ⋅ 4 − 1 , where 4 = 2 + 2 4=2+2 4 = 2 + 2 is positive; ε 1 \varepsilon_{1} ε 1 is positive and 4 ε 1 = ε 4\varepsilon_{1}=\varepsilon 4 ε 1 = ε (claims 1, 5, 7 and 8 of Elementary Order Arithmetic in an Ordered Field ). The reals κ 1 − 1 ε 1 \kappa_{1}^{-1}\varepsilon_{1} κ 1 − 1 ε 1 , κ 2 − 1 ε 1 \kappa_{2}^{-1}\varepsilon_{1} κ 2 − 1 ε 1 and α − 1 ε 1 \alpha^{-1}\varepsilon_{1} α − 1 ε 1 are positive (claims 5 and 7 of that lemma). By the upper semicontinuity of u δ − u^{-}_{\delta} u δ − at μ ^ \hat{\mu} μ ^ relative to D 1 \mathcal{D}_{1} D 1 (Upper Semicontinuous Function on a Subset of a Metric Space ) there is a positive r 1 r_{1} r 1 such that every μ ′ ∈ D 1 \mu'\in\mathcal{D}_{1} μ ′ ∈ D 1 with W ( μ ^ , μ ′ ) < r 1 W(\hat{\mu},\mu')<r_{1} W ( μ ^ , μ ′ ) < r 1 satisfies u δ − ( μ ′ ) < u δ − ( μ ^ ) + κ 1 − 1 ε 1 u^{-}_{\delta}(\mu')<u^{-}_{\delta}(\hat{\mu})+\kappa_{1}^{-1}\varepsilon_{1} u δ − ( μ ′ ) < u δ − ( μ ^ ) + κ 1 − 1 ε 1 , hence, multiplying by κ 1 \kappa_{1} κ 1 (claim 10 of Elementary Order Arithmetic in an Ordered Field ),
κ 1 u δ − ( μ ′ ) < κ 1 u δ − ( μ ^ ) + ε 1 ; \kappa_{1}u^{-}_{\delta}(\mu')<\kappa_{1}u^{-}_{\delta}(\hat{\mu})+\varepsilon_{1}; κ 1 u δ − ( μ ′ ) < κ 1 u δ − ( μ ^ ) + ε 1 ;
by the lower semicontinuity of v δ + v^{+}_{\delta} v δ + at ν ^ \hat{\nu} ν ^ relative to D 2 \mathcal{D}_{2} D 2 (Lower Semicontinuous Function on a Subset of a Metric Space ) there is a positive r 2 r_{2} r 2 such that every ν ′ ∈ D 2 \nu'\in\mathcal{D}_{2} ν ′ ∈ D 2 with W ( ν ^ , ν ′ ) < r 2 W(\hat{\nu},\nu')<r_{2} W ( ν ^ , ν ′ ) < r 2 satisfies v δ + ( ν ^ ) − κ 2 − 1 ε 1 < v δ + ( ν ′ ) v^{+}_{\delta}(\hat{\nu})-\kappa_{2}^{-1}\varepsilon_{1}<v^{+}_{\delta}(\nu') v δ + ( ν ^ ) − κ 2 − 1 ε 1 < v δ + ( ν ′ ) , hence κ 2 v δ + ( ν ^ ) − ε 1 < κ 2 v δ + ( ν ′ ) \kappa_{2}v^{+}_{\delta}(\hat{\nu})-\varepsilon_{1}<\kappa_{2}v^{+}_{\delta}(\nu') κ 2 v δ + ( ν ^ ) − ε 1 < κ 2 v δ + ( ν ′ ) in the same way. Let t t t be the least of r 1 r_{1} r 1 , r 2 r_{2} r 2 , α − 1 ε 1 \alpha^{-1}\varepsilon_{1} α − 1 ε 1 and ε 1 \varepsilon_{1} ε 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 ( a j ) j (a_{j})_{j} ( a j ) j converges to 0 0 0 , there is j ∈ N j\in\mathbb{N} j ∈ N with a j = ∣ a j − 0 ∣ < t a_{j}=|a_{j}-0|<t a 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 W W W ,
W ( μ ^ , μ m j ) < r 1 , W ( ν ^ , ν m j ) < r 2 , ∣ L j − L ^ ∣ < α − 1 ε 1 , 1 / m j < ε 1 . 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}. W ( μ ^ , μ m j ) < r 1 , W ( ν ^ , ν m j ) < r 2 , ∣ L j − L ^ ∣ < α − 1 ε 1 , 1/ m j < ε 1 .
So, with μ ′ = μ m j ∈ D 1 \mu'=\mu_{m_{j}}\in\mathcal{D}_{1} μ ′ = μ m j ∈ D 1 and ν ′ = ν m j ∈ D 2 \nu'=\nu_{m_{j}}\in\mathcal{D}_{2} ν ′ = ν m j ∈ D 2 , the two semicontinuity bounds give κ 1 u δ − ( μ m j ) < κ 1 u δ − ( μ ^ ) + ε 1 \kappa_{1}u^{-}_{\delta}(\mu_{m_{j}})<\kappa_{1}u^{-}_{\delta}(\hat{\mu})+\varepsilon_{1} κ 1 u δ − ( μ m j ) < κ 1 u δ − ( μ ^ ) + ε 1 and, by sign reversal (claim 4 of Elementary Order Arithmetic in an Ordered Field ), − κ 2 v δ + ( ν m j ) < − κ 2 v δ + ( ν ^ ) + ε 1 -\kappa_{2}v^{+}_{\delta}(\nu_{m_{j}})<-\kappa_{2}v^{+}_{\delta}(\hat{\nu})+\varepsilon_{1} − κ 2 v δ + ( ν m j ) < − κ 2 v δ + ( ν ^ ) + ε 1 ; and L ^ − L j ≤ ∣ L j − L ^ ∣ < α − 1 ε 1 \hat{L}-L_{j}\le|L_{j}-\hat{L}|<\alpha^{-1}\varepsilon_{1} L ^ − L j ≤ ∣ L j − L ^ ∣ < α − 1 ε 1 (claims 2 and 3 of Properties of the Absolute Value in an Ordered Field ) gives, multiplying by α \alpha α and reversing the sign, − α L j < − α L ^ + ε 1 -\alpha L_{j}<-\alpha\hat{L}+\varepsilon_{1} − α L j < − α L ^ + ε 1 . Adding these three strict inequalities (claim 3 of Elementary Order Arithmetic in an Ordered Field , twice),
Ψ δ , α ( μ m j , ν m j ) < Ψ δ , α ( μ ^ , ν ^ ) + 3 ε 1 . \Psi_{\delta,\alpha}(\mu_{m_{j}},\nu_{m_{j}})<\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+3\varepsilon_{1}. Ψ δ , α ( μ m j , ν m j ) < Ψ δ , α ( μ ^ , ν ^ ) + 3 ε 1 .
By the choice of the pair with index m j m_{j} m j in Step 1, M − 1 / m j < Ψ δ , α ( μ m j , ν m j ) M-1/m_{j}<\Psi_{\delta,\alpha}(\mu_{m_{j}},\nu_{m_{j}}) M − 1/ m j < Ψ δ , α ( μ m j , ν m j ) , and 1 / m j < ε 1 1/m_{j}<\varepsilon_{1} 1/ m j < ε 1 ; so M < Ψ δ , α ( μ ^ , ν ^ ) + 4 ε 1 = Ψ δ , α ( μ ^ , ν ^ ) + ε M<\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+4\varepsilon_{1}=\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})+\varepsilon M < Ψ δ , α ( μ ^ , ν ^ ) + 4 ε 1 = Ψ δ , α ( μ ^ , ν ^ ) + ε (claims 1, 2 and 3 of Elementary Order Arithmetic in an Ordered Field ). As ε \varepsilon ε was an arbitrary positive real, M ≤ Ψ δ , α ( μ ^ , ν ^ ) M\le\Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu}) M ≤ Ψ δ , α ( μ ^ , ν ^ ) by Comparison of Real Numbers with Arbitrary Positive Slack §slack-above ; and Ψ δ , α ( μ ^ , ν ^ ) ≤ M \Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})\le M Ψ δ , α ( μ ^ , ν ^ ) ≤ M , M M M being an upper bound of the values. So Ψ δ , α ( μ ^ , ν ^ ) = M \Psi_{\delta,\alpha}(\hat{\mu},\hat{\nu})=M Ψ δ , α ( μ ^ , ν ^ ) = M , with ( μ ^ , ν ^ ) ∈ D 1 × D 2 (\hat{\mu},\hat{\nu})\in\mathcal{D}_{1}\times\mathcal{D}_{2} ( μ ^ , ν ^ ) ∈ D 1 × D 2 , which proves claim 1.
Step 4 (Claim 2). Let ( μ , ν ) ∈ D 1 × D 2 (\mu,\nu)\in\mathcal{D}_{1}\times\mathcal{D}_{2} ( μ , ν ) ∈ D 1 × D 2 with 0 ≤ Ψ δ , α ( μ , ν ) 0\le\Psi_{\delta,\alpha}(\mu,\nu) 0 ≤ Ψ δ , α ( μ , ν ) . By the first inequality of (0b), 0 ≤ κ 1 b − κ 2 b ′ − κ 1 δ E 1 ( μ ) − κ 2 δ E 2 ( ν ) 0\le\kappa_{1}b-\kappa_{2}b'-\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)-\kappa_{2}\delta\,\mathcal{E}_{2}(\nu) 0 ≤ κ 1 b − κ 2 b ′ − κ 1 δ E 1 ( μ ) − κ 2 δ E 2 ( ν ) , so by claim 3 of Elementary Arithmetic in an Ordered Field and κ i δ e 0 ≤ κ i δ E i \kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i} κ i δ e 0 ≤ κ i δ E i (with claim 4 of Elementary Order Arithmetic in an Ordered Field ),
κ 1 δ E 1 ( μ ) ≤ κ 1 b − κ 2 b ′ − κ 2 δ e 0 , κ 2 δ E 2 ( ν ) ≤ κ 1 b − κ 2 b ′ − κ 1 δ e 0 . \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}. κ 1 δ E 1 ( μ ) ≤ κ 1 b − κ 2 b ′ − κ 2 δ e 0 , κ 2 δ E 2 ( ν ) ≤ κ 1 b − κ 2 b ′ − κ 1 δ 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 ′ ∣ = ∣ b ′ ∣ -b'\le|-b'|=|b'| − b ′ ≤ ∣ − b ′ ∣ = ∣ b ′ ∣ and − e 0 ≤ ∣ e 0 ∣ -e_{0}\le|e_{0}| − e 0 ≤ ∣ e 0 ∣ ; multiplying by the positive κ 1 \kappa_{1} κ 1 , κ 2 \kappa_{2} κ 2 and κ i δ \kappa_{i}\delta κ i δ (claim 5 of Elementary Arithmetic in an Ordered Field ) and adding, the right-hand sides are at most κ 1 ∣ b ∣ + κ 2 ∣ b ′ ∣ + κ 2 δ ∣ e 0 ∣ \kappa_{1}|b|+\kappa_{2}|b'|+\kappa_{2}\delta|e_{0}| κ 1 ∣ b ∣ + κ 2 ∣ b ′ ∣ + κ 2 δ ∣ e 0 ∣ and κ 1 ∣ b ∣ + κ 2 ∣ b ′ ∣ + κ 1 δ ∣ e 0 ∣ \kappa_{1}|b|+\kappa_{2}|b'|+\kappa_{1}\delta|e_{0}| κ 1 ∣ b ∣ + κ 2 ∣ b ′ ∣ + κ 1 δ ∣ e 0 ∣ respectively. By distributivity B δ = κ 1 ∣ b ∣ + κ 2 ∣ b ′ ∣ + κ 1 δ ∣ e 0 ∣ + κ 2 δ ∣ e 0 ∣ B_{\delta}=\kappa_{1}|b|+\kappa_{2}|b'|+\kappa_{1}\delta|e_{0}|+\kappa_{2}\delta|e_{0}| B δ = κ 1 ∣ b ∣ + κ 2 ∣ b ′ ∣ + κ 1 δ ∣ e 0 ∣ + κ 2 δ ∣ 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 B δ B_{\delta} B δ , and κ 1 δ E 1 ( μ ) ≤ B δ \kappa_{1}\delta\,\mathcal{E}_{1}(\mu)\le B_{\delta} κ 1 δ E 1 ( μ ) ≤ B δ , κ 2 δ E 2 ( ν ) ≤ B δ \kappa_{2}\delta\,\mathcal{E}_{2}(\nu)\le B_{\delta} κ 2 δ E 2 ( ν ) ≤ B δ . For the lower bounds, − ∣ e 0 ∣ ≤ e 0 -|e_{0}|\le e_{0} − ∣ e 0 ∣ ≤ e 0 (claim 3 of Properties of the Absolute Value in an Ordered Field ) gives − κ i δ ∣ e 0 ∣ ≤ κ i δ e 0 ≤ κ i δ E i -\kappa_{i}\delta|e_{0}|\le\kappa_{i}\delta e_{0}\le\kappa_{i}\delta\,\mathcal{E}_{i} − κ i δ ∣ e 0 ∣ ≤ κ i δ e 0 ≤ κ i δ E i , and κ i δ ∣ e 0 ∣ ≤ B δ \kappa_{i}\delta|e_{0}|\le B_{\delta} κ i δ ∣ e 0 ∣ ≤ B δ gives − B δ ≤ − κ i δ ∣ e 0 ∣ -B_{\delta}\le-\kappa_{i}\delta|e_{0}| − B δ ≤ − κ i δ ∣ e 0 ∣ (claim 4 of Elementary Order Arithmetic in an Ordered Field ); so − B δ ≤ κ 1 δ E 1 ( μ ) -B_{\delta}\le\kappa_{1}\delta\,\mathcal{E}_{1}(\mu) − B δ ≤ κ 1 δ E 1 ( μ ) and − B δ ≤ κ 2 δ E 2 ( ν ) -B_{\delta}\le\kappa_{2}\delta\,\mathcal{E}_{2}(\nu) − B δ ≤ κ 2 δ E 2 ( ν ) . By claim 6 of Properties of the Absolute Value in an Ordered Field , ∣ κ 1 δ E 1 ( μ ) ∣ ≤ B δ |\kappa_{1}\delta\,\mathcal{E}_{1}(\mu)|\le B_{\delta} ∣ κ 1 δ E 1 ( μ ) ∣ ≤ B δ and ∣ κ 2 δ E 2 ( ν ) ∣ ≤ B δ |\kappa_{2}\delta\,\mathcal{E}_{2}(\nu)|\le B_{\delta} ∣ κ 2 δ E 2 ( ν ) ∣ ≤ B δ , and by its claim 4, ∣ κ i δ E i ∣ = ∣ κ i δ ∣ ∣ E i ∣ = κ i δ ∣ E i ∣ |\kappa_{i}\delta\,\mathcal{E}_{i}|=|\kappa_{i}\delta|\,|\mathcal{E}_{i}|=\kappa_{i}\delta\,|\mathcal{E}_{i}| ∣ κ i δ E i ∣ = ∣ κ i δ ∣ ∣ E i ∣ = κ i δ ∣ E i ∣ , as κ i δ \kappa_{i}\delta κ i δ is positive (Absolute Value in an Ordered Field ). This is claim 2.
Step 5 (Claim 3). Let 0 < δ ′ < δ 0<\delta'<\delta 0 < δ ′ < δ and let ( μ ^ , ν ^ ) (\hat{\mu},\hat{\nu}) ( μ ^ , ν ^ ) be a maximising pair of Ψ δ , α \Psi_{\delta,\alpha} Ψ δ , α ; by Step 1 applied to ( δ ′ , α ) (\delta',\alpha) ( δ ′ , α ) , M ( δ ′ , α ) M(\delta',\alpha) M ( δ ′ , α ) is a real number and an upper bound of the values of Ψ δ ′ , α \Psi_{\delta',\alpha} Ψ δ ′ , α . By The Delta-Envelopes of Bounded Functions and Their Monotonicity in the Weight, for a Wasserstein-Coercive Penalty Pair §monotone , read with δ ′ \delta' δ ′ and δ \delta δ in the roles of the smaller and the larger weight there, and applied to the first pair and to the second,
u δ − ( μ ^ ) + ( δ − δ ′ ) E 1 ( μ ^ ) ≤ u δ ′ − ( μ ^ ) , v δ ′ + ( ν ^ ) ≤ v δ + ( ν ^ ) − ( δ − δ ′ ) E 2 ( 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}). u δ − ( μ ^ ) + ( δ − δ ′ ) E 1 ( μ ^ ) ≤ u δ ′ − ( μ ^ ) , v δ ′ + ( ν ^ ) ≤ v δ + ( ν ^ ) − ( δ − δ ′ ) E 2 ( ν ^ ) .
Multiplying by the positive κ 1 \kappa_{1} κ 1 and κ 2 \kappa_{2} κ 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 − α L ( μ ^ , ν ^ ) -\alpha L(\hat{\mu},\hat{\nu}) − αL ( μ ^ , ν ^ ) ,
M ( δ ′ , α ) ≥ Ψ δ ′ , α ( μ ^ , ν ^ ) ≥ Ψ δ , α ( μ ^ , ν ^ ) + ( δ − δ ′ ) ( κ 1 E 1 ( μ ^ ) + κ 2 E 2 ( ν ^ ) ) = M ( δ , α ) + ( δ − δ ′ ) ( κ 1 E 1 ( μ ^ ) + κ 2 E 2 ( 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), M ( δ ′ , α ) ≥ Ψ δ ′ , α ( μ ^ , ν ^ ) ≥ Ψ δ , α ( μ ^ , ν ^ ) + ( δ − δ ′ ) ( κ 1 E 1 ( μ ^ ) + κ 2 E 2 ( ν ^ ) ) = M ( δ , α ) + ( δ − δ ′ ) ( κ 1 E 1 ( μ ^ ) + κ 2 E 2 ( ν ^ ) ) ,
the middle step by distributivity. This is claim 3.
Step 6 (Claim 4). Let 0 < α ′ < α 0<\alpha'<\alpha 0 < α ′ < α and let ( μ ^ , ν ^ ) (\hat{\mu},\hat{\nu}) ( μ ^ , ν ^ ) be a maximising pair of Ψ δ , α \Psi_{\delta,\alpha} Ψ δ , α ; by Step 1 applied to ( δ , α ′ ) (\delta,\alpha') ( δ , α ′ ) , M ( δ , α ′ ) M(\delta,\alpha') M ( δ , α ′ ) is an upper bound of the values of Ψ δ , α ′ \Psi_{\delta,\alpha'} Ψ δ , α ′ . Since − α ′ L ( μ ^ , ν ^ ) = − α L ( 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}) − α ′ L ( μ ^ , ν ^ ) = − αL ( μ ^ , ν ^ ) + ( α − α ′ ) L ( μ ^ , ν ^ ) by distributivity,
M ( δ , α ′ ) ≥ Ψ δ , α ′ ( μ ^ , ν ^ ) = Ψ δ , 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}), M ( δ , α ′ ) ≥ Ψ δ , α ′ ( μ ^ , ν ^ ) = Ψ δ , α ( μ ^ , ν ^ ) + ( α − α ′ ) L ( μ ^ , ν ^ ) = M ( δ , α ) + ( α − α ′ ) L ( μ ^ , ν ^ ) ,
which is claim 4.