Let l l l and l ~ \tilde{l} l ~ be natural numbers with l ≥ 2 l\ge2 l ≥ 2 and l ~ ≥ 1 \tilde{l}\ge1 l ~ ≥ 1 , let β ~ \tilde{\beta} β ~ be an observation-rate family on l l l states with l ~ \tilde{l} l ~ observation channels and rate bound B ~ \tilde{B} B ~ , let ( U ~ , β ~ ˉ ) (\tilde{U},\bar{\tilde{\beta}}) ( U ~ , β ~ ˉ ) be a twice continuously differentiable extension of β ~ \tilde{\beta} β ~ with derivative bound K ~ \tilde{K} K ~ , and let b ~ ˉ \bar{\tilde{b}} b ~ ˉ be the extended aggregate observation drift of ( U ~ , β ~ ˉ ) (\tilde{U},\bar{\tilde{\beta}}) ( U ~ , β ~ ˉ ) . Adopt the coordinate and partial-derivative notation ∂ γ \partial_\gamma ∂ γ , ∂ δ ∂ γ \partial_\delta\partial_\gamma ∂ δ ∂ γ of the extension definition, write Δ l \Delta^l Δ l for the probability simplex , and write d d d for the Euclidean distance . Then for every υ ∈ { 1 , … , l ~ } \upsilon\in\{1,\dots,\tilde{l}\} υ ∈ { 1 , … , l ~ } :
(i) (Regularity, derivative formulas, and restriction.) b ~ ˉ υ \bar{\tilde{b}}^\upsilon b ~ ˉ υ is of class C 2 C^2 C 2 on the open set U ~ \tilde{U} U ~ ; in particular each ∂ γ b ~ ˉ υ \partial_\gamma\bar{\tilde{b}}^\upsilon ∂ γ b ~ ˉ υ exists and is of class C 1 C^1 C 1 on U ~ \tilde{U} U ~ , and for all γ , δ ∈ { 1 , … , l } \gamma,\delta\in\{1,\dots,l\} γ , δ ∈ { 1 , … , l } and Σ ∈ U ~ \Sigma\in\tilde{U} Σ ∈ U ~ :
∂ γ b ~ ˉ υ ( Σ ) = β ~ ˉ ( γ , υ , Σ ) + ∑ σ = 1 l Σ σ ∂ γ β ~ ˉ ( σ , υ , Σ ) , \partial_\gamma\bar{\tilde{b}}^\upsilon(\Sigma)=\bar{\tilde{\beta}}(\gamma,\upsilon,\Sigma)+\sum_{\sigma=1}^{l}\Sigma^\sigma\,\partial_\gamma\bar{\tilde{\beta}}(\sigma,\upsilon,\Sigma), ∂ γ b ~ ˉ υ ( Σ ) = β ~ ˉ ( γ , υ , Σ ) + σ = 1 ∑ l Σ σ ∂ γ β ~ ˉ ( σ , υ , Σ ) ,
∂ δ ∂ γ b ~ ˉ υ ( Σ ) = ∂ δ β ~ ˉ ( γ , υ , Σ ) + ∂ γ β ~ ˉ ( δ , υ , Σ ) + ∑ σ = 1 l Σ σ ∂ δ ∂ γ β ~ ˉ ( σ , υ , Σ ) . \partial_\delta\partial_\gamma\bar{\tilde{b}}^\upsilon(\Sigma)=\partial_\delta\bar{\tilde{\beta}}(\gamma,\upsilon,\Sigma)+\partial_\gamma\bar{\tilde{\beta}}(\delta,\upsilon,\Sigma)+\sum_{\sigma=1}^{l}\Sigma^\sigma\,\partial_\delta\partial_\gamma\bar{\tilde{\beta}}(\sigma,\upsilon,\Sigma). ∂ δ ∂ γ b ~ ˉ υ ( Σ ) = ∂ δ β ~ ˉ ( γ , υ , Σ ) + ∂ γ β ~ ˉ ( δ , υ , Σ ) + σ = 1 ∑ l Σ σ ∂ δ ∂ γ β ~ ˉ ( σ , υ , Σ ) .
Moreover b ~ ˉ \bar{\tilde{b}} b ~ ˉ agrees on Δ l \Delta^l Δ l with the aggregate observation drift of β ~ \tilde{\beta} β ~ .
(ii) (First-order bounds on the simplex.) ∣ ∂ γ b ~ ˉ υ ( Σ ) ∣ ≤ B ~ + K ~ |\partial_\gamma\bar{\tilde{b}}^\upsilon(\Sigma)|\le\tilde{B}+\tilde{K} ∣ ∂ γ b ~ ˉ υ ( Σ ) ∣ ≤ B ~ + K ~ for all γ ∈ { 1 , … , l } \gamma\in\{1,\dots,l\} γ ∈ { 1 , … , l } and all Σ ∈ Δ l \Sigma\in\Delta^l Σ ∈ Δ l , and
∣ b ~ ˉ υ ( Σ ) − b ~ ˉ υ ( Σ ′ ) ∣ ≤ l ( B ~ + K ~ ) d ( Σ , Σ ′ ) for all Σ , Σ ′ ∈ Δ l . |\bar{\tilde{b}}^\upsilon(\Sigma)-\bar{\tilde{b}}^\upsilon(\Sigma')|\le\sqrt{l}\;(\tilde{B}+\tilde{K})\;d(\Sigma,\Sigma')\qquad\text{for all }\Sigma,\Sigma'\in\Delta^l. ∣ b ~ ˉ υ ( Σ ) − b ~ ˉ υ ( Σ ′ ) ∣ ≤ l ( B ~ + K ~ ) d ( Σ , Σ ′ ) for all Σ , Σ ′ ∈ Δ l .
(iii) (Second-order bounds and uniform continuity on the simplex.) ∣ ∂ δ ∂ γ b ~ ˉ υ ( Σ ) ∣ ≤ 3 K ~ |\partial_\delta\partial_\gamma\bar{\tilde{b}}^\upsilon(\Sigma)|\le3\,\tilde{K} ∣ ∂ δ ∂ γ b ~ ˉ υ ( Σ ) ∣ ≤ 3 K ~ for all γ , δ ∈ { 1 , … , l } \gamma,\delta\in\{1,\dots,l\} γ , δ ∈ { 1 , … , l } and Σ ∈ Δ l \Sigma\in\Delta^l Σ ∈ Δ l ; and for every real ε > 0 \varepsilon>0 ε > 0 there is a real δ ∘ > 0 \delta^\circ>0 δ ∘ > 0 , which may be chosen independently of γ \gamma γ , δ \delta δ , and υ \upsilon υ , such that ∣ ∂ δ ∂ γ b ~ ˉ υ ( Σ ) − ∂ δ ∂ γ b ~ ˉ υ ( Σ ′ ) ∣ ≤ ε |\partial_\delta\partial_\gamma\bar{\tilde{b}}^\upsilon(\Sigma)-\partial_\delta\partial_\gamma\bar{\tilde{b}}^\upsilon(\Sigma')|\le\varepsilon ∣ ∂ δ ∂ γ b ~ ˉ υ ( Σ ) − ∂ δ ∂ γ b ~ ˉ υ ( Σ ′ ) ∣ ≤ ε for all γ , δ ∈ { 1 , … , l } \gamma,\delta\in\{1,\dots,l\} γ , δ ∈ { 1 , … , l } , all υ ∈ { 1 , … , l ~ } \upsilon\in\{1,\dots,\tilde{l}\} υ ∈ { 1 , … , l ~ } , and all Σ , Σ ′ ∈ Δ l \Sigma,\Sigma'\in\Delta^l Σ , Σ ′ ∈ Δ l with d ( Σ , Σ ′ ) ≤ δ ∘ d(\Sigma,\Sigma')\le\delta^\circ d ( Σ , Σ ′ ) ≤ δ ∘ .