Adopt the setting of the \reftext{lem:n-agent-compensated-martingales-2026a}{compensated counters of the controlled N N N -agent dynamics}: a \reftext{def:transition-rate-family-2026a}{transition-rate family} Ξ² \beta Ξ² with rate bound B B B on l l l states with control dimension m m m , an \reftext{def:observation-rate-family-2026a}{observation-rate family} Ξ² ~ \tilde{\beta} Ξ² ~ β with rate bound B ~ \tilde{B} B ~ and l ~ \tilde{l} l ~ channels, a horizon T > 0 T>0 T > 0 , an \reftext{def:n-agent-driving-system-2026a}{N N N -agent driving system} ( Ξ© , F , P ) (\Omega,\mathcal{F},P) ( Ξ© , F , P ) , an \reftext{def:observation-driven-control-policy-2026a}{observation-driven control policy} h h h , and a \reftext{def:n-agent-controlled-dynamics-2026a}{solution} on [ 0 , T ] [0,T] [ 0 , T ] with regular event Ξ© 0 \Omega_0 Ξ© 0 β , state processes Ο i \sigma^i Ο i , empirical state measure Ξ£ t \Sigma_t Ξ£ t β , observation counters N ~ t i , Ο
\tilde{N}^{i,\upsilon}_t N ~ t i , Ο
β , consumed clock times A ~ t i , Ο
\tilde{A}^{i,\upsilon}_t A ~ t i , Ο
β , observation total c ~ t \tilde{c}_t c ~ t β , and system filtration ( F t s y s ) t β [ 0 , T ] (\mathcal{F}^{\mathrm{sys}}_t)_{t\in[0,T]} ( F t sys β ) t β [ 0 , T ] β . Write M t ( i , Ο
) = N ~ t i , Ο
β A ~ t i , Ο
M^{(i,\upsilon)}_t=\tilde{N}^{i,\upsilon}_t-\tilde{A}^{i,\upsilon}_t M t ( i , Ο
) β = N ~ t i , Ο
β β A ~ t i , Ο
β for the compensated counters of the \reftext{lem:n-agent-compensated-martingales-2026a}{compensated-counters lemma} attached to the \textbf{observation clock labels} a = ( i , Ο
) a=(i,\upsilon) a = ( i , Ο
) , i β { 1 , β¦ , N } i\in\{1,\dots,N\} i β { 1 , β¦ , N } , Ο
β { 1 , β¦ , l ~ } \upsilon\in\{1,\dots,\tilde{l}\} Ο
β { 1 , β¦ , l ~ } ; at every Ο β Ξ© 0 \omega\in\Omega_0 Ο β Ξ© 0 β let Ο 1 < β― < Ο c ~ T \tau_1<\dots<\tau_{\tilde{c}_T} Ο 1 β < β― < Ο c ~ T β β be the jump times of the observation total in [ 0 , T ] [0,T] [ 0 , T ] and Ο
1 , β¦ , Ο
c ~ T \upsilon_1,\dots,\upsilon_{\tilde{c}_T} Ο
1 β , β¦ , Ο
c ~ T β β their channels, as in condition 5 of the \reftext{def:n-agent-controlled-dynamics-2026a}{solution definition} (where c ~ t \tilde{c}_t c ~ t β is written K t K_t K t β ). Let b ~ \tilde{b} b ~ be the \reftext{def:aggregate-observation-drift-2026a}{aggregate observation drift} of Ξ² ~ \tilde{\beta} Ξ² ~ β , with b ~ ( Ξ£ ) \tilde{b}(\Sigma) b ~ ( Ξ£ ) the vector with components b ~ 1 ( Ξ£ ) , β¦ , b ~ l ~ ( Ξ£ ) \tilde{b}^1(\Sigma),\dots,\tilde{b}^{\tilde{l}}(\Sigma) b ~ 1 ( Ξ£ ) , β¦ , b ~ l ~ ( Ξ£ ) , and let M t Ξ³ M^\gamma_t M t Ξ³ β (Ξ³ β { 1 , β¦ , l } \gamma\in\{1,\dots,l\} Ξ³ β { 1 , β¦ , l } ) be the state martingales of the \reftext{thm:n-agent-martingale-decomposition-2026a}{martingale decomposition}. Write E \mathbb{E} E for the \reftext{def:expectation-variance-2026a}{expectation}, \reftext{def:square-integrable-mean-square-2026a}{square-integrable} for membership in the mean-square space, \reftext{def:lebesgue-integral-integrable-2026a}{integrable} for finiteness of the expectation of the absolute value, 1 D \mathbf{1}_D 1 D β for the function equal to 1 1 1 on a set D D D and 0 0 0 off D D D , e Ο
e_\upsilon e Ο
β for the Ο
\upsilon Ο
-th standard basis vector of \reftext{def:euclidean-space-rn-2026a}{Euclidean space} R l ~ \mathbb{R}^{\tilde{l}} R l ~ , and N = N 1 / 2 \sqrt{N}=N^{1/2} N β = N 1/2 for the \reftext{thm:nonnegative-real-has-unique-square-root-2026a}{nonnegative square root}; vectors are identified with one-column matrices and products of matrices are \reftext{def:product-real-matrices-2026a}{matrix products}, with ( β
) β€ (\cdot)^{\top} ( β
) β€ the \reftext{def:transpose-real-matrix-2026a}{transpose}.
Fix a natural number d β₯ 1 d\ge1 d β₯ 1 and an assignment F F F of a real matrix F t F_t F t β with d d d rows and l ~ \tilde{l} l ~ columns to each t β [ 0 , T ] t\in[0,T] t β [ 0 , T ] such that every entry map t β¦ F t Ξ³ Ο
t\mapsto F^{\gamma\upsilon}_t t β¦ F t Ξ³ Ο
β is \reftext{def:continuity-closed-interval-c54-2026b}{continuous} on [ 0 , T ] [0,T] [ 0 , T ] , and fix a real F Λ β₯ 0 \bar{F}\ge0 F Λ β₯ 0 with β£ F t Ξ³ Ο
β£ β€ F Λ |F^{\gamma\upsilon}_t|\le\bar{F} β£ F t Ξ³ Ο
β β£ β€ F Λ for all Ξ³ \gamma Ξ³ , Ο
\upsilon Ο
, t t t (such a bound exists because continuous functions on a compact interval are \reftext{lem:continuous-compact-interval-bounded-2026a}{bounded}). Let likewise G G G be an assignment of real matrices with d β² d' d β² rows and l ~ \tilde{l} l ~ columns with continuous entries and entry bound G Λ \bar{G} G Λ . Define, for t β [ 0 , T ] t\in[0,T] t β [ 0 , T ] and at every Ο β Ξ© \omega\in\Omega Ο β Ξ© , the \textbf{weighted observation sum} and the \textbf{weighted compensated observation sum}
J t F = N β 1 / 2 β j = 1 c ~ t F Ο j β e Ο
j β R d , J ~ t F = J t F β N 1 / 2 β« [ 0 , t ] F r β 1 Ξ© 0 b ~ ( Ξ£ r ) β d r β R d , J^{F}_t=N^{-1/2}\sum_{j=1}^{\tilde{c}_t}F_{\tau_j}\,e_{\upsilon_j}\in\mathbb{R}^{d},\qquad\qquad \tilde{J}^{F}_t=J^{F}_t-N^{1/2}\int_{[0,t]}F_r\,\mathbf{1}_{\Omega_0}\tilde{b}(\Sigma_r)\,dr\in\mathbb{R}^{d}, J t F β = N β 1/2 j = 1 β c ~ t β β F Ο j β β e Ο
j β β β R d , J ~ t F β = J t F β β N 1/2 β« [ 0 , t ] β F r β 1 Ξ© 0 β β b ~ ( Ξ£ r β ) d r β R d ,
where the sum is 0 0 0 when c ~ t = 0 \tilde{c}_t=0 c ~ t β = 0 (in particular off Ξ© 0 \Omega_0 Ξ© 0 β , where all counters vanish), and the integral is the componentwise \reftext{lem:interval-lebesgue-toolkit-2026a}{Lebesgue integral over the compact interval} [ 0 , t ] [0,t] [ 0 , t ] of an integrand with values bounded by F Λ β l ~ β B ~ \bar{F}\,\tilde{l}\,\tilde{B} F Λ l ~ B ~ in absolute value whose sections in r r r are measurable by conclusion (a) (in particular the integrand, and hence the integral, is well defined and equal to 0 0 0 at every Ο β Ξ© 0 \omega\notin\Omega_0 Ο β / Ξ© 0 β , where the factor 1 Ξ© 0 \mathbf{1}_{\Omega_0} 1 Ξ© 0 β β vanishes identically), the integral being 0 0 0 for t = 0 t=0 t = 0 .
\textbf{(a) (Representation and regularity.)} At every Ο β Ξ© 0 \omega\in\Omega_0 Ο β Ξ© 0 β : for each Ο
\upsilon Ο
, the jump times in [ 0 , T ] [0,T] [ 0 , T ] of the path t β¦ β i = 1 N N ~ t i , Ο
t\mapsto\sum_{i=1}^{N}\tilde{N}^{i,\upsilon}_t t β¦ β i = 1 N β N ~ t i , Ο
β are exactly the Ο j \tau_j Ο j β with Ο
j = Ο
\upsilon_j=\upsilon Ο
j β = Ο
, each jump having size 1 1 1 ; the identity
β i = 1 N A ~ t i , Ο
= N β« [ 0 , t ] b ~ Ο
( Ξ£ s ) β d s \sum_{i=1}^{N}\tilde{A}^{i,\upsilon}_t=N\int_{[0,t]}\tilde{b}^\upsilon(\Sigma_s)\,ds i = 1 β N β A ~ t i , Ο
β = N β« [ 0 , t ] β b ~ Ο
( Ξ£ s β ) d s
holds for every t β [ 0 , T ] t\in[0,T] t β [ 0 , T ] and every Ο
\upsilon Ο
; and for all 0 β€ r β€ t β€ T 0\le r\le t\le T 0 β€ r β€ t β€ T and every Ξ³ β { 1 , β¦ , d } \gamma\in\{1,\dots,d\} Ξ³ β { 1 , β¦ , d } ,
β£ J t F , Ξ³ β£ β€ F Λ β N β 1 / 2 β c ~ t and β£ J ~ t F , Ξ³ β J ~ r F , Ξ³ β£ β€ F Λ β ( N β 1 / 2 ( c ~ t β c ~ r ) + N 1 / 2 β l ~ β B ~ β ( t β r ) ) , |J^{F,\gamma}_t|\le\bar{F}\,N^{-1/2}\,\tilde{c}_t\qquad\text{and}\qquad|\tilde{J}^{F,\gamma}_t-\tilde{J}^{F,\gamma}_r|\le\bar{F}\,\big(N^{-1/2}(\tilde{c}_t-\tilde{c}_r)+N^{1/2}\,\tilde{l}\,\tilde{B}\,(t-r)\big), β£ J t F , Ξ³ β β£ β€ F Λ N β 1/2 c ~ t β and β£ J ~ t F , Ξ³ β β J ~ r F , Ξ³ β β£ β€ F Λ ( N β 1/2 ( c ~ t β β c ~ r β ) + N 1/2 l ~ B ~ ( t β r ) ) ,
and every path t β¦ J ~ t F , Ξ³ t\mapsto\tilde{J}^{F,\gamma}_t t β¦ J ~ t F , Ξ³ β is right-continuous on [ 0 , T ] [0,T] [ 0 , T ] with J ~ 0 F = 0 \tilde{J}^{F}_0=0 J ~ 0 F β = 0 . Moreover, for every Ο
β { 1 , β¦ , l ~ } \upsilon\in\{1,\dots,\tilde{l}\} Ο
β { 1 , β¦ , l ~ } , the map s β¦ 1 Ξ© 0 b ~ Ο
( Ξ£ s ) s\mapsto\mathbf{1}_{\Omega_0}\tilde{b}^\upsilon(\Sigma_s) s β¦ 1 Ξ© 0 β β b ~ Ο
( Ξ£ s β ) is a section of a map that is \reftext{def:measurable-function-2026a}{measurable} for the \reftext{def:product-sigma-algebra-2026a}{product Ο \sigma Ο -algebra} of the \reftext{lem:interval-lebesgue-toolkit-2026a}{trace Borel Ο \sigma Ο -algebra} on [ 0 , T ] [0,T] [ 0 , T ] and F \mathcal{F} F ; for every t β [ 0 , T ] t\in[0,T] t β [ 0 , T ] and Ξ³ β { 1 , β¦ , d } \gamma\in\{1,\dots,d\} Ξ³ β { 1 , β¦ , d } , J ~ t F , Ξ³ \tilde{J}^{F,\gamma}_t J ~ t F , Ξ³ β is a \reftext{def:probability-space-random-variable-2026a}{random variable} that is measurable with respect to F t s y s \mathcal{F}^{\mathrm{sys}}_t F t sys β , with E [ β£ J ~ t F , Ξ³ β£ p ] < β \mathbb{E}\big[|\tilde{J}^{F,\gamma}_t|^{p}\big]<\infty E [ β£ J ~ t F , Ξ³ β β£ p ] < β for every natural number p β₯ 1 p\ge1 p β₯ 1 ; and for every Ξ³ β { 1 , β¦ , d } \gamma\in\{1,\dots,d\} Ξ³ β { 1 , β¦ , d } , the map ( t , Ο ) β¦ 1 Ξ© 0 ( Ο ) β J ~ t F , Ξ³ ( Ο ) (t,\omega)\mapsto\mathbf{1}_{\Omega_0}(\omega)\,\tilde{J}^{F,\gamma}_t(\omega) ( t , Ο ) β¦ 1 Ξ© 0 β β ( Ο ) J ~ t F , Ξ³ β ( Ο ) is product-measurable.
\textbf{(b) (First-order identity.)} Let r β [ 0 , T ] r\in[0,T] r β [ 0 , T ] and let Z Z Z be an F r s y s \mathcal{F}^{\mathrm{sys}}_r F r sys β -measurable square-integrable random variable. Then for every t β [ r , T ] t\in[r,T] t β [ r , T ] and every Ξ³ β { 1 , β¦ , d } \gamma\in\{1,\dots,d\} Ξ³ β { 1 , β¦ , d } the product Z β ( J ~ t F , Ξ³ β J ~ r F , Ξ³ ) Z\,(\tilde{J}^{F,\gamma}_t-\tilde{J}^{F,\gamma}_r) Z ( J ~ t F , Ξ³ β β J ~ r F , Ξ³ β ) is integrable and
E [ Z β ( J ~ t F , Ξ³ β J ~ r F , Ξ³ ) ] = 0. \mathbb{E}\big[Z\,\big(\tilde{J}^{F,\gamma}_t-\tilde{J}^{F,\gamma}_r\big)\big]=0 . E [ Z ( J ~ t F , Ξ³ β β J ~ r F , Ξ³ β ) ] = 0.
In particular (taking Z = 1 D Z=\mathbf{1}_D Z = 1 D β , D β F r s y s D\in\mathcal{F}^{\mathrm{sys}}_r D β F r sys β ) each component ( J ~ t F , Ξ³ ) t β [ 0 , T ] (\tilde{J}^{F,\gamma}_t)_{t\in[0,T]} ( J ~ t F , Ξ³ β ) t β [ 0 , T ] β is a \reftext{def:square-integrable-martingale-2026a}{square-integrable martingale} with respect to ( F t s y s ) t β [ 0 , T ] (\mathcal{F}^{\mathrm{sys}}_t)_{t\in[0,T]} ( F t sys β ) t β [ 0 , T ] β (time index restricted to [ 0 , T ] [0,T] [ 0 , T ] ), vanishing at 0 0 0 almost surely.
\textbf{(c) (Second-order identity.)} Let r β [ 0 , T ] r\in[0,T] r β [ 0 , T ] and let Z Z Z be an F r s y s \mathcal{F}^{\mathrm{sys}}_r F r sys β -measurable random variable whose square Z 2 Z^2 Z 2 is square-integrable. Then for every t β [ r , T ] t\in[r,T] t β [ r , T ] , every Ξ³ β { 1 , β¦ , d } \gamma\in\{1,\dots,d\} Ξ³ β { 1 , β¦ , d } , and every Ξ΄ β { 1 , β¦ , d β² } \delta\in\{1,\dots,d'\} Ξ΄ β { 1 , β¦ , d β² } , the products below are integrable and
E [ Z β ( J ~ t F , Ξ³ β J ~ r F , Ξ³ ) ( J ~ t G , Ξ΄ β J ~ r G , Ξ΄ ) ] = E [ Z β« [ r , t ] β Ο
= 1 l ~ F s Ξ³ Ο
β G s Ξ΄ Ο
β b ~ Ο
( Ξ£ s ) β d s ] , \mathbb{E}\Big[Z\,\big(\tilde{J}^{F,\gamma}_t-\tilde{J}^{F,\gamma}_r\big)\big(\tilde{J}^{G,\delta}_t-\tilde{J}^{G,\delta}_r\big)\Big]=\mathbb{E}\Big[Z\int_{[r,t]}\sum_{\upsilon=1}^{\tilde{l}}F^{\gamma\upsilon}_s\,G^{\delta\upsilon}_s\,\tilde{b}^\upsilon(\Sigma_s)\,ds\Big], E [ Z ( J ~ t F , Ξ³ β β J ~ r F , Ξ³ β ) ( J ~ t G , Ξ΄ β β J ~ r G , Ξ΄ β ) ] = E [ Z β« [ r , t ] β Ο
= 1 β l ~ β F s Ξ³ Ο
β G s Ξ΄ Ο
β b ~ Ο
( Ξ£ s β ) d s ] ,
the inner integral existing at every Ο \omega Ο as the Lebesgue integral over [ r , t ] [r,t] [ r , t ] of a measurable function bounded in absolute value by F Λ G Λ l ~ B ~ \bar{F}\bar{G}\tilde{l}\tilde{B} F Λ G Λ l ~ B ~ . In particular, with Z = 1 Z=1 Z = 1 and r = 0 r=0 r = 0 : writing D ( Ξ£ ) D(\Sigma) D ( Ξ£ ) for the diagonal matrix with l ~ \tilde{l} l ~ rows and columns and diagonal entries b ~ 1 ( Ξ£ ) , β¦ , b ~ l ~ ( Ξ£ ) \tilde{b}^1(\Sigma),\dots,\tilde{b}^{\tilde{l}}(\Sigma) b ~ 1 ( Ξ£ ) , β¦ , b ~ l ~ ( Ξ£ ) ,
E [ J ~ t F , Ξ³ β J ~ t G , Ξ΄ ] = E [ β« [ 0 , t ] ( F s β D ( Ξ£ s ) β G s β€ ) Ξ³ Ξ΄ β d s ] , \mathbb{E}\big[\tilde{J}^{F,\gamma}_t\,\tilde{J}^{G,\delta}_t\big]=\mathbb{E}\Big[\int_{[0,t]}\big(F_s\,D(\Sigma_s)\,G_s^{\top}\big)^{\gamma\delta}\,ds\Big], E [ J ~ t F , Ξ³ β J ~ t G , Ξ΄ β ] = E [ β« [ 0 , t ] β ( F s β D ( Ξ£ s β ) G s β€ β ) Ξ³ Ξ΄ d s ] ,
and, specializing G = F G=F G = F , d β² = d d'=d d β² = d , and Ξ΄ = Ξ³ \delta=\gamma Ξ΄ = Ξ³ ,
E [ ( J ~ t F , Ξ³ ) 2 ] β€ F Λ 2 β l ~ β B ~ β t . \mathbb{E}\big[(\tilde{J}^{F,\gamma}_t)^{2}\big]\le\bar{F}^{2}\,\tilde{l}\,\tilde{B}\,t . E [ ( J ~ t F , Ξ³ β ) 2 ] β€ F Λ 2 l ~ B ~ t .
\textbf{(d) (Cross identity with the state martingales.)} Let r r r and Z Z Z be as in (c). Then for every t β [ r , T ] t\in[r,T] t β [ r , T ] , every Ξ³ β { 1 , β¦ , l } \gamma\in\{1,\dots,l\} Ξ³ β { 1 , β¦ , l } , and every Ξ΄ β { 1 , β¦ , d } \delta\in\{1,\dots,d\} Ξ΄ β { 1 , β¦ , d } , the product below is integrable and
E [ Z β ( M t Ξ³ β M r Ξ³ ) ( J ~ t F , Ξ΄ β J ~ r F , Ξ΄ ) ] = 0. \mathbb{E}\Big[Z\,\big(M^{\gamma}_t-M^{\gamma}_r\big)\big(\tilde{J}^{F,\delta}_t-\tilde{J}^{F,\delta}_r\big)\Big]=0 . E [ Z ( M t Ξ³ β β M r Ξ³ β ) ( J ~ t F , Ξ΄ β β J ~ r F , Ξ΄ β ) ] = 0.
\textbf{(e) (Fourth-moment bound.)} For every t β [ 0 , T ] t\in[0,T] t β [ 0 , T ] and every Ξ³ β { 1 , β¦ , d } \gamma\in\{1,\dots,d\} Ξ³ β { 1 , β¦ , d } ,
E [ ( J ~ t F , Ξ³ ) 4 ] Β β€ Β 11 β ( 1 + F Λ ) 4 β ( 1 + l ~ β B ~ β T ) 2 Β < Β β ; \mathbb{E}\big[(\tilde{J}^{F,\gamma}_t)^{4}\big]\ \le\ 11\,(1+\bar{F})^{4}\,\big(1+\tilde{l}\,\tilde{B}\,T\big)^{2}\ <\ \infty ; E [ ( J ~ t F , Ξ³ β ) 4 ] Β β€ Β 11 ( 1 + F Λ ) 4 ( 1 + l ~ B ~ T ) 2 Β < Β β ;
in particular the bound does not depend on N N N , on the driving system, or on the solution.