Papers
Topics
Authors
Recent
Search
2000 character limit reached

Neural Expectation Operators

Updated 4 July 2026
  • Neural Expectation Operators are non-linear conditional expectation models defined by BSDE drivers parameterized via neural networks to capture ambiguity and model risk.
  • They ensure well-posedness under quadratic growth and local Lipschitz conditions, with architecture designs that enforce monotonicity and convexity.
  • The framework extends to Neural-Brownian Motion and learned measure changes, enabling robust applications in finance, stochastic control, and mean-field dynamics.

Neural Expectation Operators are non-linear conditional expectations induced by backward stochastic differential equations whose drivers are parameterized by neural networks. Within the paradigm of Measure Learning, they provide a probabilistic model of ambiguity—uncertainty over probability laws—by encoding attitude toward model misspecification directly in the BSDE driver. In the associated theory of Neural Brownian Motion, the same operator, written εθ\varepsilon^\theta, becomes the martingale notion relative to which a canonical stochastic process is defined, linking learned ambiguity to endogenous volatility and learned changes of measure (Qi, 13 Jul 2025, Qi, 19 Jul 2025).

1. BSDE definition and non-linear expectation structure

In its simplest form, a Neural Expectation Operator is induced by a neural BSDE

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,

where the driver fθf_\theta is computed by a neural network with parameters θ\theta. In the general setting, the driver also depends on a forward state process XX:

Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].

The operator acts as a non-linear conditional expectation via Yt=E[ξFt]Y_t = E[\xi\mid F_t]. In the notation used for Neural Brownian Motion, one defines

dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,

and sets εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t (Qi, 13 Jul 2025).

The economic and probabilistic content of the construction is that fθf_\theta compactly represents the structure of ambiguity. Quadratic growth in the martingale component Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,0 encodes risk and ambiguity aversion. Under suitable convexity and independence assumptions, the operator admits a dual representation over a family of measures related by Girsanov transforms: for drivers of the form Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,1, independent of Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,2 and convex in Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,3,

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,4

with Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,5 and Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,6 the (negative) Fenchel–Legendre transform of Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,7 in Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,8. In that sense, the non-linear expectation evaluates Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,9 under a worst-case change of measure from a learned universe of plausible models (Qi, 13 Jul 2025).

Classical linear conditional expectation is recovered when fθf_\theta0. In that case the BSDE reduces to the martingale representation with fθf_\theta1, so the neural construction is a strict generalization rather than a replacement of standard expectation.

2. Well-posedness under quadratic growth and local Lipschitz structure

The foundational well-posedness theorem is formulated for drivers satisfying continuity in fθf_\theta2, quadratic growth in fθf_\theta3, uniform local Lipschitz continuity in fθf_\theta4, and monotonicity in the sense that fθf_\theta5 is non-increasing. The terminal condition is required to satisfy exponential integrability, and the random part of the driver induced by the forward state fθf_\theta6 must satisfy an exponential integrability condition of the form

fθf_\theta7

The main theorem states that if fθf_\theta8, then there exists a unique adapted solution

fθf_\theta9

so θ\theta0 is essentially bounded and θ\theta1 is a BMO-martingale (Qi, 13 Jul 2025).

A notable feature of the result is that it circumvents the classical global Lipschitz assumption in the state variable θ\theta2. The theorem is explicitly described as applicable to common neural network architectures, including architectures with ReLU activations, and the exponential integrability condition on terminal data is described as the sharp condition for this setting. A priori estimates are obtained by comparison with dominating quadratic BSDEs. With auxiliary upper and lower generators, one shows

θ\theta3

which yields boundedness of θ\theta4 and BMO control of θ\theta5; uniqueness follows by strict comparison in θ\theta6 and identification of θ\theta7 via martingale representation (Qi, 13 Jul 2025).

A recurrent misconception is that neural parameterization necessarily weakens analytical control. The constructive objective of the theory is the opposite: it builds a bridge between the abstract assumptions of quadratic BSDE theory and concrete, verifiable neural network designs. In that sense, the learned operator is not an unconstrained black box, but a BSDE object whose solvability is tied to explicit structural hypotheses.

3. Architectural constraints and axiomatic properties

The theory includes constructive neural architectures that enforce the analytical assumptions required by quadratic BSDEs. A separable driver

θ\theta8

satisfies the uniform local Lipschitz property in θ\theta9 when XX0 is locally Lipschitz, and monotonicity when XX1 is chosen non-increasing. A bounded-interaction form

XX2

yields local Lipschitz continuity in XX3 provided XX4 is uniformly bounded and XX5 is locally Lipschitz (Qi, 13 Jul 2025).

Monotonicity can also be enforced directly by sign constraints. In a feed-forward network with non-decreasing activations, one imposes non-positive weights from XX6 to the first hidden layer and non-negative weights in subsequent hidden layers and in the output layer. A simple induction then gives XX7 everywhere, hence monotonicity. Convexity in XX8 can be imposed with Input-Convex Neural Networks. In that case convexity of the operator XX9 is guaranteed, and under convexity and monotonicity Jensen’s inequality holds:

Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].0

The same framework is described as encoding economically meaningful axioms such as monotonicity, time consistency, and, via ICNNs, convexity (Qi, 13 Jul 2025).

These constructions are important because they make the analytical hypotheses inspectable at the level of weights and activations. The operator’s qualitative properties are therefore not merely postulated; they can be enforced by architectural design.

4. Fully coupled forward–backward systems and mean-field asymptotics

The framework extends to fully coupled forward–backward stochastic differential equations of the form

Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].1

Under continuity and global Lipschitz conditions on Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].2, Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].3, and Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].4, together with the quadratic-growth, monotone-in-Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].5, and local-Lipschitz-in-Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].6 conditions on Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].7, and a small-time or small-Lipschitz condition Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].8, the system admits a unique adapted solution

Ys=ξ+sTfθ(r,Xr,Yr,Zr)drsTZrdWr,s[t,T].Y_s = \xi + \int_s^T f_\theta(r, X_r, Y_r, Z_r)\,dr - \int_s^T Z_r\,dW_r, \quad s\in[t,T].9

for any Yt=E[ξFt]Y_t = E[\xi\mid F_t]0 (Qi, 13 Jul 2025).

The proof follows the four-step scheme. One identifies a quasilinear parabolic PDE for Yt=E[ξFt]Y_t = E[\xi\mid F_t]1, with the quadratic Yt=E[ξFt]Y_t = E[\xi\mid F_t]2-dependence entering through Yt=E[ξFt]Y_t = E[\xi\mid F_t]3; one then uses viscosity solution theory and comparison to obtain a unique spatially Lipschitz solution Yt=E[ξFt]Y_t = E[\xi\mid F_t]4; finally one reconstructs Yt=E[ξFt]Y_t = E[\xi\mid F_t]5 by the Markovian ansatz Yt=E[ξFt]Y_t = E[\xi\mid F_t]6 and Yt=E[ξFt]Y_t = E[\xi\mid F_t]7 (Qi, 13 Jul 2025).

The same program is pushed to interacting particle systems. For exchangeable particles with empirical law Yt=E[ξFt]Y_t = E[\xi\mid F_t]8, the theory establishes a Law of Large Numbers, described as propagation of chaos, and a Central Limit Theorem. The LLN states that, for each particle index Yt=E[ξFt]Y_t = E[\xi\mid F_t]9,

dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,0

Under differentiability of the coefficients in dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,1 and Lions differentiability in the measure argument, the centered fluctuations converge in law to the unique solution of a linear McKean–Vlasov FBSDE. Because the fluctuation dynamics are linear and driven by Brownian inputs, the limit law is Gaussian (Qi, 13 Jul 2025).

5. Self-referential martingales and canonical Neural-Brownian Motion

A particularly distinctive development is the use of the Neural Expectation Operator to define a new martingale notion. For self-referential processes, the driver is specialized by identifying the value and state variables with the process itself:

dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,2

A one-dimensional process dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,3 is then called a Neural-Brownian Motion if it is continuous, dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,4, and is an dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,5-martingale it generates:

dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,6

It is canonical if it has zero drift under the physical measure dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,7 (Qi, 19 Jul 2025).

If dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,8 is an Itô process

dYs=fθ(s,Xs,Ys,Zs)dsZsdWs,YT=ξ,- dY_s = f_\theta(s, X_s, Y_s, Z_s) ds - Z_s dW_s, \qquad Y_T = \xi,9

then εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t0 is an εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t1-martingale if and only if

εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t2

for almost every εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t3. The canonical condition εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t4 therefore implies the algebraic constraint

εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t5

so the volatility is characterized as a root of εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t6 rather than postulated a priori. Under the implicit volatility assumption that, for each εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t7, the equation εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t8 has a unique positive root εθ[ξFt]:=Yt\varepsilon^\theta[\xi \mid F_t] := Y_t9, that the root is regular, and that fθf_\theta0 has global linear growth, the canonical Neural-Brownian Motion exists and is the unique strong solution of

fθf_\theta1

The regular root condition yields fθf_\theta2 regularity of fθf_\theta3 via the Implicit Function Theorem, and local Lipschitz continuity in fθf_\theta4 follows immediately (Qi, 19 Jul 2025).

This produces a learned stochastic calculus in which the infinitesimal generator is

fθf_\theta5

The volatility fθf_\theta6 is endogenous: it emerges as the unique positive root of fθf_\theta7 and is therefore learned from the ambiguity structure encoded by the driver. The process is correspondingly no longer characterized by stationary independent increments; its volatility is state- and driver-dependent, learned from data (Qi, 19 Jul 2025).

In the quadratic specialized case

fθf_\theta8

with fθf_\theta9 and Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,00, the canonical constraint yields a constant volatility

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,01

Under Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,02,

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,03

so Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,04 is a scaled Brownian motion. Defining a new measure Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,05 by the Radon–Nikodym density with kernel Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,06,

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,07

one obtains a Girsanov-type theorem: Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,08 is a Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,09-Brownian motion and

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,10

Thus a canonical Neural-Brownian Motion acquires a drift under the learned measure. The sign of Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,11 determines the interpretation: Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,12 corresponds to a convex driver and is interpreted as ambiguity aversion, whereas Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,13 corresponds to a concave driver and is interpreted as ambiguity seeking (Qi, 19 Jul 2025).

From the computational side, the framework is designed for learning from data. Neural Expectation Operators are computed by solving the BSDE for Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,14 given Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,15 and Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,16, and training Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,17 is described as well-posed because the theory provides a sensitivity BSDE that yields exact gradients for Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,18. If Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,19 and the driver is differentiable in Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,20, then the gradient processes Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,21 solve the linear BSDE

Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,22

with Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,23, which enables principled gradient-based learning with SGD or Adam (Qi, 13 Jul 2025).

The stated application domain includes stochastic control, robust finance, and macro models of systemic ambiguity. A concrete example is the Merton portfolio problem under the driver Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,24, which is described as consistent with the theory and as predicting ambiguity-induced caution; the optimal policy is wealth-dependent and strictly more conservative than the classical Merton strategy, with the ambiguity parameter Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,25 estimable from data via the sensitivity machinery. In the Neural-Brownian Motion formulation, the same learned-volatility mechanism is presented as opening principled applications such as consistent implicit-volatility models in finance, while also opening a path to mean-field limits when interactions are introduced through measure-dependent drivers (Qi, 13 Jul 2025, Qi, 19 Jul 2025).

Neural Expectation Operators should be distinguished from methods that estimate linear expectations through PDE surrogates. The Feynman–Kac Operator Expectation Estimator, for example, estimates Yt=ξ+tTfθ(s,Ys,Zs)dstTZsdWs,Y_t = \xi + \int_t^T f_\theta(s,Y_s,Z_s)\,ds - \int_t^T Z_s\,dW_s,26 by combining diffusion bridge models with approximation of the Feynman–Kac operator using Physically Informed Neural Networks. That construction is an expectation estimator for a target mathematical expectation, whereas Neural Expectation Operators define a non-linear conditional expectation itself through a BSDE driver and are expressly designed to model ambiguity (Li et al., 2024).

Definition Search Book Streamline Icon: https://streamlinehq.com
References (3)

Topic to Video (Beta)

No one has generated a video about this topic yet.

Whiteboard

No one has generated a whiteboard explanation for this topic yet.

Follow Topic

Get notified by email when new papers are published related to Neural Expectation Operators.