 # Solving HJB PDE using deep learning

Dear All,

sorry for bothering with a possibly stupid question.

I would like to ask for some advice about solving the Hamilton-Jacobi-Bellman equation using deep learning. I am trying to solve an HJB equation of a simple neoclassical growth model from macroeconomics. Its HJB equation is

\rho V(k_t) = \frac{c_t^{1-\gamma}}{1-\gamma} + \frac{\partial V}{\partial k} \{A k_t^\alpha - \delta k_t - c_t\}
Control variable in this problem is c_t \geq 0, characterized by following first-order condition.
c_t^{-\gamma} = \frac{\partial V}{\partial k}

Following paper by Fernandéz-Villaverde et. al (2020), I am trying to solve this HJB problem using deep learning. I parameterize the value function V(k_t) and consumption function C(k_t) using feed-forward networks designed to guarantee non-negativity of consumption, and use ADAM to minimize a loss function that includes squared error in HJB equation and FOC over a reasonable interval of state-space.
\mathcal{E}_{HJB} = \rho V(k_t) - \frac{c_t^{1-\gamma}}{1-\gamma} - \frac{\partial V}{\partial k} \{A k_t^\alpha - \delta k_t - c_t\}
\mathcal{E}_{FOC} = c_t^{-\gamma} - \frac{\partial V}{\partial k}
\mathcal{L} = \sum_i {\mathcal{E}_{HJB}}_i + \sum_i {\mathcal{E}_{FOC}}_i

While the minimization procedure converges to \approx 0 loss, instead of getting concave and increasing value function, I got something totally weird.

I checked the result for many different choices of activation functions in my networks, but the problem persists, in all these cases I still got this shape of the value function.

In the paper (page 19), the authors show, that minimization of this loss function composed of HJB and FOC error (should?) converges to a solution of accurate upwind finite-difference scheme. Unfortunately, I am getting something totally different. Should I use some boundary conditions? Unfortunately, I think that there aren’t natural boundary conditions in this problem, other than transversality conditions.

I would be really glad for any insight, especially from
@Tamas_Papp and @jlperla

Best,
Honza

Here is a MWE of my code.

#*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*
#*-*-* Solve non-stochastic neoclassical growth model in continuous time *-*
#*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*-*

#(1) Import libraries
using Pkg
using Plots
using Parameters
using LinearAlgebra
using Flux
using Random
using Distributions
using ForwardDiff
using ZygoteRules
ZygoteRules.@adjoint function ForwardDiff.Dual{T}(x, ẋ::Tuple) where T
@assert length(ẋ) == 1
ForwardDiff.Dual{T}(x, ẋ), ḋ -> (ḋ.partials, (ḋ.value,))
end
ZygoteRules.@adjoint ZygoteRules.literal_getproperty(d::ForwardDiff.Dual{T}, ::Val{:partials}) where T =
d.partials, ṗ -> (ForwardDiff.Dual{T}(ṗ, 0),)
ZygoteRules.@adjoint ZygoteRules.literal_getproperty(d::ForwardDiff.Dual{T}, ::Val{:value}) where T =
d.value, ẋ -> (ForwardDiff.Dual{T}(0, ẋ),)

#(2) Build model structure
function uCRRA(c,γ)
if(γ==1.0)
return log(c)
else
return (c^(1-γ))/(1-γ)
end
end
@with_kw struct NCG
#(A) Structural parameters
Α::Float32 = 0.5
α::Float32 = 0.36
β::Float32 = 1/(1+0.04)
ρ::Float32 = 1/β-1
γ::Float32 = 2.0
δ::Float32 = 0.05
kss::Float32 = (α/(1/β-(1-δ)))^(1/(1-α))
kl::Float32 = 10^(-4)
ku::Float32 = 10.0
#(C) Grid
ϰ::Int64 = 2500
𝓚::Array{Float32} = collect(range(kl,ku,length=ϰ))'
#(D) Approximator
T::Int64 = 8
g::Function = swish
end
@with_kw struct Optimizer
S1::Float32 = 0.0
S2::Float32 = 1.0
ϰ::Int64 = 2500
ϑ::Int64 = 150
T::Int64 = 32
Γ::Float32 = 0.001
β1::Float32 = 0.9
β2::Float32 = 0.99
ϵ::Float32 = 10^(-8)
ν::Float32 = 10^(-5)
𝚰::Int64 = 5000000
𝛀::Float32 = 0.1
𝒯::Int64 = 1500
𝓇::Float32 = 0.9
end

#Try swish,gelu,elu,mish,leakyrelu => all leads to the more or less same result
NC1 = NCG(g=swish)
@unpack Α,T,α,β,ρ,γ,δ,kl,ku,𝓚,g = NC1

#(3) Define approximation networks
#(3.1) Define policy network
𝓒 = Chain(Dense(1,T,g),Dense(T,T,g),
Dense(T,T,g),Dense(T,1,softplus))

#(3.3) Value network
𝓥 = Chain(Dense(1,T,g),Dense(T,T,g),
Dense(T,T,g),Dense(T,T,g),Dense(T,1,identity))
d𝓥(t) = ForwardDiff.derivative(x->𝓥([x]),t)
𝚹 = Flux.params(𝓒,𝓥)

#(4) Build production function
f(x) = Α*x^α - δ*x

#(4) Build a loss function
function 𝓡(x)
#HJB Error
ϵ_hjb = sum((ρ*𝓥(x) - uCRRA.(𝓒(x),γ) - d𝓥.(x).*(f.(x)-𝓒(x))).^2)
#FOC Error
ϵ_foc = sum((𝓒(x).^(-γ) - d𝓥.(x)).^2)
return ϵ_hjb+ϵ_foc
end

plot(𝓚',𝓥(𝓚)',title="Value Function",xlabel="K_t",ylabel="V(K),",legend=false)
plot(𝓚',d𝓥.(𝓚)',title="V_k(K)",xlabel="K_t",ylabel="V(K)",legend=false)
plot(𝓚',𝓒(𝓚)',title="Policy Function",xlabel="K_t",ylabel="C(K),",legend=false)



For replication, here is my implementation of the ADAM optimizer (FastADAM.jl file). There should’t be any problem, I used it sucessfully for many other problems.

function Adam(𝕱,𝚯,Data,Par,per,show,loc="NO")
let
#Initialize momentum estimates
@unpack ϑ,Γ,β1,β2,ϵ,𝚰,𝛀,𝒯,𝓇 = Par
n = length(𝚯)
m = Array{Array{Float32}}(undef,n)
v = Array{Array{Float32}}(undef,n)
∇ = Array{Array{Float32}}(undef,n)
hm = Array{Array{Float32}}(undef,n)
hv = Array{Array{Float32}}(undef,n)
u = Array{Array{Float32}}(undef,n)
if(loc=="YES")
𝚴 = Array{Array{Float32}}(undef,n)
𝕻 = [Array{Array{Float32}}(undef,n)]
𝕸 = Array{Float32}(undef,1)
𝖈 = Array{Int64}(undef,1)
𝕸 = 𝕱(Data)
𝖈 = 0
end
for j in 1:n
m[j] = zeros(Float32,length(𝚯[j]))
v[j] = zeros(Float32,length(𝚯[j]))
∇[j] = zeros(Float32,length(𝚯[j]))
end
#Main training loop
for i in 1:𝚰
𝓓,𝓜 = size(Data)
if(𝓓==1)
xg = reshape(sample(Data,ϑ),1,ϑ)
else
𝓘 = sample(1:𝓜,ϑ)
xg = Data[:,𝓘]
end
for j in 1:n
#Check duality
𝖙 = ForwardDiff.partials(∇𝕱[𝚯[j]])
if(length(𝖙)==1)
λ(t) = ForwardDiff.value(ForwardDiff.partials(∇𝕱[𝚯[j]][t]))
∇[j] = λ.(1:length(𝚯[j]))
else
∇[j] = Array{Float32,1}(∇𝕱[𝚯[j]][:])
end
#Update momentum estimates
m[j] = β1.*m[j] .+ (1-β1).*∇[j]
v[j] = β2.*v[j] .+ (1-β2).*∇[j].^2
hm[j] = m[j]./(1-β1^(i))
hv[j] = v[j]./(1-β2^(i))
#Update parameters
u[j] = hm[j]./(sqrt.(hv[j]) .+ ϵ)
𝚯[j] .= 𝚯[j] .- reshape(Γ.*u[j],size(𝚯[j]))
if(loc=="YES")
𝚴[j] = copy(𝚯[j] .- reshape(Γ.*u[j],size(𝚯[j])))
end
end
#Compute loss
if(i%per==0)
𝕷 = 𝕱(Data)
if(show=="YES")
#println(i)
println(𝕷)
end
#Secundary convergence check
if(loc=="YES")
if(𝕷<𝓇*𝕸)
𝕸 = 𝕷
𝕻 = 𝚴
𝖈 = 0
else
𝖈 = 𝖈 + 1
end
if(𝖈>=𝒯)
for j in 1:length(𝚯)
𝚯[j] .= 𝚴[j]
end
println("Secundary convergence")
return 𝚴
break
end
end
if(𝕷<𝛀)
println("Convergence ",i)
break
end
end
end
#
return 𝚯
end
end



Sorry, I am not familiar with deep learning. As you mention, there aren’t natural boundary conditions for these kind of problems.

In practice, I find that a good initial guess matters a lot. I usually find

@article{den2015exact,
title={Exact present solution with consistent future approximation: A gridless algorithm to solve stochastic dynamic models},
author={Den Haan, Wouter J and Kobielarz, Michal L and Rendahl, Pontus},
year={2015},
publisher={Centre For Macroeconomics}
}


useful for that purpose. I would start from this and then monitor the solver.

1 Like

@Tamas_Papp Thank you, I will try that! So, from your experience Chebyshev/Spline collocation tend to converge to the right solution of HJB even without imposing boundary conditions?

Yes. Again, with a good initial guess. That’s something I would invest in.

1 Like

@Honza9723 this looks really cool.

You want to restrict the neural network to be
1: monotonically increasing
2: strictly concave
I don’t know how to do this, but if someone else does I’m all ears (@ChrisRackauckas)…

More importantly, you wanna use the state boundary condition:
Let k_{min} be the minimum point in your capital grid.
Your transition function: \dot{k}=Ak^{\alpha} -\delta k -c \Rightarrow c(k,\dot{k}) =Ak^{\alpha} -\delta k -\dot{k}
At k_{min} when \dot{k}=0: c(k_{min},0) =Ak_{min}^{\alpha} -\delta k_{min}
state constraint boundary condition: V_k(k_{min}) \geq u'(c(k_{min},0) ) = u'(Ak_{min}^{\alpha} -\delta k_{min})
I’d love to see

Btw, I solve the non-stochastic NGM using much less fancy FD methods here.

Remark in passing: if you’re solving for the value function directly (rather than the marginal value function) and if you’re going to explore the logarithmic case, you may want to change the utility function to the standard \frac{c^{1-\gamma}-1}{1-\gamma} (i.e. don’t forget the -1).

2 Likes

I’m not sure how to do it other than imposing these charcteristics via sampling in the loss. Developing a neural network which enforces these properties is probably possible though? However, strictly concave might mean the best way to do it is to just impose a multi-quadratic and learn a representation of that.

3 Likes

Maybe you can use the NN to represent the second derivative (then you just need to enforce it to be negative) and integrate it to get the result?

Something is not right…

if V is decreasing, and the error from foc is small, consumption must be negative then. What if you change \gamma to a non-integer, say 2.1? This can force consumption to be positive (otherwise the c^{-\gamma} will yield NaN) and v to be increasing.

I don’t know too much about that paper and deep learning, but here is my general conjecture:

Boundary conditions are crucial in pinning down the exact solution to the PDE. Without proper defined boundary conditions it’s not surprising that you didn’t get anything sensible.

When the PDE is solved using upwinding, it effectively imposes reflective boundaries on the grid, and it can be shown that two boundary inequalities can uniquely determine the viscosity solution to the PDE (see Ben Moll’s note).

Here are some random thoughts that most likely won’t work, but probably worth a try:

I wonder if you could impose something like reflective boundaries using neural network, say force households to consume k down if k is large enough. This may be implicitly imposed already by the production function with depreciation, but since you are also learning the foc so who knows what would happen.

Or probably you could try to approximate the transversality condition, here \lim_{k\rightarrow 0} V'(k)=eps(), with a very large \bar k and small but positive eps(). It might be very inaccurate but at least gives you the right sign of c.

Hi @RangeFu

I tried to bypass this problem by imposing a state-constraint boundary condition that would pin down value function, but this boundary condition made the training process divergent (both ADAM and standard stochastic gradient descent diverged). From my experience, after starting from random (Xavier) initialization whole process is convergend for some time, but before it would reach reasonable loss level, it starts to diverge and then it gets trapped at some high loss level.

@Albert_Zevelev I tried to overcome this problem by employing monotonic network (just use increasing activation functions, and restrict parameters to be positive eg. by applying ReLU to them), but I got exactly the same problem => non-convergence.

I guess that those problems have something to do with the (degenerate) elliptic nature of the time-independent HJB. All the successful algorithms (for example Ben Moll’s implicit upwind FD method) implements some kind of false-transient method rather than directly attacking the original non-linear elliptic equation.

1 Like