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1 change: 1 addition & 0 deletions docs/src/api.md
Original file line number Diff line number Diff line change
Expand Up @@ -8,6 +8,7 @@ This modularity means that different HMC variants can be easily constructed by c
- Unit metric: `UnitEuclideanMetric(dim)`
- Diagonal metric: `DiagEuclideanMetric(dim)`
- Dense metric: `DenseEuclideanMetric(dim)`
- Rank update metric: `RankUpdateEuclideanMetric(dim)`

where `dim` is the dimensionality of the sampling space.

Expand Down
16 changes: 14 additions & 2 deletions src/AdvancedHMC.jl
Original file line number Diff line number Diff line change
Expand Up @@ -2,7 +2,18 @@ module AdvancedHMC

using Statistics: mean, var, middle
using LinearAlgebra:
Symmetric, UpperTriangular, mul!, ldiv!, dot, I, diag, cholesky, UniformScaling
Symmetric,
UpperTriangular,
mul!,
ldiv!,
dot,
I,
diag,
cholesky,
UniformScaling,
Diagonal,
qr,
lmul!
using StatsFuns: logaddexp, logsumexp, loghalf
using Random: Random, AbstractRNG
using ProgressMeter: ProgressMeter
Expand Down Expand Up @@ -40,7 +51,8 @@ struct GaussianKinetic <: AbstractKinetic end
export GaussianKinetic

include("metric.jl")
export UnitEuclideanMetric, DiagEuclideanMetric, DenseEuclideanMetric
export UnitEuclideanMetric,
DiagEuclideanMetric, DenseEuclideanMetric, RankUpdateEuclideanMetric

include("hamiltonian.jl")
export Hamiltonian
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19 changes: 19 additions & 0 deletions src/hamiltonian.jl
Original file line number Diff line number Diff line change
Expand Up @@ -61,6 +61,18 @@ function ∂H∂r(h::Hamiltonian{<:DenseEuclideanMetric,<:GaussianKinetic}, r::A
return M⁻¹ * r
end

function ∂H∂r(
h::Hamiltonian{<:RankUpdateEuclideanMetric,<:GaussianKinetic}, r::AbstractVecOrMat
)
(; M⁻¹) = h.metric
axes_M⁻¹ = __axes(M⁻¹)
axes_r = __axes(r)
(first(axes_M⁻¹) !== first(axes_r)) && throw(
ArgumentError("AxesMismatch: M⁻¹ has axes $(axes_M⁻¹) but r has axes $(axes_r)")
)
return M⁻¹ * r
end

# TODO (kai) make the order of θ and r consistent with neg_energy
# TODO (kai) add stricter types to block hamiltonian.jl#L37 from working on unknown metric/kinetic
# The gradient of a position-dependent Hamiltonian system depends on both θ and r.
Expand Down Expand Up @@ -165,6 +177,13 @@ function neg_energy(
return -dot(r, h.metric._temp) / 2
end

function neg_energy(
h::Hamiltonian{<:RankUpdateEuclideanMetric,<:GaussianKinetic}, r::T, θ::T
) where {T<:AbstractVecOrMat}
M⁻¹ = h.metric.M⁻¹
return -r' * M⁻¹ * r / 2
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end

energy(args...) = -neg_energy(args...)

####
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94 changes: 94 additions & 0 deletions src/metric.jl
Original file line number Diff line number Diff line change
Expand Up @@ -98,6 +98,84 @@ function Base.show(io::IO, dem::DenseEuclideanMetric)
return print(io, "DenseEuclideanMetric(diag=$(_string_M⁻¹(dem.M⁻¹)))")
end

"""
RankUpdateEuclideanMetric{T,AM,AB,AD,F} <: AbstractMetric
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Suggested change
RankUpdateEuclideanMetric{T,AM,AB,AD,F} <: AbstractMetric
RankUpdateEuclideanMetric{T,AM<:AbstractVecOrMat{T},AB,AD,F} <: AbstractMetric


A Gaussian Euclidean metric whose inverse is constructed by rank-updates.
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Suggested change
A Gaussian Euclidean metric whose inverse is constructed by rank-updates.
A Gaussian Euclidean metric whose inverse is constructed by low-rank updates to a diagonal matrix.


# Fields

$(TYPEDFIELDS)

# Constructors

RankUpdateEuclideanMetric(n::Int)
RankUpdateEuclideanMetric(M⁻¹, B, D)

- Construct a Gaussian Euclidean metric of size `(n, n)` with `M⁻¹` being diagonal matrix.
- Construct a Gaussian Euclidean metric of `M⁻¹`, where `M⁻¹` should be a full rank positive definite matrix,
and `B` `D` must be chose so that the Woodbury matrix `W = M⁻¹ + B D B^\\mathrm{T}` is positive definite.
Comment on lines +115 to +117
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For the other metrics M⁻¹ is defined as the inverse of the metric. Wouldn't it be more consistent to here define M⁻¹ = A + B D B' as the inverse metric and require A be diagonal and positive-definite? (also, "full-rank" for diagonal PD-mat is redundant).

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For Pathfinder to safely convert its WoodburyPDMat to this type, we'll need the contents/form of the factorization field to be documented.

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Suggested change
and `B` `D` must be chose so that the Woodbury matrix `W = M⁻¹ + B D B^\\mathrm{T}` is positive definite.
and `B` `D` must be chosen so that the Woodbury matrix `W = M⁻¹ + B D B^\\mathrm{T}` is positive definite.


# Example

```julia
julia> RankUpdateEuclideanMetric(3)
RankUpdateEuclideanMetric(diag=[1.0, 1.0, 1.0])
```

# References

- Ben Bales, Arya Pourzanjani, Aki Vehtari, Linda Petzold, Selecting the Metric in Hamiltonian Monte Carlo, 2019
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The factorized form used here is due to the Pathfinder paper, so I recommend also citing http://jmlr.org/papers/v23/21-0889.html

"""
struct RankUpdateEuclideanMetric{T,AM<:AbstractVecOrMat{T},AB,AD,F} <: AbstractMetric
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More a question than a request: Is there a reason why AM can be a Vector? Also, is it intentional that AB and AD don't have to have the same element type?

"Diagnal of the inverse of the mass matrix"
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Suggested change
"Diagnal of the inverse of the mass matrix"
"Diagonal of the inverse of the mass matrix"

M⁻¹::AM
B::AB
D::AD
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D::AD
D::AD
"Woodbury factorisation of M⁻¹ + B D transpose(B)"

factorization::F
end

function woodbury_factorize(A, B, D)
cholA = cholesky(A isa Diagonal ? A : Symmetric(A))
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Pathfinder's implementation allows for arbitrary PD A but for the use-cases in Pathfinder and Bales's paper, diagonal A is sufficient. Since you've already documented A as diagonal, perhaps you can drop this check.

U = cholA.U
Q, R = qr(U' \ B)
V = cholesky(Symmetric(muladd(R, D * R', I))).U
return (U=U, Q=Q, V=V)
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Suggested change
return (U=U, Q=Q, V=V)
return (; U, Q, V)

end

function RankUpdateEuclideanMetric(n::Int)
M⁻¹ = Diagonal(ones(n))
B = zeros(n, 0)
D = zeros(0, 0)
factorization = woodbury_factorize(M⁻¹, B, D)
return RankUpdateEuclideanMetric(M⁻¹, B, D, factorization)
end
Comment on lines +146 to +152
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Note: this is probably fine for now, but there are multiple ways to form the identity matrix here, and later it might be better to initialize a different way (e.g. for tuning a covariance matrix for factor analysis, B=0 and D=0 prohibits convergence)

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I know it breaks with the API of other metric constructors, but I think you want to be able to initialize the rank of the update as well. Otherwise you have no way to fix the rank for future tuning algorithms.

function RankUpdateEuclideanMetric(::Type{T}, n::Int) where {T}
M⁻¹ = Diagonal(ones(T, n))
B = Matrix{T}(undef, n, 0)
D = Matrix{T}(undef, 0, 0)
factorization = woodbury_factorize(M⁻¹, B, D)
return RankUpdateEuclideanMetric(M⁻¹, B, D, factorization)
end

function RankUpdateEuclideanMetric(M⁻¹, B, D)
factorization = woodbury_factorize(M⁻¹, B, D)
return RankUpdateEuclideanMetric(M⁻¹, B, D, factorization)
end

function RankUpdateEuclideanMetric(::Type{T}, sz::Tuple{Int}) where {T}
return RankUpdateEuclideanMetric(T, first(sz))
end
RankUpdateEuclideanMetric(sz::Tuple{Int}) = RankUpdateEuclideanMetric(Float64, sz)

renew(::RankUpdateEuclideanMetric, (M⁻¹, B, D)) = RankUpdateEuclideanMetric(M⁻¹, B, D)

Base.size(metric::RankUpdateEuclideanMetric, dim...) = size(metric.M⁻¹.diag, dim...)

function Base.show(io::IO, ::MIME"text/plain", metric::RankUpdateEuclideanMetric)
return print(io, "RankUpdateEuclideanMetric(diag=$(diag(metric.M⁻¹)))")
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Here's another example where calling the full-rank part of the inverse-metric M⁻¹ leads to a different diagonal being shown than the diagonal of the full inverse-metric. The diagonal entries needed can be efficiently computed, see https://github.com/mlcolab/Pathfinder.jl/blob/f4ca90dc3d91f077f479d13904a2b6bf99e8ee25/src/woodbury.jl#L326-L329

end

# `rand` functions for `metric` types.

function rand_momentum(
Expand Down Expand Up @@ -131,3 +209,19 @@ function rand_momentum(
ldiv!(metric.cholM⁻¹, r)
return r
end

function rand_momentum(
rng::Union{AbstractRNG,AbstractVector{<:AbstractRNG}},
metric::RankUpdateEuclideanMetric{T},
kinetic::GaussianKinetic,
::AbstractVecOrMat,
) where {T}
M⁻¹ = metric.M⁻¹
r = _randn(rng, T, size(M⁻¹.diag)...)
F = metric.factorization
k = min(size(F.U, 1), size(F.V, 1))
@views ldiv!(F.V, r isa AbstractVector ? r[1:k] : r[1:k, :])
lmul!(F.Q, r)
ldiv!(F.U, r)
return r
end
9 changes: 7 additions & 2 deletions test/metric.jl
Original file line number Diff line number Diff line change
Expand Up @@ -10,6 +10,7 @@ using ReTest, Random, AdvancedHMC
UnitEuclideanMetric((D, n_chains)),
DiagEuclideanMetric((D, n_chains)),
# DenseEuclideanMetric((D, n_chains)) # not supported ATM
# RankUpdateEuclideanMetric((D, n_chains)) # not supported ATM
]
r = AdvancedHMC.rand_momentum(rng, metric, GaussianKinetic(), θ)
all_same = true
Expand All @@ -25,8 +26,12 @@ using ReTest, Random, AdvancedHMC
rng = MersenneTwister(1)
θ = randn(rng, D)
ℓπ(θ) = 1
for metric in
[UnitEuclideanMetric(1), DiagEuclideanMetric(1), DenseEuclideanMetric(1)]
for metric in [
UnitEuclideanMetric(1),
DiagEuclideanMetric(1),
DenseEuclideanMetric(1),
RankUpdateEuclideanMetric(1),
]
h = Hamiltonian(metric, ℓπ, ℓπ)
h = AdvancedHMC.resize(h, θ)
@test size(h.metric) == size(θ)
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6 changes: 6 additions & 0 deletions test/sampler.jl
Original file line number Diff line number Diff line change
Expand Up @@ -62,6 +62,7 @@ end
:UnitEuclideanMetric => UnitEuclideanMetric(D),
:DiagEuclideanMetric => DiagEuclideanMetric(D),
:DenseEuclideanMetric => DenseEuclideanMetric(D),
:RankUpdateEuclideanMetric => RankUpdateEuclideanMetric(D),
)
h = Hamiltonian(metric, ℓπ, ∂ℓπ∂θ)
@testset "$lfsym" for (lfsym, lf) in Dict(
Expand Down Expand Up @@ -104,6 +105,11 @@ end
@test mean(samples) ≈ zeros(D) atol = RNDATOL
end

if metricsym == :RankUpdateEuclideanMetric
# Skip tests with `RankUpdateEuclideanMetric` for `MassMatrixAdaptor`
continue
end

@testset "$adaptorsym" for (adaptorsym, adaptor) in Dict(
:MassMatrixAdaptorOnly => MassMatrixAdaptor(metric),
:StepSizeAdaptorOnly => StepSizeAdaptor(0.8, τ.integrator),
Expand Down
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