Different library functions
Documentation for ManifoldDiff.jl
's methods and types for finite differences and automatic differentiation.
Derivatives
ManifoldDiff.geodesic_derivative
— MethodY = geodesic_derivative(M, p, X, t::Number; γt = geodesic(M, p, X, t))
geodesic_derivative!(M, Y, p, X, t::Number; γt = geodesic(M, p, X, t))
Evaluate the derivative of the geodesic $γ(t)$ with $γ_{p,X}(0) = p$ and $\dot γ_{p,X}(0) = X$ at $t$. The formula reads
\[\dot γ(t) = \mathcal P_{γ(t) \gets p} X\]
where $\mathcal P$ denotes the parallel transport. This computation can also be done in-place of $Y$.
Optional Parameters
γt
– (geodesic(M, p, X, t)
) the point on the geodesic at $t$. This way if the point was computed earlier it can be resued here.
ManifoldDiff.shortest_geodesic_derivative
— MethodY = shortest_geodesic_derivative(M, p, X, t::Number; γt = shortest_geodesic(M, p, q, t))
shortest_geodesic_derivative!(M, Y, p, X, t::Number; γt = shortest_geodesic(M, p, q, t))
Evaluate the derivative of the shortest geodesic $γ(t)$ with $γ_{p,q}(0) = p$ and $\dot γ_{p,q}(1) = q$ at $t$. The formula reads
\[\dot γ(t) = \mathcal P_{γ(t) \gets p} \log_pq\]
where $\mathcal P$ denotes the parallel transport. This computation can also be done in-place of $Y$.
Optional Parameters
γt = geodesic(M, p, X, t)
the point on the geodesic at $t$. This way if the point was computed earlier it can be resued here.
Differentials and their adjoints
ManifoldDiff.adjoint_differential_exp_argument
— Methodadjoint_differential_exp_argument(M, p, X, Y)
adjoint_differential_exp_argument!(M, Z, p, X, Y)
Compute the adjoint of $D_X\exp_p X[Y]$ (in place of Z
). Note that $X ∈ T_p(T_p\mathcal M) = T_p\mathcal M$ is still a tangent vector.
See also
ManifoldDiff.adjoint_differential_exp_basepoint
— Methodadjoint_differential_exp_basepoint(M, p, X, Y)
adjoint_differential_exp_basepoint!(M, Z, p, X, Y)
Computes the adjoint of $D_p \exp_p X[Y]$ (in place of Z
).
See also
ManifoldDiff.adjoint_differential_log_argument
— Methodadjoint_differential_log_argument(M, p, q, X)
adjoint_differential_log_argument!(M, Y, p, q, X)
Compute the adjoint of $D_q log_p q[X]$ (in place of Y
).
See also
ManifoldDiff.adjoint_differential_log_basepoint
— Methodadjoint_differential_log_basepoint(M, p, q, X)
adjoint_differential_log_basepoint!(M, Y, p, q, X)
computes the adjoint of $D_p log_p q[X]$ (in place of Y
).
See also
ManifoldDiff.adjoint_differential_shortest_geodesic_endpoint
— Methodadjoint_differential_shortest_geodesic_endpoint(M, p, q, t, X)
adjoint_differential_shortest_geodesic_endpoint!(M, Y, p, q, t, X)
Compute the adjoint of $D_q γ(t; p, q)[X]$ (in place of Y
).
See also
differential_shortest_geodesic_endpoint
, adjoint_Jacobi_field
ManifoldDiff.adjoint_differential_shortest_geodesic_startpoint
— Methodadjoint_differential_shortest_geodesic_startpoint(M, p, q, t, X)
adjoint_differential_shortest_geodesic_startpoint!(M, Y, p, q, t, X)
Compute the adjoint of $D_p γ(t; p, q)[X]$ (in place of Y
).
See also
differential_shortest_geodesic_startpoint
, adjoint_Jacobi_field
ManifoldDiff.differential_exp_argument
— MethodZ = differential_exp_argument(M, p, X, Y)
differential_exp_argument!(M, Z, p, X, Y)
Compute $D_X\exp_pX[Y]$ (in place of Z
). Note that $X ∈ T_X(T_p\mathcal M) = T_p\mathcal M$ is still a tangent vector.
See also
ManifoldDiff.differential_exp_argument_lie_approx
— Methoddifferential_exp_argument_lie_approx(M::AbstractManifold, p, X, Y; n)
Approximate differential of exponential map based on Lie group exponential. The formula reads (see Theorem 1.7 of [Helgason1978])
\[D_X \exp_{p}(X)[Y] = (\mathrm{d}L_{\exp_e(X)})_e\left(\sum_{k=0}^{n}\frac{(-1)^k}{(k+1)!}(\operatorname{ad}_X)^k(Y)\right)\]
where $(\operatorname{ad}_X)^k(Y)$ is defined recursively as $(\operatorname{ad}_X)^0(Y) = Y$, $\operatorname{ad}_X^{k+1}(Y) = [X, \operatorname{ad}_X^k(Y)]$.
ManifoldDiff.differential_exp_basepoint
— MethodZ = differential_exp_basepoint(M, p, X, Y)
differential_exp_basepoint!(M, Z, p, X, Y)
Compute $D_p\exp_p X[Y]$ (in place of Z
).
See also
ManifoldDiff.differential_inverse_retract_argument_fd_approx
— Methoddifferential_inverse_retract_argument_fd_approx(
M::AbstractManifold,
p,
q,
X;
retr::AbstractRetractionMethod = default_retraction_method(M),
invretr::AbstractInverseRetractionMethod = default_inverse_retraction_method(M),
h::Real=sqrt(eps(eltype(X))),
)
Approximate the differential of the inverse retraction invretr
using a finite difference formula (see Eq. (16) in [Zim20]
\[\frac{\operatorname{retr}^{-1}_q(\operatorname{retr}_p(hX)) - \operatorname{retr}^{-1}_q(\operatorname{retr}_p(-hX))}{2h}\]
where $h$ is the finite difference step h
, $\operatorname{retr}^{-1}$ is the inverse retraction invretr
and $\operatorname{retr}$ is the retraction retr
.
ManifoldDiff.differential_log_argument
— MethodY = differential_log_argument(M, p, q, X)
differential_log_argument!(M, Y, p, q, X)
computes $D_q\log_pq[X]$ (in place of Y
).
See also
ManifoldDiff.differential_log_basepoint
— MethodY = differential_log_basepoint(M, p, q, X)
differential_log_basepoint!(M, Y, p, q, X)
computes $D_p\log_pq[X]$ (in place of Y
).
See also
ManifoldDiff.differential_shortest_geodesic_endpoint
— MethodY = differential_shortest_geodesic_endpoint(M, p, q, t, X)
differential_shortest_geodesic_endpoint!(M, Y, p, q, t, X)
Compute $D_qγ(t;p,q)[X]$ (in place of Y
).
See also
ManifoldDiff.differential_shortest_geodesic_startpoint
— MethodY = differential_shortest_geodesic_startpoint(M, p, q, t, X)
differential_shortest_geodesic_startpoint!(M, Y, p, q, t, X)
Compute $D_p γ(t;p,q)[η]$ (in place of Y
).
See also
ManifoldDiff.AbstractProjector
— Typeabstract type AbstractProjector end
An abstract type for projectors on a tangent space $T_pM$ for fixed values of p
and M
. Calling a projector on a tangent vector returns a new tangent vector:
(Π::AbstractProjector)(X) -> Y
Projectors assume that X
is a valid vector from $T_pM$.
ManifoldDiff.CoprojectorOntoVector
— TypeCoprojectorOntoVector{TM<:AbstractManifold,TP,TX}
A structure that represents projector onto the subspace of the tangent space at p
from manifold M
othogonal to vector X
of unit norm.
Constructor
CoprojectorOntoVector(M::AbstractManifold, p, X)
ManifoldDiff.ProjectorOntoVector
— TypeProjectorOntoVector{TM<:AbstractManifold,TP,TX}
A structure that represents projector onto the subspace of the tangent space at p
from manifold M
spanned by tangent vector X
of unit norm.
Constructor
ProjectorOntoVector(M::AbstractManifold, p, X)
ManifoldDiff.diagonalizing_projectors
— Methoddiagonalizing_projectors(M::AbstractManifold, p, X)
Compute eigenvalues of the Jacobi operator $Y → R(Y,X)X$, where $R$ is the curvature endomorphism, together with projectors onto eigenspaces of the operator. Projectors are objects of subtypes of AbstractProjector
.
By default constructs projectors using the DiagonalizingOrthonormalBasis
.
Gradients
ManifoldDiff.grad_distance
— Functiongrad_distance(M, q, p[, c=2])
grad_distance!(M, X, q, p[, c=2])
compute the (sub)gradient of the distance (default: squared), in place of X
.
\[f(p) = \frac{1}{c} d^c_{\mathcal M}(p, q)\]
to a fixed point q
on the manifold M
and c
is an integer. The (sub-)gradient reads
\[\operatorname{grad}f(p) = -d_{\mathcal M}^{c-2}(p, q)\log_pq\]
for $c\neq 1$ or $p\neq q$. Note that for the remaining case $c=1$, $p=q$, the function is not differentiable. In this case, the function returns the corresponding zero tangent vector, since this is an element of the subdifferential.
Optional
c
– (2
) the exponent of the distance, i.e. the default is the squared distance
ManifoldDiff.subgrad_distance
— Functionsubgrad_distance(M, q, p[, c = 2; atol = 0])
subgrad_distance!(M, X, q, p[, c = 2; atol = 0])
compute the subgradient of the distance (in place of X
)
\[f(p) = \frac{1}{c} d^c_{\mathcal M}(p, q)\]
to a fixed point q
on the manifold M
and c
is an integer. The subgradient reads
\[\partial f(p) = -d_{\mathcal M}^{c-2}(p, q)\log_pq\]
for $c\neq 1$ or $p\neq q$. Note that for the remaining case $c=1$, $p=q$, the function is not differentiable. In this case, the subgradient is given by a tangent vector at p
with norm less than or equal to one.
Optional
c
– (2
) the exponent of the distance, i.e. the default is the distanceatol
– (0
) the tolerance to use when evaluating the distance betweenp
andq
.
Jacobi fields
ManifoldDiff.adjoint_Jacobi_field
— MethodY = adjoint_Jacobi_field(M, p, q, t, X, β)
adjoint_Jacobi_field!(M, Y, p, q, t, X, β)
Compute the AdjointJacobiField $J$ along the geodesic $γ_{p,q}$ on the manifold $\mathcal M$ with initial conditions (depending on the application) $X ∈ T_{γ_{p,q}(t)}\mathcal M$ and weights $β$. The result is a vector $Y ∈ T_p\mathcal M$. The main difference to jacobi_field
is the, that the input X
and the output Y
switched tangent spaces. The computation can be done in place of Y
.
For details see jacobi_field
ManifoldDiff.jacobi_field
— MethodY = jacobi_field(M, p, q, t, X, β)
jacobi_field!(M, Y, p, q, t, X, β)
compute the Jacobi field $J$ along the geodesic $γ_{p,q}$ on the manifold $\mathcal M$ with initial conditions (depending on the application) $X ∈ T_p\mathcal M$ and weights $β$. The result is a tangent vector Y
from $T_{γ_{p,q}(t)}\mathcal M$. The computation can be done in place of Y
.
See also
ManifoldDiff.βdifferential_exp_argument
— Methodβdifferential_exp_argument(κ,t,d)
weights for the jacobi_field
corresponding to the differential of the geodesic with respect to its start point $D_X \exp_p X[Y]$. They are
\[β(κ) = \begin{cases} \frac{\sinh(d\sqrt{-κ})}{d\sqrt{-κ}}&\text{ if }κ < 0,\\ 1 & \text{ if } κ = 0,\\ \frac{\sin(d\sqrt{κ})}{d\sqrt{κ}}&\text{ if }κ > 0. \end{cases}\]
See also
ManifoldDiff.βdifferential_exp_basepoint
— Methodβdifferential_exp_basepoint(κ,t,d)
weights for the jacobi_field
corresponding to the differential of the geodesic with respect to its start point $D_p \exp_p X [Y]$. They are
\[β(κ) = \begin{cases} \cosh(\sqrt{-κ})&\text{ if }κ < 0,\\ 1 & \text{ if } κ = 0,\\ \cos(\sqrt{κ}) &\text{ if }κ > 0. \end{cases}\]
See also
ManifoldDiff.βdifferential_log_argument
— Methodβdifferential_log_argument(κ,t,d)
weights for the JacobiField corresponding to the differential of the logarithmic map with respect to its argument $D_q \log_p q[X]$. They are
\[β(κ) = \begin{cases} \frac{ d\sqrt{-κ} }{\sinh(d\sqrt{-κ})}&\text{ if }κ < 0,\\ 1 & \text{ if } κ = 0,\\ \frac{ d\sqrt{κ} }{\sin(d\sqrt{κ})}&\text{ if }κ > 0. \end{cases}\]
See also
ManifoldDiff.βdifferential_log_basepoint
— Methodβdifferential_log_basepoint(κ,t,d)
weights for the jacobi_field
corresponding to the differential of the geodesic with respect to its start point $D_p \log_p q[X]$. They are
\[β(κ) = \begin{cases} -\sqrt{-κ}d\frac{\cosh(d\sqrt{-κ})}{\sinh(d\sqrt{-κ})}&\text{ if }κ < 0,\\ -1 & \text{ if } κ = 0,\\ -\sqrt{κ}d\frac{\cos(d\sqrt{κ})}{\sin(d\sqrt{κ})}&\text{ if }κ > 0. \end{cases}\]
See also
differential_log_argument
, differential_log_argument
, jacobi_field
ManifoldDiff.βdifferential_shortest_geodesic_startpoint
— Methodβdifferential_shortest_geodesic_startpoint(κ,t,d)
weights for the jacobi_field
corresponding to the differential of the geodesic with respect to its start point $D_x g(t;p,q)[X]$. They are
\[β(κ) = \begin{cases} \frac{\sinh(d(1-t)\sqrt{-κ})}{\sinh(d\sqrt{-κ})} &\text{ if }κ < 0,\\ 1-t & \text{ if } κ = 0,\\ \frac{\sin((1-t)d\sqrt{κ})}{\sinh(d\sqrt{κ})} &\text{ if }κ > 0. \end{cases}\]
Due to a symmetry argument, these are also used to compute $D_q g(t; p,q)[η]$
See also
differential_shortest_geodesic_endpoint
, differential_shortest_geodesic_startpoint
, jacobi_field
Jacobians
ManifoldDiff.allocate_jacobian
— Methodallocate_jacobian(
M_domain::AbstractManifold,
M_codomain::AbstractManifold,
f,
p;
basis_domain::AbstractBasis = DefaultOrthonormalBasis(),
basis_codomain::AbstractBasis = DefaultOrthonormalBasis(),
)
Allocate Jacobian of function f
with given domain and codomain at point p
. basis_domain
and basis_codomain
denote bases of tangent spaces at, respectively, p
and f(p)
.
ManifoldDiff.jacobian_exp_argument
— Functionjacobian_exp_argument(
M::AbstractManifold,
p,
X,
basis_domain::AbstractBasis=DefaultOrthonormalBasis(),
basis_codomain::AbstractBasis=DefaultOrthonormalBasis(),
)
Compute Jacobian of the exponential map with respect to its argument (tangent vector). Differential of the exponential map is here considered as a function from $T_p \mathcal{M}$ to $T_{\exp_p X} \mathcal{M}$. Jacobian coefficients are represented in basis basis_domain
in the domain and in basis_codomain
in the codomain.
ManifoldDiff.jacobian_exp_basepoint
— Functionjacobian_exp_basepoint(
M::AbstractManifold,
p,
X,
basis_domain::AbstractBasis=DefaultOrthonormalBasis(),
basis_codomain::AbstractBasis=DefaultOrthonormalBasis(),
)
Compute Jacobian of the exponential map with respect to the basepoint. Differential of the exponential map is here considered as a function from $T_p \mathcal{M}$ to $T_{\exp_p X} \mathcal{M}$. Jacobian coefficients are represented in basis basis_domain
in the domain and in basis_codomain
in the codomain.
ManifoldDiff.jacobian_log_argument
— Functionjacobian_log_argument(
M::AbstractManifold,
p,
q,
basis_domain::AbstractBasis=DefaultOrthonormalBasis(),
basis_codomain::AbstractBasis=DefaultOrthonormalBasis(),
)
Compute Jacobian of the logarithmic map with respect to its argument (point q
). Differential of the logarithmic map is here considered as a function from $T_q \mathcal{M}$ to $T_p \mathcal{M}$. Jacobian coefficients are represented in basis basis_domain
in the domain and in basis_codomain
in the codomain.
ManifoldDiff.jacobian_log_basepoint
— Functionjacobian_log_basepoint(
M::AbstractManifold,
p,
q,
basis_domain::AbstractBasis=DefaultOrthonormalBasis(),
basis_codomain::AbstractBasis=DefaultOrthonormalBasis(),
)
Compute Jacobian of the logarithmic map with respect to the basepoint. Differential of the logarithmic map is here considered as a function from $T_q \mathcal{M}$ to $T_p \mathcal{M}$. Jacobian coefficients are represented in basis basis_domain
in the domain and in basis_codomain
in the codomain.
Riemannian differentials
ManifoldDiff.AbstractRiemannianDiffBackend
— TypeAbstractRiemannianDiffBackend
An abstract type for backends for differentiation.
ManifoldDiff.RiemannianProjectionBackend
— TypeRiemannianProjectionBackend <: AbstractRiemannianDiffBackend
This backend computes the differentiation in the embedding, which is currently limited to the gradient. Let $mathcal M$ denote a manifold embedded in some $R^m$, where $m$ is usually (much) larger than the manifold dimension. Then we require three tools
- A function $f̃: ℝ^m → ℝ$ such that its restriction to the manifold yields the cost function $f$ of interest.
- A
project
function to project tangent vectors from the embedding (at $T_pℝ^m$) back onto the tangent space $T_p\mathcal M$. This also includes possible changes of the representation of the tangent vector (e.g. in the Lie algebra or in a different data format). - A
change_representer
for non-isometrically embedded manifolds, i.e. where the tangent space $T_p\mathcal M$ of the manifold does not inherit the inner product from restriction of the inner product from the tangent space $T_pℝ^m$ of the embedding
see also riemannian_gradient
and [AMS08], Section 3.6.1 for a derivation on submanifolds.
ManifoldDiff.TangentDiffBackend
— TypeTangentDiffBackend <: AbstractRiemannianDiffBackend
A backend that uses tangent spaces and bases therein to derive an intrinsic differentiation scheme.
Since it works in tangent spaces at argument and function value, methods might require a retraction and an inverse retraction as well as a basis.
In the tangent space itself, this backend then employs an (Euclidean) AbstractDiffBackend
Constructor
TangentDiffBackend(diff_backend)
where diff_backend
is an AbstractDiffBackend
to be used on the tangent space.
With the keyword arguments
retraction
an AbstractRetractionMethod (ExponentialRetraction
by default)inverse_retraction
an AbstractInverseRetractionMethodLogarithmicInverseRetraction
by default)basis_arg
an AbstractBasis (DefaultOrthogonalBasis
by default)basis_val
an AbstractBasis (DefaultOrthogonalBasis
by default)
ManifoldDiff.differential
— Methoddifferential(M::AbstractManifold, f, t::Real, backend::AbstractDiffBackend)
differential!(M::AbstractManifold, f, X, t::Real, backend::AbstractDiffBackend)
Compute the Riemannian differential of a curve $f: ℝ\to M$ on a manifold M
represented by function f
at time t
using the given backend. It is calculated as the tangent vector equal to $\mathrm{d}f_t(t)[1]$.
The mutating variant computes the differential in place of X
.
ManifoldDiff.gradient
— Methodgradient(M::AbstractManifold, f, p, backend::AbstractRiemannianDiffBackend)
gradient!(M::AbstractManifold, f, X, p, backend::AbstractRiemannianDiffBackend)
Compute the Riemannian gradient $∇f(p)$ of a real-valued function $f:\mathcal M \to ℝ$ at point p
on the manifold M
using the specified AbstractRiemannianDiffBackend
.
The mutating variant computes the gradient in place of X
.
ManifoldDiff.gradient
— Methodgradient(M, f, p, backend::TangentDiffBackend)
This method uses the internal backend.diff_backend
(Euclidean) on the function
\[ f(\operatorname{retr}_p(\cdot))\]
which is given on the tangent space. In detail, the gradient can be written in terms of the backend.basis_arg
. We illustrate it here for an AbstractOrthonormalBasis, since that simplifies notations:
\[\operatorname{grad}f(p) = \operatorname{grad}f(p) = \sum_{i=1}^{d} g_p(\operatorname{grad}f(p),X_i)X_i = \sum_{i=1}^{d} Df(p)[X_i]X_i\]
where the last equality is due to the definition of the gradient as the Riesz representer of the differential.
If the backend is a forward (or backward) finite difference, these coefficients in the sum can be approximates as
\[DF(p)[Y] ≈ \frac{1}{h}\bigl( f(\exp_p(hY)) - f(p) \bigr)\]
writing $p=\exp_p(0)$ we see that this is a finite difference of $f\circ\exp_p$, i.e. for a function on the tangent space, so we can also use other (Euclidean) backends
ManifoldDiff.hessian
— Methodhessian(M::AbstractManifold, f, p, backend::TangentDiffBackend)
Compute the Hessian of function f
at point p
using the given backend
. The formula for normal coordinate systems from[SommerFletcherPennec2020] is used.
ManifoldDiff.riemannian_Hessian
— Methodriemannian_Hessian(M, p, eG, eH, X)
riemannian_Hessian!(M, Y, p, eG, eH, X)
Convert the Euclidean Hessian eH=
$\operatorname{Hess} \tilde f(p) [X]$ of a function $f \colon \mathcal M \to \mathbb R$, which is the restriction of $\tilde f$ to $\mathcal M$, given additionally the (Euclidean) gradient $\operatorname{grad} \tilde f(p)$.
The Riemannian Hessian is then computed by
\[\operatorname{Hess} f(p)[X] = \operatorname{proj}_{T_p\mathcal M}\bigl(\operatorname{Hess} \tilde f(p)[X]) + \mathcal W_p\Bigl( X, \operatorname{proj}_{N_p\mathcal M}\bigl( \operatorname{grad} \tilde f (p) \bigr) \Bigr),\]
where $N_p\mathcal M$ denotes the normal space, i.e. the orthogonal complement of the tangent space in the embedding, and $\mathcal W_p$ denotes the Weingarten
map. See [Bou23] for more details
The function is inspired by ehess2rhess
in the Matlab package Manopt.
ManifoldDiff.riemannian_gradient
— Methodriemannian_gradient(M, p, Y; embedding_metric=EuclideanMetric())
riemannian_gradient!(M, X, p, Y; embedding_metric=EuclideanMetric())
For a given gradient $Y = \operatorname{grad} \tilde f(p)$ in the embedding of a manifold, this function computes the Riemannian gradient $\operatorname{grad} f(p)$ of the function $\tilde f$ restricted to the manifold $M$. This can also be done in place of X
.
By default it uses the following computation: Let the projection $Z = \operatorname{proj}_{T_p\mathcal M}(Y)$ of $Y$ onto the tangent space at $p$ be given, that is with respect to the inner product in the embedding. Then
\[⟨Z-Y, W⟩ = 0 \text{ for all } W \in T_p\mathcal M,\]
or rearranged $⟨Y,W⟩ = ⟨Z,W⟩$. We then use the definition of the Riemannian gradient
\[⟨\operatorname{grad} f(p), W⟩_p = Df(p)[X] = ⟨\operatorname{grad}f(p), W⟩ = ⟨\operatorname{proj}_{T_p\mathcal M}(\operatorname{grad}f(p)),W⟩ \quad\text{for all } W \in T_p\mathcal M.\]
Comparing the first and the last term, the remaining computation is the function change_representer
.
This method can also be implemented directly, if a more efficient/stable version is known.
The function is inspired by egrad2rgrad
in the Matlab package Manopt.
Proximal Maps
Given a convex, lower semi-continuous function $f\colon \mathcal M \to \mathbb R$, its proximal map is defined for some $λ>0$ as [Bac14]
\[\operatorname{prox}_{λf}(p) := \operatorname*{arg\,min}_{q\in\mathcal M} \frac{1}{2λ}d^2_{\mathcal M}(p,q) + f(q).\]
Another name for the proximal map is resolvent. Intuitively this means to minimize the function $f$ while at the same timme “staying close” to the argument $p$.
ManifoldDiff.prox_distance
— Functiony = prox_distance(M::AbstractManifold, λ::Real, p_data, p [, r=2])
prox_distance!(M::AbstractManifold, q, λ::Real, p_data, p [, r=2])
Compute the proximal map $\operatorname{prox}_{λf}$ with parameter λ of $f(p) = \frac{1}{r}d_{\mathcal M}^r(p_{\mathrm{data}},p)$. For the in-place variant the computation is done in place of q
.
Input
M
a manifoldM
λ
the prox parameter, a positive real number.p_data
a point onM
.p
the argument of the proximal mapr
(2
) exponent of the distance.
Output
q
– the result of the proximal map of $f$
For more details see [WDS14]
- Helgason1978
S. Helgason, Differential Geometry, Lie Groups, and Symmetric Spaces, First Edition. Academic Press, 1978.
- SommerFletcherPennec2020
S. Sommer, T. Fletcher, and X. Pennec, “1 - Introduction to differential and Riemannian geometry,” in Riemannian Geometric Statistics in Medical Image Analysis, X. Pennec, S. Sommer, and T. Fletcher, Eds. Academic Press, 2020, pp. 3–37. doi: 10.1016/B978-0-12-814725-2.00008-X.