Generalized Grassmann
Manifolds.GeneralizedGrassmann
β TypeGeneralizedGrassmann{T,π½,TB<:AbstractMatrix} <: AbstractDecoratorManifold{π½}
The generalized Grassmann manifold $\operatorname{Gr}(n,k,B)$ consists of all subspaces spanned by $k$ linear independent vectors $π½^n$, where $π½ β \{β, β\}$ is either the real- (or complex-) valued vectors. This yields all $k$-dimensional subspaces of $β^n$ for the real-valued case and all $2k$-dimensional subspaces of $β^n$ for the second.
The manifold can be represented as
\[\operatorname{Gr}(n, k, B) := \bigl\{ \operatorname{span}(p)\ \big|\ p β π½^{nΓk}, p^\mathrm{H}Bp = I_k\},\]
where $β
^{\mathrm{H}}$ denotes the complex conjugate (or Hermitian) transpose and $I_k$ is the $kΓk$ identity matrix. This means, that the columns of $p$ form an unitary basis of the subspace with respect to the scaled inner product, that is a point on $\operatorname{Gr}(n,k,B)$, and hence the subspace can actually be represented by a whole equivalence class of representers. For $B=I_n$ this simplifies to the Grassmann
manifold.
The tangent space at a point (subspace) $p$ is given by
\[T_x\mathrm{Gr}(n,k,B) = \bigl\{ X β π½^{nΓk} : X^{\mathrm{H}}Bp + p^{\mathrm{H}}BX = 0_{k} \bigr\},\]
where $0_{k}$ denotes the $kΓk$ zero matrix.
Note that a point $p β \operatorname{Gr}(n,k,B)$ might be represented by different matrices (i.e. matrices with $B$-unitary column vectors that span the same subspace). Different representations of $p$ also lead to different representation matrices for the tangent space $T_p\mathrm{Gr}(n,k,B)$
The manifold is named after Hermann G. GraΓmann (1809-1877).
Constructor
GeneralizedGrassmann(n, k, B=I_n, field=β)
Generate the (real-valued) Generalized Grassmann manifold of $nΓk$ dimensional orthonormal matrices with scalar product B
.
Base.exp
β Methodexp(M::GeneralizedGrassmann, p, X)
Compute the exponential map on the GeneralizedGrassmann
M
$= \mathrm{Gr}(n,k,B)$ starting in p
with tangent vector (direction) X
. Let $X^{\mathrm{H}}BX = USV$ denote the SVD decomposition of $X^{\mathrm{H}}BX$. Then the exponential map is written using
\[\exp_p X = p V\cos(S)V^\mathrm{H} + U\sin(S)V^\mathrm{H},\]
where $β ^{\mathrm{H}}$ denotes the complex conjugate transposed or Hermitian and the cosine and sine are applied element wise to the diagonal entries of $S$.
Base.log
β Methodlog(M::GeneralizedGrassmann, p, q)
Compute the logarithmic map on the GeneralizedGrassmann
M
$= \mathcal M=\mathrm{Gr}(n,k,B)$, i.e. the tangent vector X
whose corresponding geodesic
starting from p
reaches q
after time 1 on M
. The formula reads
\[\log_p q = Vβ \operatorname{atan}(S) β U^\mathrm{H},\]
where $β ^{\mathrm{H}}$ denotes the complex conjugate transposed or Hermitian. The matrices $U$ and $V$ are the unitary matrices, and $S$ is the diagonal matrix containing the singular values of the SVD-decomposition
\[USV = (q^\mathrm{H}Bp)^{-1} ( q^\mathrm{H} - q^\mathrm{H}Bpp^\mathrm{H}).\]
In this formula the $\operatorname{atan}$ is meant elementwise.
Base.rand
β Methodrand(::GeneralizedGrassmann; vector_at=nothing, Ο::Real=1.0)
When vector_at
is nothing
, return a random (Gaussian) point p
on the GeneralizedGrassmann
manifold M
by generating a (Gaussian) matrix with standard deviation Ο
and return the (generalized) orthogonalized version, i.e. return the projection onto the manifold of the Q component of the QR decomposition of the random matrix of size $nΓk$.
When vector_at
is not nothing
, return a (Gaussian) random vector from the tangent space $T_{vector\_at}\mathrm{St}(n,k)$ with mean zero and standard deviation Ο
by projecting a random Matrix onto the tangent vector at vector_at
.
ManifoldsBase.change_metric
β Methodchange_metric(M::GeneralizedGrassmann, ::EuclideanMetric, p X)
Change X
to the corresponding vector with respect to the metric of the GeneralizedGrassmann
M
, i.e. let $B=LL'$ be the Cholesky decomposition of the matrix M.B
, then the corresponding vector is $L\X$.
ManifoldsBase.change_representer
β Methodchange_representer(M::GeneralizedGrassmann, ::EuclideanMetric, p, X)
Change X
to the corresponding representer of a cotangent vector at p
with respect to the scaled metric of the GeneralizedGrassmann
M
, i.e, since
\[g_p(X,Y) = \operatorname{tr}(Y^{\mathrm{H}}BZ) = \operatorname{tr}(X^{\mathrm{H}}Z) = β¨X,Zβ©\]
has to hold for all $Z$, where the repreenter X
is given, the resulting representer with respect to the metric on the GeneralizedGrassmann
is given by $Y = B^{-1}X$.
ManifoldsBase.check_point
β Methodcheck_point(M::GeneralizedGrassmann, p)
Check whether p
is representing a point on the GeneralizedGrassmann
M
, i.e. its a n
-by-k
matrix of unitary column vectors with respect to the B inner product and of correct eltype
with respect to π½
.
ManifoldsBase.check_vector
β Methodcheck_vector(M::GeneralizedGrassmann, p, X; kwargs...)
Check whether X
is a tangent vector in the tangent space of p
on the GeneralizedGrassmann
M
, i.e. that X
is of size and type as well as that
\[ p^{\mathrm{H}}BX + \overline{X^{\mathrm{H}}Bp} = 0_k,\]
where $β ^{\mathrm{H}}$ denotes the complex conjugate transpose or Hermitian, $\overline{β }$ the (elementwise) complex conjugate, and $0_k$ denotes the $kΓk$ zero natrix.
ManifoldsBase.distance
β Methoddistance(M::GeneralizedGrassmann, p, q)
Compute the Riemannian distance on GeneralizedGrassmann
manifold M
$= \mathrm{Gr}(n,k,B)$.
The distance is given by
\[d_{\mathrm{Gr}(n,k,B)}(p,q) = \operatorname{norm}(\log_p(q)).\]
ManifoldsBase.injectivity_radius
β Methodinjectivity_radius(M::GeneralizedGrassmann)
injectivity_radius(M::GeneralizedGrassmann, p)
Return the injectivity radius on the GeneralizedGrassmann
M
, which is $\frac{Ο}{2}$.
ManifoldsBase.inner
β Methodinner(M::GeneralizedGrassmann, p, X, Y)
Compute the inner product for two tangent vectors X
, Y
from the tangent space of p
on the GeneralizedGrassmann
manifold M
. The formula reads
\[g_p(X,Y) = \operatorname{tr}(X^{\mathrm{H}}BY),\]
where $β ^{\mathrm{H}}$ denotes the complex conjugate transposed or Hermitian.
ManifoldsBase.is_flat
β Methodis_flat(M::GeneralizedGrassmann)
Return true if GeneralizedGrassmann
M
is one-dimensional.
ManifoldsBase.manifold_dimension
β Methodmanifold_dimension(M::GeneralizedGrassmann)
Return the dimension of the GeneralizedGrassmann(n,k,π½)
manifold M
, i.e.
\[\dim \operatorname{Gr}(n,k,B) = k(n-k) \dim_β π½,\]
where $\dim_β π½$ is the real_dimension
of π½
.
ManifoldsBase.project
β Methodproject(M::GeneralizedGrassmann, p, X)
Project the n
-by-k
X
onto the tangent space of p
on the GeneralizedGrassmann
M
, which is computed by
\[\operatorname{proj_p}(X) = X - pp^{\mathrm{H}}B^\mathrm{T}X,\]
where $β ^{\mathrm{H}}$ denotes the complex conjugate transposed or Hermitian and $β ^{\mathrm{T}}$ the transpose.
ManifoldsBase.project
β Methodproject(M::GeneralizedGrassmann, p)
Project p
from the embedding onto the GeneralizedGrassmann
M
, i.e. compute q
as the polar decomposition of $p$ such that $q^{\mathrm{H}}Bq$ is the identity, where $β
^{\mathrm{H}}$ denotes the Hermitian, i.e. complex conjugate transpose.
ManifoldsBase.representation_size
β Methodrepresentation_size(M::GeneralizedGrassmann)
Return the representation size or matrix dimension of a point on the GeneralizedGrassmann
M
, i.e. $(n,k)$ for both the real-valued and the complex value case.
ManifoldsBase.retract
β Methodretract(M::GeneralizedGrassmann, p, X, ::PolarRetraction)
Compute the SVD-based retraction PolarRetraction
on the GeneralizedGrassmann
M
, by project
ing $p + X$ onto M
.
ManifoldsBase.zero_vector
β Methodzero_vector(M::GeneralizedGrassmann, p)
Return the zero tangent vector from the tangent space at p
on the GeneralizedGrassmann
M
, which is given by a zero matrix the same size as p
.
Statistics.mean
β Methodmean(
M::GeneralizedGrassmann,
x::AbstractVector,
[w::AbstractWeights,]
method = GeodesicInterpolationWithinRadius(Ο/4);
kwargs...,
)
Compute the Riemannian mean
of x
using GeodesicInterpolationWithinRadius
.