
In
linear algebra
Linear algebra is the branch of mathematics concerning linear equations such as
:a_1x_1+\cdots +a_nx_n=b,
linear maps such as
:(x_1, \ldots, x_n) \mapsto a_1x_1+\cdots +a_nx_n,
and their representations in vector spaces and through matrix (mathemat ...
and
functional analysis
Functional analysis is a branch of mathematical analysis, the core of which is formed by the study of vector spaces endowed with some kind of limit-related structure (for example, Inner product space#Definition, inner product, Norm (mathematics ...
, a projection is a
linear transformation
In mathematics, and more specifically in linear algebra, a linear map (also called a linear mapping, linear transformation, vector space homomorphism, or in some contexts linear function) is a mapping V \to W between two vector spaces that pr ...
from a
vector space
In mathematics and physics, a vector space (also called a linear space) is a set (mathematics), set whose elements, often called vector (mathematics and physics), ''vectors'', can be added together and multiplied ("scaled") by numbers called sc ...
to itself (an
endomorphism) such that
. That is, whenever
is applied twice to any vector, it gives the same result as if it were applied once (i.e.
is
idempotent
Idempotence (, ) is the property of certain operations in mathematics and computer science whereby they can be applied multiple times without changing the result beyond the initial application. The concept of idempotence arises in a number of pl ...
). It leaves its
image
An image or picture is a visual representation. An image can be Two-dimensional space, two-dimensional, such as a drawing, painting, or photograph, or Three-dimensional space, three-dimensional, such as a carving or sculpture. Images may be di ...
unchanged. This definition of "projection" formalizes and generalizes the idea of
graphical projection. One can also consider the effect of a projection on a geometrical object by examining the effect of the projection on
points in the object.
Definitions
A projection on a vector space
is a linear operator
such that
.
When
has an
inner product
In mathematics, an inner product space (or, rarely, a Hausdorff pre-Hilbert space) is a real vector space or a complex vector space with an operation called an inner product. The inner product of two vectors in the space is a scalar, ofte ...
and is
complete, i.e. when
is a
Hilbert space
In mathematics, a Hilbert space is a real number, real or complex number, complex inner product space that is also a complete metric space with respect to the metric induced by the inner product. It generalizes the notion of Euclidean space. The ...
, the concept of
orthogonality
In mathematics, orthogonality is the generalization of the geometric notion of '' perpendicularity''. Although many authors use the two terms ''perpendicular'' and ''orthogonal'' interchangeably, the term ''perpendicular'' is more specifically ...
can be used. A projection
on a Hilbert space
is called an orthogonal projection if it satisfies
for all
. A projection on a Hilbert space that is not orthogonal is called an oblique projection.
Projection matrix
* A
square matrix is called a projection matrix if it is equal to its square, i.e. if
.
* A square matrix
is called an orthogonal projection matrix if
for a
real matrix
Matrix (: matrices or matrixes) or MATRIX may refer to:
Science and mathematics
* Matrix (mathematics), a rectangular array of numbers, symbols or expressions
* Matrix (logic), part of a formula in prenex normal form
* Matrix (biology), the m ...
, and respectively
for a
complex
Complex commonly refers to:
* Complexity, the behaviour of a system whose components interact in multiple ways so possible interactions are difficult to describe
** Complex system, a system composed of many components which may interact with each ...
matrix, where
denotes the
transpose
In linear algebra, the transpose of a Matrix (mathematics), matrix is an operator which flips a matrix over its diagonal;
that is, it switches the row and column indices of the matrix by producing another matrix, often denoted by (among other ...
of
and
denotes the adjoint or
Hermitian transpose of
.
* A projection matrix that is not an orthogonal projection matrix is called an oblique projection matrix.
The
eigenvalue
In linear algebra, an eigenvector ( ) or characteristic vector is a vector that has its direction unchanged (or reversed) by a given linear transformation. More precisely, an eigenvector \mathbf v of a linear transformation T is scaled by a ...
s of a projection matrix must be 0 or 1.
Examples
Orthogonal projection
For example, the function which maps the point
in three-dimensional space
to the point
is an orthogonal projection onto the ''xy''-plane. This function is represented by the matrix
The action of this matrix on an arbitrary
vector
Vector most often refers to:
* Euclidean vector, a quantity with a magnitude and a direction
* Disease vector, an agent that carries and transmits an infectious pathogen into another living organism
Vector may also refer to:
Mathematics a ...
is
To see that
is indeed a projection, i.e.,
, we compute
Observing that
shows that the projection is an orthogonal projection.
Oblique projection
A simple example of a non-orthogonal (oblique) projection is
Via
matrix multiplication
In mathematics, specifically in linear algebra, matrix multiplication is a binary operation that produces a matrix (mathematics), matrix from two matrices. For matrix multiplication, the number of columns in the first matrix must be equal to the n ...
, one sees that
showing that
is indeed a projection.
The projection
is orthogonal
if and only if
In logic and related fields such as mathematics and philosophy, "if and only if" (often shortened as "iff") is paraphrased by the biconditional, a logical connective between statements. The biconditional is true in two cases, where either bo ...
because only then
Properties and classification
Idempotence
By definition, a projection
is
idempotent
Idempotence (, ) is the property of certain operations in mathematics and computer science whereby they can be applied multiple times without changing the result beyond the initial application. The concept of idempotence arises in a number of pl ...
(i.e.
).
Open map
Every projection is an
open map
In mathematics, more specifically in topology, an open map is a function between two topological spaces that maps open sets to open sets.
That is, a function f : X \to Y is open if for any open set U in X, the image f(U) is open in Y.
Likewise, ...
onto its image, meaning that it maps each
open set
In mathematics, an open set is a generalization of an Interval (mathematics)#Definitions_and_terminology, open interval in the real line.
In a metric space (a Set (mathematics), set with a metric (mathematics), distance defined between every two ...
in the
domain to an open set in the
subspace topology
In topology and related areas of mathematics, a subspace of a topological space (''X'', ''𝜏'') is a subset ''S'' of ''X'' which is equipped with a topology induced from that of ''𝜏'' called the subspace topology (or the relative topology ...
of the
image
An image or picture is a visual representation. An image can be Two-dimensional space, two-dimensional, such as a drawing, painting, or photograph, or Three-dimensional space, three-dimensional, such as a carving or sculpture. Images may be di ...
. That is, for any vector
and any ball
(with positive radius) centered on
, there exists a ball
(with positive radius) centered on
that is wholly contained in the image
.
Complementarity of image and kernel
Let
be a finite-dimensional vector space and
be a projection on
. Suppose the
subspaces
and
are the
image
An image or picture is a visual representation. An image can be Two-dimensional space, two-dimensional, such as a drawing, painting, or photograph, or Three-dimensional space, three-dimensional, such as a carving or sculpture. Images may be di ...
and
kernel of
respectively. Then
has the following properties:
#
is the
identity operator on
:
# We have a
direct sum
The direct sum is an operation between structures in abstract algebra, a branch of mathematics. It is defined differently but analogously for different kinds of structures. As an example, the direct sum of two abelian groups A and B is anothe ...
. Every vector
may be decomposed uniquely as
with
and
, and where
The image and kernel of a projection are ''complementary'', as are
and
. The operator
is also a projection as the image and kernel of
become the kernel and image of
and vice versa. We say
is a projection along
onto
(kernel/image) and
is a projection along
onto
.
Spectrum
In infinite-dimensional vector spaces, the
spectrum
A spectrum (: spectra or spectrums) is a set of related ideas, objects, or properties whose features overlap such that they blend to form a continuum. The word ''spectrum'' was first used scientifically in optics to describe the rainbow of co ...
of a projection is contained in
as
Only 0 or 1 can be an
eigenvalue
In linear algebra, an eigenvector ( ) or characteristic vector is a vector that has its direction unchanged (or reversed) by a given linear transformation. More precisely, an eigenvector \mathbf v of a linear transformation T is scaled by a ...
of a projection. This implies that an orthogonal projection
is always a
positive semi-definite matrix. In general, the corresponding
eigenspace
In linear algebra, an eigenvector ( ) or characteristic vector is a Vector (mathematics and physics), vector that has its direction (geometry), direction unchanged (or reversed) by a given linear map, linear transformation. More precisely, an e ...
s are (respectively) the kernel and range of the projection. Decomposition of a vector space into direct sums is not unique. Therefore, given a subspace
, there may be many projections whose range (or kernel) is
.
If a projection is nontrivial it has
minimal polynomial , which factors into distinct linear factors, and thus
is
diagonalizable.
Product of projections
The product of projections is not in general a projection, even if they are orthogonal. If two projections
commute then their product is a projection, but the
converse is false: the product of two non-commuting projections may be a projection.
If two orthogonal projections commute then their product is an orthogonal projection. If the product of two orthogonal projections is an orthogonal projection, then the two orthogonal projections commute (more generally: two self-adjoint
endomorphisms commute if and only if their product is self-adjoint).
Orthogonal projections
When the vector space
has an
inner product
In mathematics, an inner product space (or, rarely, a Hausdorff pre-Hilbert space) is a real vector space or a complex vector space with an operation called an inner product. The inner product of two vectors in the space is a scalar, ofte ...
and is complete (is a
Hilbert space
In mathematics, a Hilbert space is a real number, real or complex number, complex inner product space that is also a complete metric space with respect to the metric induced by the inner product. It generalizes the notion of Euclidean space. The ...
) the concept of
orthogonality
In mathematics, orthogonality is the generalization of the geometric notion of '' perpendicularity''. Although many authors use the two terms ''perpendicular'' and ''orthogonal'' interchangeably, the term ''perpendicular'' is more specifically ...
can be used. An orthogonal projection is a projection for which the range
and the kernel
are
orthogonal subspaces. Thus, for every
and
in
,
. Equivalently:
A projection is orthogonal if and only if it is
self-adjoint
In mathematics, an element of a *-algebra is called self-adjoint if it is the same as its adjoint (i.e. a = a^*).
Definition
Let \mathcal be a *-algebra. An element a \in \mathcal is called self-adjoint if
The set of self-adjoint elements ...
. Using the self-adjoint and idempotent properties of
, for any
and
in
we have
,
, and
where
is the inner product associated with
. Therefore,
and
are orthogonal projections. The other direction, namely that if
is orthogonal then it is self-adjoint, follows from the implication from
to
for every
and
in
; thus
.
The existence of an orthogonal projection onto a closed subspace follows from the
Hilbert projection theorem.
Properties and special cases
An orthogonal projection is a
bounded operator. This is because for every
in the vector space we have, by the
Cauchy–Schwarz inequality
The Cauchy–Schwarz inequality (also called Cauchy–Bunyakovsky–Schwarz inequality) is an upper bound on the absolute value of the inner product between two vectors in an inner product space in terms of the product of the vector norms. It is ...
:
Thus
.
For finite-dimensional complex or real vector spaces, the
standard inner product can be substituted for
.
=Formulas
=
A simple case occurs when the orthogonal projection is onto a line. If
is a
unit vector
In mathematics, a unit vector in a normed vector space is a Vector (mathematics and physics), vector (often a vector (geometry), spatial vector) of Norm (mathematics), length 1. A unit vector is often denoted by a lowercase letter with a circumfle ...
on the line, then the projection is given by the
outer product
In linear algebra, the outer product of two coordinate vectors is the matrix whose entries are all products of an element in the first vector with an element in the second vector. If the two coordinate vectors have dimensions ''n'' and ''m'', the ...
(If
is complex-valued, the transpose in the above equation is replaced by a Hermitian transpose). This operator leaves u invariant, and it annihilates all vectors orthogonal to
, proving that it is indeed the orthogonal projection onto the line containing u. A simple way to see this is to consider an arbitrary vector
as the sum of a component on the line (i.e. the projected vector we seek) and another perpendicular to it,
. Applying projection, we get
by the properties of the
dot product
In mathematics, the dot product or scalar productThe term ''scalar product'' means literally "product with a Scalar (mathematics), scalar as a result". It is also used for other symmetric bilinear forms, for example in a pseudo-Euclidean space. N ...
of parallel and perpendicular vectors.
This formula can be generalized to orthogonal projections on a subspace of arbitrary
dimension
In physics and mathematics, the dimension of a mathematical space (or object) is informally defined as the minimum number of coordinates needed to specify any point within it. Thus, a line has a dimension of one (1D) because only one coo ...
. Let
be an
orthonormal basis
In mathematics, particularly linear algebra, an orthonormal basis for an inner product space V with finite Dimension (linear algebra), dimension is a Basis (linear algebra), basis for V whose vectors are orthonormal, that is, they are all unit vec ...
of the subspace
, with the assumption that the integer
, and let
denote the
matrix whose columns are
, i.e.,
. Then the projection is given by:
which can be rewritten as
The matrix
is the
partial isometry that vanishes on the
orthogonal complement of
, and
is the isometry that embeds
into the underlying vector space. The range of
is therefore the ''final space'' of
. It is also clear that
is the identity operator on
.
The orthonormality condition can also be dropped. If
is a (not necessarily orthonormal)
basis with
, and
is the matrix with these vectors as columns, then the projection is:
The matrix
still embeds
into the underlying vector space but is no longer an isometry in general. The matrix
is a "normalizing factor" that recovers the norm. For example, the
rank-1 operator
is not a projection if
After dividing by
we obtain the projection
onto the subspace spanned by
.
In the general case, we can have an arbitrary
positive definite matrix
defining an inner product
, and the projection
is given by
. Then
When the range space of the projection is generated by a
frame (i.e. the number of generators is greater than its dimension), the formula for the projection takes the form:
. Here
stands for the
Moore–Penrose pseudoinverse. This is just one of many ways to construct the projection operator.
If
is a non-singular matrix and
(i.e.,
is the
null space matrix of
), the following holds:
If the orthogonal condition is enhanced to
with
non-singular, the following holds:
All these formulas also hold for complex inner product spaces, provided that the
conjugate transpose is used instead of the transpose. Further details on sums of projectors can be found in Banerjee and Roy (2014). Also see Banerjee (2004) for application of sums of projectors in basic
spherical trigonometry
Spherical trigonometry is the branch of spherical geometry that deals with the metrical relationships between the edge (geometry), sides and angles of spherical triangles, traditionally expressed using trigonometric functions. On the sphere, ge ...
.
Oblique projections
The term ''oblique projections'' is sometimes used to refer to non-orthogonal projections. These projections are also used to represent spatial figures in two-dimensional drawings (see
oblique projection), though not as frequently as orthogonal projections. Whereas calculating the fitted value of an
ordinary least squares regression requires an orthogonal projection, calculating the fitted value of an
instrumental variables regression requires an oblique projection.
A projection is defined by its kernel and the basis vectors used to characterize its range (which is a complement of the kernel). When these basis vectors are orthogonal to the kernel, then the projection is an orthogonal projection. When these basis vectors are not orthogonal to the kernel, the projection is an oblique projection, or just a projection.
A matrix representation formula for a nonzero projection operator
Let
be a linear operator such that
and assume that
is not the zero operator. Let the vectors
form a basis for the range of
, and assemble these vectors in the
matrix
. Then
, otherwise
and
is the zero operator. The range and the kernel are complementary spaces, so the kernel has dimension
. It follows that the
orthogonal complement of the kernel has dimension
. Let
form a basis for the orthogonal complement of the kernel of the projection, and assemble these vectors in the matrix
. Then the projection
(with the condition
) is given by
This expression generalizes the formula for orthogonal projections given above. A standard proof of this expression is the following. For any vector
in the vector space
, we can decompose
, where vector
is in the image of
, and vector
So
, and then
is in the kernel of
, which is the null space of
In other words, the vector
is in the column space of
so
for some
dimension vector
and the vector
satisfies
by the construction of
. Put these conditions together, and we find a vector
so that
. Since matrices
and
are of full rank
by their construction, the
-matrix
is invertible. So the equation
gives the vector
In this way,
for any vector
and hence
.
In the case that
is an orthogonal projection, we can take
, and it follows that
. By using this formula, one can easily check that
. In general, if the vector space is over complex number field, one then uses the
Hermitian transpose and has the formula
. Recall that one can express the
Moore–Penrose inverse of the matrix
by
since
has full column rank, so
.
Singular values
is also an oblique projection. The singular values of
and
can be computed by an
orthonormal basis
In mathematics, particularly linear algebra, an orthonormal basis for an inner product space V with finite Dimension (linear algebra), dimension is a Basis (linear algebra), basis for V whose vectors are orthonormal, that is, they are all unit vec ...
of
. Let
be an orthonormal basis of
and let
be the
orthogonal complement of
. Denote the singular values of the matrix
by the positive values
. With this, the singular values for
are:
and the singular values for
are
This implies that the largest singular values of
and
are equal, and thus that the
matrix norm
In the field of mathematics, norms are defined for elements within a vector space. Specifically, when the vector space comprises matrices, such norms are referred to as matrix norms. Matrix norms differ from vector norms in that they must also ...
of the oblique projections are the same. However, the
condition number satisfies the relation
, and is therefore not necessarily equal.
Finding projection with an inner product
Let
be a vector space (in this case a plane) spanned by orthogonal vectors
. Let
be a vector. One can define a projection of
onto
as
where repeated indices are summed over (
Einstein sum notation). The vector
can be written as an orthogonal sum such that
.
is sometimes denoted as
. There is a theorem in linear algebra that states that this
is the smallest distance (the ''
orthogonal distance'') from
to
and is commonly used in areas such as
machine learning
Machine learning (ML) is a field of study in artificial intelligence concerned with the development and study of Computational statistics, statistical algorithms that can learn from data and generalise to unseen data, and thus perform Task ( ...
.
Canonical forms
Any projection
on a vector space of dimension
over a
field is a
diagonalizable matrix
In linear algebra, a square matrix A is called diagonalizable or non-defective if it is matrix similarity, similar to a diagonal matrix. That is, if there exists an invertible matrix P and a diagonal matrix D such that . This is equivalent to ...
, since its
minimal polynomial divides
, which splits into distinct linear factors. Thus there exists a basis in which
has the form
:
where
is the
rank of
. Here
is the
identity matrix
In linear algebra, the identity matrix of size n is the n\times n square matrix with ones on the main diagonal and zeros elsewhere. It has unique properties, for example when the identity matrix represents a geometric transformation, the obje ...
of size
,
is the
zero matrix
In mathematics, particularly linear algebra, a zero matrix or null matrix is a matrix all of whose entries are zero. It also serves as the additive identity of the additive group of m \times n matrices, and is denoted by the symbol O or 0 followe ...
of size
, and
is the
direct sum
The direct sum is an operation between structures in abstract algebra, a branch of mathematics. It is defined differently but analogously for different kinds of structures. As an example, the direct sum of two abelian groups A and B is anothe ...
operator. If the vector space is complex and equipped with an
inner product
In mathematics, an inner product space (or, rarely, a Hausdorff pre-Hilbert space) is a real vector space or a complex vector space with an operation called an inner product. The inner product of two vectors in the space is a scalar, ofte ...
, then there is an ''orthonormal'' basis in which the matrix of ''P'' is
:
where
. The
integer
An integer is the number zero (0), a positive natural number (1, 2, 3, ...), or the negation of a positive natural number (−1, −2, −3, ...). The negations or additive inverses of the positive natural numbers are referred to as negative in ...
s
and the real numbers
are uniquely determined.
. The factor
corresponds to the maximal invariant subspace on which
acts as an ''orthogonal'' projection (so that ''P'' itself is orthogonal if and only if
) and the
-blocks correspond to the ''oblique'' components.
Projections on normed vector spaces
When the underlying vector space
is a (not necessarily finite-dimensional)
normed vector space, analytic questions, irrelevant in the finite-dimensional case, need to be considered. Assume now
is a
Banach space
In mathematics, more specifically in functional analysis, a Banach space (, ) is a complete normed vector space. Thus, a Banach space is a vector space with a metric that allows the computation of vector length and distance between vectors and ...
.
Many of the algebraic results discussed above survive the passage to this context. A given direct sum decomposition of
into complementary subspaces still specifies a projection, and vice versa. If
is the direct sum
, then the operator defined by
is still a projection with range
and kernel
. It is also clear that
. Conversely, if
is projection on
, i.e.
, then it is easily verified that
. In other words,
is also a projection. The relation
implies
and
is the direct sum
.
However, in contrast to the finite-dimensional case, projections need not be
continuous in general. If a subspace
of
is not closed in the norm topology, then the projection onto
is not continuous. In other words, the range of a continuous projection
must be a closed subspace. Furthermore, the kernel of a continuous projection (in fact, a continuous linear operator in general) is closed. Thus a ''continuous'' projection
gives a decomposition of
into two complementary ''closed'' subspaces:
.
The converse holds also, with an additional assumption. Suppose
is a closed subspace of
. If there exists a closed subspace
such that , then the projection
with range
and kernel
is continuous. This follows from the
closed graph theorem. Suppose and . One needs to show that
. Since
is closed and , ''y'' lies in
, i.e. . Also, . Because
is closed and , we have
, i.e.
, which proves the claim.
The above argument makes use of the assumption that both
and
are closed. In general, given a closed subspace
, there need not exist a complementary closed subspace
, although for
Hilbert space
In mathematics, a Hilbert space is a real number, real or complex number, complex inner product space that is also a complete metric space with respect to the metric induced by the inner product. It generalizes the notion of Euclidean space. The ...
s this can always be done by taking the
orthogonal complement. For Banach spaces, a one-dimensional subspace always has a closed complementary subspace. This is an immediate consequence of
Hahn–Banach theorem
In functional analysis, the Hahn–Banach theorem is a central result that allows the extension of bounded linear functionals defined on a vector subspace of some vector space to the whole space. The theorem also shows that there are sufficient ...
. Let
be the linear span of
. By Hahn–Banach, there exists a bounded
linear functional
In mathematics, a linear form (also known as a linear functional, a one-form, or a covector) is a linear mapIn some texts the roles are reversed and vectors are defined as linear maps from covectors to scalars from a vector space to its field of ...
such that . The operator
satisfies
, i.e. it is a projection. Boundedness of
implies continuity of
and therefore
is a closed complementary subspace of
.
Applications and further considerations
Projections (orthogonal and otherwise) play a major role in
algorithm
In mathematics and computer science, an algorithm () is a finite sequence of Rigour#Mathematics, mathematically rigorous instructions, typically used to solve a class of specific Computational problem, problems or to perform a computation. Algo ...
s for certain linear algebra problems:
*
QR decomposition (see
Householder transformation and
Gram–Schmidt decomposition);
*
Singular value decomposition
In linear algebra, the singular value decomposition (SVD) is a Matrix decomposition, factorization of a real number, real or complex number, complex matrix (mathematics), matrix into a rotation, followed by a rescaling followed by another rota ...
* Reduction to
Hessenberg form (the first step in many
eigenvalue algorithms)
*
Linear regression
In statistics, linear regression is a statistical model, model that estimates the relationship between a Scalar (mathematics), scalar response (dependent variable) and one or more explanatory variables (regressor or independent variable). A mode ...
* Projective elements of matrix algebras are used in the construction of certain K-groups in
Operator K-theory
As stated above, projections are a special case of idempotents. Analytically, orthogonal projections are non-commutative generalizations of
characteristic functions. Idempotents are used in classifying, for instance,
semisimple algebras, while
measure theory
In mathematics, the concept of a measure is a generalization and formalization of geometrical measures (length, area, volume) and other common notions, such as magnitude (mathematics), magnitude, mass, and probability of events. These seemingl ...
begins with considering characteristic functions of
measurable sets. Therefore, as one can imagine, projections are very often encountered in the context of
operator algebra
In functional analysis, a branch of mathematics, an operator algebra is an algebra of continuous linear operators on a topological vector space, with the multiplication given by the composition of mappings.
The results obtained in the study o ...
s. In particular, a
von Neumann algebra
In mathematics, a von Neumann algebra or W*-algebra is a *-algebra of bounded operators on a Hilbert space that is closed in the weak operator topology and contains the identity operator. It is a special type of C*-algebra.
Von Neumann al ...
is generated by its complete
lattice of projections.
Generalizations
More generally, given a map between normed vector spaces
one can analogously ask for this map to be an isometry on the orthogonal complement of the kernel: that
be an isometry (compare
Partial isometry); in particular it must be
onto
In mathematics, a surjective function (also known as surjection, or onto function ) is a function such that, for every element of the function's codomain, there exists one element in the function's domain such that . In other words, for a f ...
. The case of an orthogonal projection is when ''W'' is a subspace of ''V.'' In
Riemannian geometry
Riemannian geometry is the branch of differential geometry that studies Riemannian manifolds, defined as manifold, smooth manifolds with a ''Riemannian metric'' (an inner product on the tangent space at each point that varies smooth function, smo ...
, this is used in the definition of a
Riemannian submersion.
See also
*
Centering matrix, which is an example of a projection matrix.
*
Dykstra's projection algorithm to compute the projection onto an intersection of sets
*
Invariant subspace
*
Least-squares spectral analysis
Least-squares spectral analysis (LSSA) is a method of estimating a Spectral density estimation#Overview, frequency spectrum based on a least-squares fit of Sine wave, sinusoids to data samples, similar to Fourier analysis. Fourier analysis, the ...
*
Orthogonalization
*
Properties of trace
Notes
References
*
*
*
* Brezinski, Claude: ''Projection Methods for Systems of Equations'', North-Holland, ISBN 0-444-82777-3 (1997).
External links
* , from MIT OpenCourseWare
* , by
Pavel Grinfeld.
Planar Geometric Projections Tutorial– a simple-to-follow tutorial explaining the different types of planar geometric projections.
{{linear algebra
Functional analysis
Linear algebra
Linear operators