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GENERALIZED EIGENVECTOR

  • Generalized eigenvector
  • Vector satisfying some of the criteria of an eigenvector

    In linear algebra, a generalized eigenvector of an n × n {\displaystyle n\times n} matrix A {\displaystyle A} is a vector which satisfies certain criteria

    Generalized eigenvector

    Generalized_eigenvector

  • Eigendecomposition of a matrix
  • Matrix decomposition

    {\displaystyle k} ⁠. That is, it is the space of generalized eigenvectors (in the first sense), where a generalized eigenvector is any vector which eventually becomes

    Eigendecomposition of a matrix

    Eigendecomposition_of_a_matrix

  • Eigenvalue algorithm
  • Numerical methods for matrix eigenvalue calculation

    also find eigenvectors. Given an n × n square matrix A of real or complex numbers, an eigenvalue λ and its associated generalized eigenvector v are a pair

    Eigenvalue algorithm

    Eigenvalue_algorithm

  • Dual linear program
  • Mathematical optimization concept

    solution to a linear programming problem can be regarded as a generalized eigenvector. The eigenequations of a square matrix are as follows: p T A =

    Dual linear program

    Dual_linear_program

  • Eigenvalues and eigenvectors
  • Concepts from linear algebra

    matrices, the notion of eigenvectors generalizes to generalized eigenvectors and the diagonal matrix of eigenvalues generalizes to the Jordan normal form

    Eigenvalues and eigenvectors

    Eigenvalues_and_eigenvectors

  • Jordan normal form
  • Form of a matrix indicating its eigenvalues and their algebraic multiplicities

    the complex Jordan form. For a real matrix the nonreal eigenvectors and generalized eigenvectors can always be chosen to form complex conjugate pairs.

    Jordan normal form

    Jordan_normal_form

  • Canonical basis
  • Basis of a type of algebraic structure

    In linear algebra, it refers to a set of n linearly independent generalized eigenvectors of an n×n matrix A {\displaystyle A} , if the set is composed entirely

    Canonical basis

    Canonical_basis

  • Spectral theorem
  • Result about when a matrix can be diagonalized

    delta-functions are "generalized eigenvectors" of A {\displaystyle A} but not eigenvectors in the usual sense. In the absence of (true) eigenvectors, one can look

    Spectral theorem

    Spectral_theorem

  • Principal component analysis
  • Method of data analysis

    the variance that each eigenvector represents can be calculated by dividing the eigenvalue corresponding to that eigenvector by the sum of all eigenvalues

    Principal component analysis

    Principal component analysis

    Principal_component_analysis

  • Modal matrix
  • of one linearly independent generalized eigenvector of rank 3 (generalized eigenvector rank; see generalized eigenvector), two of rank 2 and four of rank

    Modal matrix

    Modal_matrix

  • Defective matrix
  • Non-diagonalizable matrix; one lacking a basis of eigenvectors

    n} linearly independent eigenvectors. A complete basis is formed by augmenting the eigenvectors with generalized eigenvectors, which are necessary for

    Defective matrix

    Defective_matrix

  • Eigenvector centrality
  • Measure in graph theory

    algorithms that may be used to find this dominant eigenvector. Furthermore, this can be generalized so that the entries in A can be real numbers representing

    Eigenvector centrality

    Eigenvector_centrality

  • Rank
  • Position in a hierarchy

    subset Rank of an elliptic curve Rank of a free module Rank of a generalized eigenvector Rank of a greedoid, the maximal size of a feasible set Rank of

    Rank

    Rank

  • Discrete Fourier transform
  • Function in discrete mathematics

    Ding, J. J., Hsue, W. L., & Chang, K. W. (2008). Generalized commuting matrices and their eigenvectors for DFTs, offset DFTs, and other periodic operations

    Discrete Fourier transform

    Discrete Fourier transform

    Discrete_Fourier_transform

  • Schrödinger equation
  • Description of a quantum-mechanical system

    eigenstates, composed of elements outside the Hilbert space, as "generalized eigenvectors". These are used for calculational convenience and do not represent

    Schrödinger equation

    Schrödinger_equation

  • Center manifold
  • Mathematical concept

    system, and then compute its eigenvalues and eigenvectors. The eigenvectors (and generalized eigenvectors if they occur) corresponding to eigenvalues with

    Center manifold

    Center_manifold

  • Generalized pencil-of-function method
  • Signal processing technique

    which are λ = z i {\displaystyle \lambda =z_{i}} . Then, the generalized eigenvectors p i {\displaystyle p_{i}} can be obtained by the following identities:

    Generalized pencil-of-function method

    Generalized pencil-of-function method

    Generalized_pencil-of-function_method

  • Symmetrizable compact operator
  • Mathematical compact operator

    is true for generalized eigenvalues since powers of K − λI and K* − λI are also Fredholm of index 0. Since any generalized λ eigenvector of A is already

    Symmetrizable compact operator

    Symmetrizable_compact_operator

  • Self-adjoint operator
  • Linear operator equal to its own adjoint

    would say that the eigenvectors are "non-normalizable.") Physicists would then go on to say that these "generalized eigenvectors" form an "orthonormal

    Self-adjoint operator

    Self-adjoint_operator

  • Definite matrix
  • Property of a mathematical matrix

    matrix having as columns the generalized eigenvectors and Λ {\displaystyle \Lambda } is a diagonal matrix of the generalized eigenvalues. Now premultiplication

    Definite matrix

    Definite_matrix

  • Quantum state
  • Mathematical entity to describe the probability of each possible measurement on a system

    \psi } is a pure state belonging to H {\displaystyle H} , the (generalized) eigenvectors of the position operator do not. Though closely related, pure

    Quantum state

    Quantum_state

  • Schur's lemma
  • Homomorphisms between simple modules over the same ring are isomorphisms or zero

    (z))^{n}m=0} , i.e. if every m ∈ M {\displaystyle m\in M} is a generalized eigenvector of z {\displaystyle z} with eigenvalue χ ( z ) {\displaystyle \chi

    Schur's lemma

    Schur's_lemma

  • Eigenmoments
  • equation, w {\displaystyle w} is called a generalized eigenvector and λ {\displaystyle \lambda } is called a generalized eigenvalue. Finding w {\displaystyle

    Eigenmoments

    Eigenmoments

  • Dirac delta function
  • Generalized function whose value is zero everywhere except at zero

    {\displaystyle P\varphi _{y}=y\varphi _{y}.} That is, φy are the generalized eigenvectors of P. If they form an "orthonormal basis" in the distribution sense

    Dirac delta function

    Dirac delta function

    Dirac_delta_function

  • Bra–ket notation
  • Notation for quantum states

    =\mathbf {r} |\mathbf {r} \rangle .} The position states are "generalized eigenvectors", not elements of the Hilbert space itself, and do not form a countable

    Bra–ket notation

    Bra–ket_notation

  • Diagonalizable matrix
  • Matrices similar to diagonal matrices

    corresponding eigenvalues of T {\displaystyle T} ; with respect to this eigenvector basis, T {\displaystyle T}  is represented by D {\displaystyle D} . Diagonalization

    Diagonalizable matrix

    Diagonalizable_matrix

  • Quantum logic
  • Theory of logic to account for observations from quantum theory

    operator f(A) is a self-adjoint projection onto the subspace of generalized eigenvectors of A with eigenvalue in [a,b]. That subspace can be interpreted

    Quantum logic

    Quantum_logic

  • Schur decomposition
  • Matrix factorisation in mathematics

    T are upper triangular. The generalized Schur decomposition is also sometimes called the QZ decomposition. The generalized eigenvalues λ {\displaystyle

    Schur decomposition

    Schur_decomposition

  • Position operator
  • Operator in quantum mechanics

    }} ), surjective, endowed with complete families of generalized eigenvectors and real generalized eigenvalues. It is self-adjoint with respect to the

    Position operator

    Position_operator

  • Jordan matrix
  • Block diagonal matrix of Jordan blocks

    represented by Jordan blocks) of the domain which the associated generalized eigenvectors make a basis for. Let A ∈ M n ( C ) {\displaystyle A\in \mathbb

    Jordan matrix

    Jordan_matrix

  • Graph Fourier transform
  • Mathematical transform

    eigenvalues and eigenvectors. Analogously to the classical Fourier transform, the eigenvalues represent frequencies and eigenvectors form what is known

    Graph Fourier transform

    Graph_Fourier_transform

  • Centrality
  • Degree of connectedness within a graph

    algorithms that may be used to find this dominant eigenvector. Furthermore, this can be generalized so that the entries in A can be real numbers representing

    Centrality

    Centrality

    Centrality

  • Nonlinear eigenproblem
  • Type of equation involving matrix-valued functions

    x r − 1 {\displaystyle x_{0},x_{1},\dots ,x_{r-1}} are called generalized eigenvectors, r {\displaystyle r} is called the length of the Jordan chain,

    Nonlinear eigenproblem

    Nonlinear_eigenproblem

  • Vector space model
  • Model for representing text documents

    Champion list Compound term processing Conceptual space Eigenvalues and eigenvectors Inverted index Nearest neighbor search Sparse distributed memory w-shingling

    Vector space model

    Vector_space_model

  • Eigenvalue perturbation
  • Concept in mathematics

    finding the eigenvectors and eigenvalues of a system A x = λ x {\displaystyle Ax=\lambda x} that is perturbed from one with known eigenvectors and eigenvalues

    Eigenvalue perturbation

    Eigenvalue_perturbation

  • Gauss–Markov theorem
  • Theorem related to ordinary least squares

    {k} =(k_{1},\dots ,k_{p+1})^{T}\in \mathbb {R} ^{(p+1)\times 1}} be an eigenvector of H {\displaystyle {\mathcal {H}}} . k ≠ 0 ⟹ ( k 1 v 1 + ⋯ + k p + 1

    Gauss–Markov theorem

    Gauss–Markov_theorem

  • Drazin inverse
  • {\displaystyle A_{s}} . Constrained generalized inverse Inverse element Moore–Penrose inverse Jordan normal form Generalized eigenvector Drazin, M. P. (1958). "Pseudo-inverses

    Drazin inverse

    Drazin_inverse

  • Rigged Hilbert space
  • Construction for adding objects to a Hilbert space

    introduced to study spectral theory. They bring together the 'bound state' (eigenvector) and 'continuous spectrum', in one place. Using this notion, a version

    Rigged Hilbert space

    Rigged_Hilbert_space

  • Riemann hypothesis
  • Conjecture on zeros of the zeta function

    would also work for the generalized Riemann hypothesis for Dirichlet L-functions. Several results first proved using the generalized Riemann hypothesis were

    Riemann hypothesis

    Riemann hypothesis

    Riemann_hypothesis

  • Chain (disambiguation)
  • Topics referred to by the same term

    using arrows Jordan chain, a sequence of linearly independent generalized eigenvectors of descending rank Markov chain, a discrete-time stochastic process

    Chain (disambiguation)

    Chain_(disambiguation)

  • Rayleigh quotient
  • Construct for Hermitian matrices

    {\displaystyle x} is v min {\displaystyle v_{\min }} (the corresponding eigenvector). Similarly, R ( M , x ) ≤ λ max {\displaystyle R(M,x)\leq \lambda _{\max

    Rayleigh quotient

    Rayleigh_quotient

  • Markov chain
  • Random process independent of past history

    ) multiple of a left eigenvector e of the transition matrix P with an eigenvalue of 1. If there is more than one unit eigenvector then a weighted sum of

    Markov chain

    Markov chain

    Markov_chain

  • Bethe ansatz
  • Method for finding the exact solution of certain quantum mechanics models

    eigenvalues and eigenvectors of the one-dimensional antiferromagnetic isotropic (XXX) Heisenberg model. The approach was later generalized into the quantum

    Bethe ansatz

    Bethe_ansatz

  • Laguerre polynomials
  • Sequence of differential equation solutions

    L_{n}^{(\alpha )}(x),} which shows that L(α) n is an eigenvector for the eigenvalue n. The generalized Laguerre polynomials are orthogonal over [0, ∞) with

    Laguerre polynomials

    Laguerre polynomials

    Laguerre_polynomials

  • Rotation
  • Movement of an object which leaves at least one point unchanged

    the existence of such a direction is the question of existence of an eigenvector for the matrix A representing the rotation. Every 2D rotation around

    Rotation

    Rotation

    Rotation

  • Decomposition of spectrum (functional analysis)
  • Construction in functional analysis, useful to solve differential equations

    operators, these states are referred to as "generalized eigenvectors" of an observable with "generalized eigenvalues" that do not necessarily belong to

    Decomposition of spectrum (functional analysis)

    Decomposition_of_spectrum_(functional_analysis)

  • Characteristic polynomial
  • Polynomial whose roots are the eigenvalues of a matrix

    matrix. Eigenvalues and eigenvectors play a fundamental role in linear algebra, since, given a linear transformation, an eigenvector is a vector whose direction

    Characteristic polynomial

    Characteristic_polynomial

  • Gordon Eugene Martin
  • American physicist (born 1925)

    contracted with the Navy for high-resolution beamforming with generalized eigenvector/eigenvalue (GEVEV) digital signal processing from 1985 through

    Gordon Eugene Martin

    Gordon Eugene Martin

    Gordon_Eugene_Martin

  • Rigid body dynamics
  • Study of the effects of forces on undeformable bodies

    {q}}}}\right),} is the generalized force acting on this one degree of freedom system. If the mechanical system is defined by m generalized coordinates, qj,

    Rigid body dynamics

    Rigid body dynamics

    Rigid_body_dynamics

  • Quadratic eigenvalue problem
  • and solve a generalized eigenvalue problem. Once eigenvalues and eigenvectors of the linear problem have been determined, eigenvectors and eigenvalues

    Quadratic eigenvalue problem

    Quadratic_eigenvalue_problem

  • LOBPCG
  • Method for finding largest (or smallest) eigenvalues

    largest (or smallest) eigenvalues and the corresponding eigenvectors of a symmetric generalized eigenvalue problem A x = λ B x , {\displaystyle Ax=\lambda

    LOBPCG

    LOBPCG

  • Hermitian matrix
  • Matrix equal to its conjugate-transpose

    like Fourier analysis and signal representation. The eigenvalues and eigenvectors of Hermitian matrices play a crucial role in analyzing signals and extracting

    Hermitian matrix

    Hermitian_matrix

  • Spectrum of a matrix
  • Set of a matrix's eigenvalues

    by matrix multiplication. We now say that x ∈ V is an eigenvector of M if x is an eigenvector of T. Similarly, λ ∈ K is an eigenvalue of M if it is an

    Spectrum of a matrix

    Spectrum_of_a_matrix

  • EISPACK
  • banded, real symmetric tridiagonal, special real tridiagonal, generalized real, and generalized real symmetric matrices. In addition, it includes subroutines

    EISPACK

    EISPACK

  • Fractional anisotropy
  • Non-uniformity of a diffusion process

    the corresponding eigenvalues give the magnitude of the peak in each eigenvector direction. FA = 3 2 ( ( λ 1 − λ ^ ) 2 + ( λ 2 − λ ^ ) 2 + ( λ 3 − λ ^

    Fractional anisotropy

    Fractional_anisotropy

  • Slow manifold
  • subspace is the slow subspace given by the span of the eigenvectors, and generalized eigenvectors, corresponding to the eigenvalue λ = 0 {\displaystyle

    Slow manifold

    Slow_manifold

  • Singular value decomposition
  • Matrix decomposition

    \mathbf {u} } ⁠ is a unit length eigenvector of ⁠ M {\displaystyle \mathbf {M} } ⁠. For every unit-length eigenvector ⁠ v {\displaystyle \mathbf {v} }

    Singular value decomposition

    Singular value decomposition

    Singular_value_decomposition

  • Wannier equation
  • -representation is useful when introducing the generalized Wannier equation. The Wannier equation can be generalized by including the presence of many electrons

    Wannier equation

    Wannier_equation

  • Generalizations of Pauli matrices
  • Families of matrices in mathematics, physics, and quantum information

    particular quantum information, the term generalized Pauli matrices refers to families of matrices which generalize the (linear algebraic) properties of the

    Generalizations of Pauli matrices

    Generalizations_of_Pauli_matrices

  • Triangular matrix
  • Special kind of square matrix

    by using induction on the fact that A has an eigenvector, by taking the quotient space by the eigenvector and inducting to show that A stabilizes a flag

    Triangular matrix

    Triangular_matrix

  • Dimensionality reduction
  • Process of reducing the number of random variables under consideration

    correlation) matrix of the data is constructed and the eigenvectors on this matrix are computed. The eigenvectors that correspond to the largest eigenvalues (the

    Dimensionality reduction

    Dimensionality_reduction

  • Laplacian matrix
  • Matrix representation of a graph

    cut of a graph can be approximated through the Fiedler vector — the eigenvector corresponding to the second smallest eigenvalue of the graph Laplacian

    Laplacian matrix

    Laplacian_matrix

  • Algebra representation
  • Study of abstract algebraic structures

    but the analysis is much more difficult. Eigenvalues and eigenvectors can be generalized to algebra representations. The generalization of an eigenvalue

    Algebra representation

    Algebra_representation

  • Second derivative
  • Mathematical operation

    well-known cases, see Eigenvalues and eigenvectors of the second derivative. The second derivative generalizes to higher dimensions through the notion

    Second derivative

    Second derivative

    Second_derivative

  • Rotation matrix
  • Matrix representing a Euclidean rotation

    v with (R – I)v = 0, that is Rv = v, a fixed eigenvector. There may also be pairs of fixed eigenvectors in the even-dimensional subspace orthogonal to

    Rotation matrix

    Rotation_matrix

  • SLEPc
  • is a software library for the parallel computation of eigenvalues and eigenvectors of large, sparse matrices. It can be seen as a module of PETSc that provides

    SLEPc

    SLEPc

  • Translation functor
  • algebra is said to have central character χλ if every vector v is a generalized eigenvector of the center Z with eigenvalue χλ; in other words if z∈Z and v∈V

    Translation functor

    Translation_functor

  • Katz centrality
  • Measure of centrality in a network based on nodal influence

    between a pair of actors. It is similar to Google's PageRank and to the eigenvector centrality. Katz centrality computes the relative influence of a node

    Katz centrality

    Katz centrality

    Katz_centrality

  • Weight (representation theory)
  • Concept in Lie algebra representation theory

    a basis of V consisting of simultaneous eigenvectors of all elements of S. Each of these common eigenvectors v ∈ V defines a linear functional on the

    Weight (representation theory)

    Weight_(representation_theory)

  • Chi-squared distribution
  • Probability distribution and special case of gamma distribution

    {\displaystyle {\bar {1}}} the all ones vector. M {\displaystyle M} has one eigenvector b 1 := 1 n 1 ¯ {\displaystyle b_{1}:={\textstyle {\frac {1}{\sqrt {n}}}}{\bar

    Chi-squared distribution

    Chi-squared distribution

    Chi-squared_distribution

  • Matrix (mathematics)
  • Array of numbers

    expressible as a linear combination of eigenvectors. In both cases, all eigenvalues are real. This theorem can be generalized to infinite-dimensional situations

    Matrix (mathematics)

    Matrix (mathematics)

    Matrix_(mathematics)

  • Window function
  • Function used in signal processing

    values of N) to L × σt for σt < 0.14. A more generalized version of the Gaussian window is the generalized normal window. Retaining the notation from the

    Window function

    Window function

    Window_function

  • Canonical transformation
  • Coordinate transformation that preserves the form of Hamilton's equations

    is much broader, since the old generalized coordinates, momenta and even time may be combined to form the new generalized coordinates and momenta. Canonical

    Canonical transformation

    Canonical_transformation

  • Courant minimax principle
  • the eigenvector, and its length is the eigenvalue. All other eigenvectors will be perpendicular to this. The minimax principle also generalizes to eigenvalues

    Courant minimax principle

    Courant_minimax_principle

  • Spectral theory
  • Collection of mathematical theories

    mathematics, spectral theory is an inclusive term for theories extending the eigenvector and eigenvalue theory of a single square matrix to a much broader theory

    Spectral theory

    Spectral_theory

  • Jacobi eigenvalue algorithm
  • Numerical linear algebra algorithm

    algorithm is an iterative method for the calculation of the eigenvalues and eigenvectors of a real symmetric matrix (a process known as diagonalization). It is

    Jacobi eigenvalue algorithm

    Jacobi_eigenvalue_algorithm

  • Arnoldi iteration
  • Iterative method for approximating eigenvectors

    iterative method. Arnoldi finds an approximation to the eigenvalues and eigenvectors of general (possibly non-Hermitian) matrices by constructing an orthonormal

    Arnoldi iteration

    Arnoldi_iteration

  • Cauchy–Schwarz inequality
  • Mathematical inequality relating inner products and norms

    {u} } is an eigenvector of A 2 {\displaystyle A^{2}} . From here it is straightforward to deduce that A {\displaystyle A} has an eigenvector, then the spectral

    Cauchy–Schwarz inequality

    Cauchy–Schwarz_inequality

  • Bloch sphere
  • Representation of a quantum mechanical system

    \rangle } invariant must have | ψ ⟩ {\displaystyle |\psi \rangle } as an eigenvector. Since the corresponding eigenvalue must be a complex number of modulus

    Bloch sphere

    Bloch sphere

    Bloch_sphere

  • Exceptional point
  • Singularities in the parameter space

    in the parameter space where two or more eigenstates (eigenvalues and eigenvectors) coalesce. These points appear in dissipative systems, which make the

    Exceptional point

    Exceptional_point

  • NetworkX
  • Python library for graphs and networks

    come from the third eigenvector. Scale and center the resulting layout as needed. Nodes in dense clusters have similar eigenvector entries, causing them

    NetworkX

    NetworkX

    NetworkX

  • Normal matrix
  • Matrix that commutes with its conjugate transpose

    and the columns of U are the eigenvectors of A. The matching eigenvalues in Λ come in the same order as the eigenvectors are ordered as columns of U.

    Normal matrix

    Normal_matrix

  • Born rule
  • Calculation rule in quantum mechanics

    {\displaystyle \lambda _{i}} is one-dimensional and spanned by the normalized eigenvector | λ i ⟩ {\displaystyle |\lambda _{i}\rangle } , P i {\displaystyle P_{i}}

    Born rule

    Born_rule

  • Skew-Hermitian matrix
  • Matrix whose conjugate transpose is its negative (additive inverse)

    skew-Hermitian matrices are normal. Hence they are diagonalizable and their eigenvectors for distinct eigenvalues must be orthogonal. All entries on the main

    Skew-Hermitian matrix

    Skew-Hermitian_matrix

  • Neumann–Poincaré operator
  • Non-self-adjoint compact operator used to solve boundary value problems for the Laplacian

    each of the statements for either T or T*. To check that T has no generalized eigenvectors with eigenvalue 1/2 it suffices to show that T K φ − 1 2 φ = 1

    Neumann–Poincaré operator

    Neumann–Poincaré_operator

  • Liouville field theory
  • Two-dimensional conformal field theory

    is called the coupling constant. In a free field theory, the energy eigenvectors e 2 α φ {\displaystyle e^{2\alpha \varphi }} are linearly independent

    Liouville field theory

    Liouville_field_theory

  • Linear algebra
  • Branch of mathematics

    If f is a linear endomorphism of a vector space V over a field F, an eigenvector of f is a nonzero vector v of V such that f(v) = av for some scalar a

    Linear algebra

    Linear algebra

    Linear_algebra

  • Compact operator on Hilbert space
  • Functional analysis concept

    the existence of one eigenvector x {\displaystyle x} of T {\displaystyle T} . In finite dimension, the existence of an eigenvector can be shown in (at

    Compact operator on Hilbert space

    Compact_operator_on_Hilbert_space

  • Measurement in quantum mechanics
  • Interaction of a quantum system with a classical observer

    spectral theory; the present article will avoid them whenever possible. The eigenvectors of a von Neumann observable form an orthonormal basis for the Hilbert

    Measurement in quantum mechanics

    Measurement_in_quantum_mechanics

  • Regular representation
  • Representation theory of groups

    simultaneous eigenvectors for all the n×n circulants. In fact if ζ is any n-th root of unity, the element 1 + ζg + ζ2g2 + ... + ζn−1gn−1 is an eigenvector for

    Regular representation

    Regular_representation

  • Backfitting algorithm
  • Iterative procedure

    procedure used to fit a generalized additive model. It was introduced in 1985 by Leo Breiman and Jerome Friedman along with generalized additive models. In

    Backfitting algorithm

    Backfitting_algorithm

  • Multidimensional scaling
  • Set of related ordination techniques used in information visualization

    {\textstyle \lambda _{1},\lambda _{2},...,\lambda _{m}} and corresponding eigenvectors e 1 , e 2 , . . . , e m {\textstyle e_{1},e_{2},...,e_{m}} of B {\textstyle

    Multidimensional scaling

    Multidimensional scaling

    Multidimensional_scaling

  • Dynamic mode decomposition
  • Dimensionality reduction algorithm

    {\displaystyle y} is an eigenvector of S {\displaystyle S} , then V 1 N − 1 y {\displaystyle V_{1}^{N-1}y} is an approximate eigenvector of A {\displaystyle

    Dynamic mode decomposition

    Dynamic_mode_decomposition

  • Segmentation-based object categorization
  • number of pixels in the image. Since only one eigenvector, corresponding to the second smallest generalized eigenvalue, is used by the uncut algorithm,

    Segmentation-based object categorization

    Segmentation-based_object_categorization

  • Oja's rule
  • Model of how neurons in the brain or artificial neural networks learn over time

    is a single-neuron special case of the Generalized Hebbian Algorithm. However, Oja's rule can also be generalized in other ways to varying degrees of stability

    Oja's rule

    Oja's_rule

  • Fractional Brownian motion
  • Probability theory concept

    i {\displaystyle i} -th column is the eigenvector v i {\displaystyle \,v_{i}} . Note that since the eigenvectors are linearly independent, the matrix P

    Fractional Brownian motion

    Fractional_Brownian_motion

  • Hebbian theory
  • Neuroscientific theory

    ^{*}\mathbf {x} } Because, again, c ∗ {\displaystyle \mathbf {c} ^{*}} is the eigenvector corresponding to the largest eigenvalue of the correlation matrix between

    Hebbian theory

    Hebbian_theory

  • Canonical correlation
  • Way of inferring information from cross-covariance matrices

    the maximum of correlation is attained if c {\displaystyle c} is the eigenvector with the maximum eigenvalue for the matrix Σ X X − 1 / 2 Σ X Y Σ Y Y

    Canonical correlation

    Canonical_correlation

  • Square matrix
  • Matrix with the same number of rows and columns

    eigenbasis; i.e., every vector is expressible as a linear combination of eigenvectors. In both cases, all eigenvalues are real. A symmetric n×n-matrix is called

    Square matrix

    Square matrix

    Square_matrix

  • Gaussian function
  • Mathematical function

    matrix C {\displaystyle C} and changing the integration variables to the eigenvectors of C {\displaystyle C} . More generally a shifted Gaussian function is

    Gaussian function

    Gaussian_function

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  • Squire
  • Surname or Lastname

    English

    Squire

    English : status name from Middle English squyer ‘esquire’, ‘a man belonging to the feudal rank immediately below that of knight’ (from Old French esquier ‘shield bearer’). At first it denoted a young man of good birth attendant on a knight, or by extension any attendant or servant, but by the 14th century the meaning had been generalized, and referred to social status rather than age. By the 17th century, the term denoted any member of the landed gentry, but this is unlikely to have influenced the development of the surname.

    Squire

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Online names & meanings

  • Udayveer
  • Boy/Male

    Indian, Punjabi, Sikh

    Udayveer

    Loving / Joyful

  • Prateechi
  • Girl/Female

    Hindu, Indian

    Prateechi

    Prayer

  • Adhinath | அதிநத
  • Boy/Male

    Tamil

    Adhinath | அதிநத

    The first Lord or Lord Vishnu

  • Vanini | வநிநீ
  • Girl/Female

    Tamil

    Vanini | வநிநீ

    Soft spoken

  • Jawa
  • Girl/Female

    Hindu

    Jawa

    Flower

  • Rainhardt
  • Boy/Male

    German

    Rainhardt

    Strong Judgment

  • Dann
  • Boy/Male

    Hebrew

    Dann

    Judge. Biblical fifth son of Jacob and founder of one of the twelve tribes of Israel. An...

  • Saihajamrit
  • Girl/Female

    Sikh

    Saihajamrit

    Love for coast

  • Dahbal
  • Boy/Male

    Indian

    Dahbal

    This ws the name of Wahb Ibn

  • APRONADIUS
  • Male

    Egyptian

    APRONADIUS

    , Asshur-nadin, ("Asshur gives").

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GENERALIZED EIGENVECTOR

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GENERALIZED EIGENVECTOR

  • Mineralize
  • v. t.

    To impregnate with a mineral; as, mineralized water.

  • Generalize
  • v. t.

    To bring under a genus or under genera; to view in relation to a genus or to genera.

  • Universalize
  • v. t.

    To make universal; to generalize.

  • Generalized
  • a.

    Comprising structural characters which are separated in more specialized forms; synthetic; as, a generalized type.

  • Generalizable
  • a.

    Capable of being generalized, or reduced to a general form of statement, or brought under a general rule.

  • Centralization
  • n.

    The act or process of centralizing, or the state of being centralized; the act or process of combining or reducing several parts into a whole; as, the centralization of power in the general government; the centralization of commerce in a city.

  • Generalized
  • imp. & p. p.

    of Generalize

  • Generalize
  • v. t.

    To derive or deduce (a general conception, or a general principle) from particulars.

  • Amphioxus
  • n.

    A fishlike creature (Amphioxus lanceolatus), two or three inches long, found in temperature seas; -- also called the lancelet. Its body is pointed at both ends. It is the lowest and most generalized of the vertebrates, having neither brain, skull, vertebrae, nor red blood. It forms the type of the group Acrania, Leptocardia, etc.

  • Manifoldness
  • n.

    A generalized concept of magnitude.

  • Federalized
  • imp. & p. p.

    of Federalize

  • Induce
  • v. t.

    To generalize or conclude as an inference from all the particulars; -- the opposite of deduce.

  • Generalize
  • v. i.

    To form into a genus; to view objects in their relations to a genus or class; to take general or comprehensive views.

  • Centralized
  • imp. & p. p.

    of Centralize

  • Mineralized
  • imp. & p. p.

    of Mineralize

  • Generalizer
  • n.

    One who takes general or comprehensive views.

  • Generalizing
  • p. pr. & vb. n.

    of Generalize

  • Centralism
  • n.

    The system by which power is centralized, as in a government.

  • Generalize
  • v. t.

    To apply to other genera or classes; to use with a more extensive application; to extend so as to include all special cases; to make universal in application, as a formula or rule.