For a basis e1,…,en with cyclic indexing, the vectors ej+ej+1 have coefficient matrix I+S, where S cyclically shifts coordinates. Its determinant is 1−(−1)n. They therefore form a basis exactly when n is odd over a field of characteristic different from two. For even n, alternating coefficients produce a nontrivial linear dependence.
Every linearly independent subset of a finite-dimensional vector space extends to a basis. Starting with its vectors, add a vector outside their current span until the span is the whole space. Each addition preserves linear independence, and the process stops because the dimension is finite. This also lets a linear functional on a vector subspace extend to the ambient space by assigning arbitrary values on the additional basis vectors.
The standard basis of the vector space Rn consists of the vectors ei whose ith coordinate is one and whose other coordinates are zero. Every vector x has the unique expression x=∑ixiei in this basis.
If a vector space is spanned by n vectors, every linearly independent family in it has at most n members. Consequently, any two finite bases have the same number of vectors.
For polynomials in fixed variables and of a fixed degree, the monomials of that degree form a basis of the corresponding homogeneous component.
Ancestors (6)
Incoming links (501)
- Adjacent sums of a cyclic basis
- Affine Lie algebra of the line
- Algebraic integer
- Antisymmetry of a Lie bracket
- Basis
- Basis extension
- Basis of a topology
- Bernstein filtration
- Bidual evaluation map
- Boolean multilinearization
- Change of basis
- Change-of-basis matrix
- Circulant matrix
- Closed-path corner of a path algebra is a domain
- Complete flag
- Connection components
- Coordinate basis
- Criterion for membership in a diagonal basis
- Determinant of Hermitian congruence
- Discrete Fourier transform
- Dual basis
- Dual pairing
- Dual space
- Eigenbasis
- Exterior square of a direct sum
- Failure of Lie theorem in positive characteristic
- Field norm
- Field with four elements
- Finite-dimensional vector space
- Finite element method
- Finite field
- Flag (linear algebra)
- Free module
- Fundamental matrix of a linear differential equation
- Generalized-weight decomposition for a nilpotent Lie algebra
- Gram-Schmidt process
- Group representation
- Hermitian form
- Hyperbolic function
- Hyperbolic plane (quadratic form)
- Independence of eigenvectors for distinct eigenvalues
- Infinite-dimensional vector space
- Invertible matrix
- Lagrange cardinal polynomial
- Lattice point
- Length bound for a Schur module
- Length-two Jordan chain solution
- Lie algebra
- Lie theory
- Linear algebra
- Linear dependence
- Linear independence
- Matrix coefficient
- Matrix determinant lemma
- Matrix trace
- Matrix unit
- Mészáros equation solution basis
- Mixed state
- Monomial alternant
- Nondegenerate bilinear form
- Norm for a finite free ring extension
- Number field
- Order-p matrices in GL2 over the prime field
- Orthonormal basis
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- Piecewise-linear hat function
- Prime field
- QR decomposition
- Quantum plane
- Quantum superposition
- Quantum torus
- Quotient theorem for Cartesian tensors
- Rank-nullity theorem
- Right inverse
- Rotation matrix
- Row Hermite normal form in rank two
- Row lattice of an integer matrix
- Schur orthogonality relations
- Sesquilinear form
- Shape operator
- Sharply three-transitive on a projective line
- Simple coroot
- Simultaneous triangularization of a Lie algebra representation
- Sphere center from three tetrahedron face distances
- Square matrix
- Standard basis
- Standard Young tableau
- Symmetric bilinear form
- Symplectic basis
- Tangent space by point derivations
- Tensor-product basis
- Two-dimensional lattice reconstruction from vector lengths
- Universal property of a tensor product
- Variational characterization of trace distance
- Vector space
- Vector-space freeness from maximal independence
- Vector subspace
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