The determinant is the alternating multilinear volume scale of a square matrix; it is nonzero exactly for invertible matrices.
The block matrix M=(AB−BA) is similar over C to diag(A+iB,A−iB) via T=(I−iIIiI). Therefore its determinant is det(A+iB)det(A−iB) for arbitrary square matrices A,B. The argument uses a constant change-of-basis matrix and multiplicativity of the determinant.
For a differentiable invertible matrix A(t), dtdlogdetA=tr(A−1A˙) wherever a consistent logarithm is defined. In particular a positive spatial metric tensor satisfies hijh˙ij=h˙/h. This separates its local volume change from shape change.
For an invertible matrix A and any matrix H,Indeed det(A+tH)=det(A)det(I+tA−1H), and multilinearity shows that the linear coefficient of det(I+tB) is trB. At a singular matrix the derivative is instead written tr(adj(A)H); this polynomial formula holds for all A.
D(det)A(H)=det(A)tr(A−1H).
On positive-definite matrices, the log-determinant has differential dlogdetA=Tr(A−1dA) and is a strictly concave function.
The determinant is linear in each row and in each column when all the others are held fixed.
For diagonal entries ai, superdiagonal entries bi, and subdiagonal entries ci, the leading principal determinants satisfy
dn=andn−1−bn−1cn−1dn−2,d0=1,d1=a1.
Ancestors (6)
Incoming links (520)
- Accretive complex quadratic reciprocal Fourier transform
- Adjacent sums of a cyclic basis
- Alexander breadth bound on Seifert genus
- Alternating bilinear form
- Analytic determinant square root for accretive symmetric matrices
- Automorphism of a one-dimensional complex torus
- Block diagonal matrix
- Cartesian second-rank tensor
- Closed fermion loop sign
- Complex-linear map
- Complex special linear group in dimension two
- Counterterm closure of a massive Yukawa theory
- Cusp holomorphy under rational slash operators
- Determinantal point process
- Determinant line bundle
- Determinant-normalized slash operator
- Determinant of a complex block representation
- Determinant of Hermitian congruence
- Determinant twist
- Direct-product decomposition of the cube symmetry group
- Dust gravitational dispersion relation with gas drag
- Euclidean invariance of the shape operator
- Fixed-point congruence for an involution on an odd-sphere connected sum
- Full-row-rank matrix manifold
- Gaussian path integral
- Gaussian specific-heat infrared threshold
- Highest-weight classification of rational GL representations
- Instanton fluctuation prefactor
- Jacobian determinant
- Keller--Segel aggregation threshold
- Lagrange optical invariant
- Leading coefficient of an exponential alternant
- Liouville formula for a fundamental matrix
- Lower triangular matrix
- Matrix exponential determinant identity
- Monomial alternant
- Multilinear map
- Odd-dimensional orthogonal determinant splitting
- Orthogonal polynomial projection kernel
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- Planar rotation
- Principal minor
- Projection kernel determinant integration
- Rational conjugation of finite-index modular subgroups
- Rational representation of the general linear group
- Reduced norm
- Rotational symmetry group of a cube
- Rotation invariance of the Levi-Civita symbol
- Routh-Hurwitz stability criterion
- Row Hermite normal form in rank two
- Row lattice of an integer matrix
- Shear mapping
- Singular matrix
- SO(3) group
- Square matrix
- SU(2) matrix
- SU(4) group
- Two-dimensional Routh-Hurwitz stability criterion
- Upper triangular matrix
- Vandermonde determinant invariance under monic basis change
- Weighted Vandermonde determinant
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Name origin: likely because it "determines" if a matrix is invertible or not, as a matrix is invertible iff determinant is not zero.