Empirical spectral measures of matrices #
For a Hermitian matrix A of positive size n, the empirical spectral measure
L_A = n⁻¹ ∑ᵢ δ_{λᵢ(A)} is the probability measure on ℝ putting mass 1/n at each eigenvalue,
counted with multiplicity. For a general complex square matrix, the eigenvalue measure is the
probability measure n⁻¹ ∑ δ_z on ℂ, the sum running over the roots of the characteristic
polynomial with algebraic multiplicity. These are the basic objects of random matrix theory:
global laws such as the semicircle and circular laws are limit theorems for them.
Both measures are built from TauCeti.Probability.empiricalMeasureOfFintype, whose evaluation,
integration and pushforward API applies to them directly. The Hermitian measure depends only on the
characteristic polynomial, not on the basis or on the eigenvector choice, and its pushforward along
ℝ → ℂ is the eigenvalue measure. The eigenvalue measure of a nilpotent matrix is the Dirac mass at
0; this records that roots are counted with algebraic, not geometric, multiplicity.
The spectral measure depends continuously on the Hermitian matrix for the weak topology and measurably for the entrywise measurable structure. Thus a measurable random Hermitian matrix has a measurable empirical spectral measure, including when eigenvalues collide.
The moments and the resolvent transform of the Hermitian spectral measure are normalized traces:
∫ x ^ k dL_A = n⁻¹ Re tr (A ^ k) and, off the spectrum, m_{L_A}(z) = n⁻¹ tr (A - z • 1)⁻¹.
These identities turn the moment method and the resolvent method for global laws into
computations with traces of matrices.
If A.charpoly = X ^ k * B.charpoly, the spectral measure of A is the mixture of that of B
and of the Dirac mass at 0, with weights proportional to the size of B and to k. For the
Gram matrices of a card m × card n matrix A with card m ≤ card n this is the exact
zero-mass correction L_{AᴴA} = (card m / card n) L_{AAᴴ} + (1 - card m / card n) δ₀, and with
k = card n - card m the resolvent transforms satisfy the companion identity
m_{L_{AᴴA}}(z) = (card m / card n) m_{L_{AAᴴ}}(z) - (k / card n) z⁻¹. These relate the
spectral measures of a sample covariance matrix X * Xᴴ / n and of its companion Xᴴ * X / n.
Main definitions #
Matrix.spectralMeasure A hA— the empirical spectral measure of a Hermitian matrix;Matrix.eigenvalueMeasure A— the empirical measure of the characteristic roots of a complex square matrix.
Main results #
Matrix.spectralMeasure_eq_of_charpoly_eq— Hermitian matrices with the same characteristic polynomial have the same spectral measure;Matrix.spectralMeasure_units_conj,Matrix.eigenvalueMeasure_units_conj— both measures are invariant under conjugation by an invertible matrix;Matrix.eigenvalueMeasure_apply— the eigenvalue measure of a set is the proportion of characteristic roots in it, counted with algebraic multiplicity;Matrix.map_spectralMeasure_ofReal— for a complex Hermitian matrix, the eigenvalue measure is the pushforward of the spectral measure alongℝ → ℂ;Matrix.spectralMeasure_apply_singleton_zero— the zero atom has mass equal to the normalized nullity;Matrix.charpoly_roots_filter_ne_zero_mul_eq— rectangular products have the same nonzero characteristic roots, counted with multiplicity;Matrix.gram_spectralMeasure_moments_mul_card_eq— their positive spectral moments agree after weighting by the matrix dimensions;Matrix.PosSemidef.ae_mem_Ici_spectralMeasure— the spectral measure of a positive-semidefinite matrix is concentrated on the nonnegative reals;Matrix.eigenvalueMeasure_toMeasure_of_isNilpotent— a nilpotent matrix has eigenvalue measureδ₀;Matrix.integral_pow_spectralMeasure— thek-th moment of the spectral measure is the normalized trace ofA ^ k;Matrix.resolventTransform_spectralMeasure— the resolvent transform of the spectral measure is the normalized trace of the resolvent(A - z • 1)⁻¹;Matrix.spectralMeasure_toMeasure_of_charpoly_eq_X_pow_mul,Matrix.integral_spectralMeasure_of_charpoly_eq_X_pow_mulandMatrix.resolventTransform_spectralMeasure_of_charpoly_eq_X_pow_mul— the spectral measure, its integrals and its resolvent transform whenA.charpoly = X ^ k * B.charpoly;Matrix.spectralMeasure_conjTranspose_mul_self,Matrix.spectralMeasure_mul_conjTranspose_self— the zero-mass correction between the spectral measures ofAᴴ * AandA * Aᴴ;Matrix.IsHermitian.spectralMeasure_real_Iic— the distribution function of the spectral measure is the proportion of eigenvalues at mostt.
References #
- G. W. Anderson, A. Guionnet, O. Zeitouni, An Introduction to Random Matrices, Cambridge University Press (2010), §2.1.
- T. Tao, Topics in Random Matrix Theory, American Mathematical Society (2012), §2.4.
The empirical spectral measure L_A = (card n)⁻¹ ∑ᵢ δ_{λᵢ(A)} of a Hermitian matrix of
positive size, with the eigenvalues counted with multiplicity.
Instances For
The spectral measure is the empirical measure of the eigenvalue family.
The spectral measure is the empirical measure of the decreasingly sorted eigenvalues.
The empirical spectral measure depends continuously on the Hermitian matrix for the weak topology on probability measures.
The empirical spectral measure is measurable for the entrywise Borel structure on Hermitian matrices and the evaluation σ-algebra on probability measures.
The spectral measure of a set is the proportion of eigenvalues in it, counted with multiplicity.
The distribution function of the spectral measure at t is the proportion of eigenvalues at
most t, counted with multiplicity.
The spectral measure's atom at zero is the proportion of zero eigenvalues, expressed in terms of the matrix rank.
The spectral measure of a positive-semidefinite matrix is concentrated on the nonnegative reals.
Integrating against the spectral measure is averaging over the eigenvalues.
Integrating against the spectral measure is averaging over the decreasingly sorted eigenvalues.
Hermitian matrices with the same characteristic polynomial have the same spectral measure. In particular the spectral measure does not depend on a choice of basis.
Conjugating a Hermitian matrix by an invertible matrix does not change its spectral measure, provided the conjugate is again Hermitian.
The Lebesgue integral against the spectral measure is the average over the eigenvalues.
The empirical measure (card n)⁻¹ ∑ δ_z of a complex square matrix of positive size, the
sum running over the roots z of its characteristic polynomial with algebraic multiplicity.
Instances For
The eigenvalue measure is the empirical measure of the family of characteristic roots, indexed by the elements of the root multiset.
The measure underlying the eigenvalue measure is the normalized sum of the Dirac masses at the characteristic roots, counted with algebraic multiplicity.
The eigenvalue measure of a set is the proportion of characteristic roots in it, counted with algebraic multiplicity.
Integrating against the eigenvalue measure is averaging over the characteristic roots, counted with algebraic multiplicity.
Conjugating a complex square matrix by an invertible matrix does not change its eigenvalue measure.
For a complex Hermitian matrix, the eigenvalue measure is the pushforward of the spectral
measure along ℝ → ℂ.
A nilpotent complex matrix of positive size has eigenvalue measure δ₀: its characteristic
polynomial is X ^ n, whose root 0 has algebraic multiplicity n.
The k-th moment of the spectral measure of a Hermitian matrix is the normalized trace of
A ^ k: ∫ x ^ k dL_A = (card n)⁻¹ * Re tr (A ^ k).
The positive moments of the two Gram-matrix spectral measures agree after weighting by the
dimensions of their respective matrices, over any RCLike field and finite nonempty index types.
Off the spectrum, the resolvent transform m(z) = ∫ (x - z)⁻¹ dL_A(x) of the spectral measure
of a complex Hermitian matrix is the normalized trace of its resolvent (A - z • 1)⁻¹.
If the characteristic polynomial of a Hermitian matrix A of size card n is X ^ k times
that of a Hermitian matrix B of size card m, then L_A is the mixture of L_B and of the
Dirac mass at 0, with weights card m / card n and k / card n.
If the characteristic polynomial of a Hermitian matrix A of size card n is X ^ k times
that of a Hermitian matrix B of size card m, then integrating against L_A is the weighted
average of integrating against L_B and evaluating at 0, with weights card m / card n and
k / card n.
If the characteristic polynomial of a complex Hermitian matrix A of size card n is X ^ k
times that of a complex Hermitian matrix B of size card m, then the resolvent transforms of
their spectral measures satisfy
m_{L_A}(z) = (card m / card n) m_{L_B}(z) - (k / card n) z⁻¹.
For a matrix A with card m ≤ card n rows and columns, the spectral measure of the
card n × card n Gram matrix Aᴴ * A is that of A * Aᴴ with the missing mass at 0:
L_{AᴴA} = (card m / card n) L_{AAᴴ} + (1 - card m / card n) δ₀.
For a matrix A with card m ≥ card n rows and columns, the spectral measure of the
card m × card m Gram matrix A * Aᴴ is that of Aᴴ * A with the missing mass at 0:
L_{AAᴴ} = (card n / card m) L_{AᴴA} + (1 - card n / card m) δ₀.