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Computed dichotomy constants for a Jordan block and for a diagonal sink-source
Example
Use zero-based coordinates and the standard vectors and of .
- A non-diagonalisable Jordan block. For
the exponential series gives ; the only eigenvalue is , so the dichotomy theorem has , , and the constants , are admissible: for every and ,
- A diagonal sink-source. For the vectors are eigenvectors with eigenvalues and , which have nonzero real part, and the dichotomy theorem gives , with admissible constants , : for one has and , and for one has .
Facts & Assumptions
Given: The matrices and , and the Euclidean norm on (The Euclidean inner product on ).
Euclidean is complete ( and for with the Euclidean metric are complete, componentwise from the Cauchy criterion in ), and a finite matrix is bounded: Cauchy-Schwarz row by row gives (Cauchy-Schwarz with its equality case, the triangle inequality for , the parallelogram law and polarisation). For the exponential series defines with and for all real (The exponential series of a bounded operator, Rectangular matrix multiplication and the identity matrix , including zero-sized shapes).
For a fixed matrix the initial value problem , has a unique solution on every compact interval containing , so a differentiable matrix curve satisfying these two conditions on equals : apply uniqueness on for arbitrary (Linear matrix ODEs have unique global solutions on a fixed interval).
The dichotomy theorem gives -invariant subspaces with and constants , such that clauses 1-3 of the theorem hold, and , , whenever no eigenvalue of its complexification has real part (Exponential dichotomy for a hyperbolic endomorphism: invariant stable and unstable subspaces with exponential estimates); is the complex-linear extension of (Complexification as with its canonical real-linear embedding, Complexification of a real-linear map), represented by the same matrix on in the standard coordinate identification (the dichotomy theorem, Fact F1); is its eigenvalue when for some (Eigenvalues, eigenvectors, eigenspaces , and the spectrum of an endomorphism).
Scalar exponential: , and for all real ; as and as ; (The exponential addition formula , The exponential is positive and satisfies , for every real , hence , The exponential tends to at and to at , The exponential function is smooth and ).
A continuous real function on an interval that is differentiable in its interior and has nonpositive derivative is nonincreasing (On an interval , for continuous on and differentiable at every interior point: throughout gives nondecreasing, gives increasing, and give the two decreasing forms; conversely a nondecreasing has and a nonincreasing has wherever it is differentiable, and no strict converse is claimed).
Verification
Write with , so that and commutes with . Define ; differentiating entrywise with the product rule and [L4] gives and ; since , [L2] gives for all .
For define ; differentiating entrywise gives and , so [L2] gives ; in particular and . No eigenvalue of is purely imaginary: if with and , the two coordinates give and , so forces while forces . Hence [L3] applies to .
The only eigenvalue of is : if with and , the second coordinate gives and the first gives . If then and ; if then from the second coordinate. So no eigenvalue of has real part , and applies to .
Norm estimate for : put , so by step 1.1. For the product rule gives because , equivalently . Hence , and the derivative sign criterion [L5] gives for . Taking nonnegative square roots yields for all and , including . Thus , are admissible constants for in the sense of [L3].
Identification of the subspaces for : the estimate of step 2.2 holds for every , so as for every (by from [L4]); by the characterisation in [L3] the stable subspace is , and since we get .
Subspaces and constants for : for step 1.2 gives ; from the limits in [L4], as this tends to exactly when , and as exactly when . By [L3], and . With the estimates hold: for , and ; for , . Each follows from whenever , which is a consequence of and for [L4]. Hence , are admissible constants for . This proves the computed constants.
Remarks
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The first matrix shows that the dichotomy does not require diagonalisability: the explicit shear has a polynomial factor in its entries, while the symmetric-part estimate in step 2.2 proves the Euclidean bound with , . The constant is not claimed to be for every admissible rate: the computation is a finite check for the displayed rates, not a general bound.
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In both examples the admissible rates are strictly below the spectral gap, and the conclusion of [L3] is realized with ; no claim is made about optimal constants or about the converse direction of the theorem.
Depends on
Complexification as with its canonical real-linear embedding
Complexification of a real-linear map
and for with the Euclidean metric are complete, componentwise from the Cauchy criterion in
On an interval , for continuous on and differentiable at every interior point: throughout gives nondecreasing, gives increasing, and give the two decreasing forms; conversely a nondecreasing has and a nonincreasing has wherever it is differentiable, and no strict converse is claimed
Exponential dichotomy for a hyperbolic endomorphism: invariant stable and unstable subspaces with exponential estimates
The exponential series of a bounded operator
Linear matrix ODEs have unique global solutions on a fixed interval
Eigenvalues, eigenvectors, eigenspaces , and the spectrum of an endomorphism
The Euclidean inner product on
Rectangular matrix multiplication and the identity matrix , including zero-sized shapes
Cauchy-Schwarz with its equality case, the triangle inequality for , the parallelogram law and polarisation
The exponential addition formula
The exponential is positive and satisfies
for every real , hence
The exponential tends to at and to at
The exponential function is smooth and
Dependency tree · 2 levels
Sources
- G. Teschl, Ordinary Differential Equations and Dynamical Systems (AMS Graduate Studies in Mathematics 140, online edition), Section 9.1, Theorem 9.2 and formula (9.4): exponential dichotomy estimates with the polynomial factor for a Jordan block
- F. Ramponi, Notes on Lyapunov's theorem, Section 3 (the Lyapunov equation solved by the integral of e^{A^T t} e^{A t})