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Ranks of shifted powers determine Jordan form up to block order

Statement

Let T have split characteristic polynomial. For each eigenvalue λ, put ρk(λ)=rank(TλI)k(k0). Then for every k1, the number of Jordan blocks for λ of size exactly k is ρk1(λ)2ρk(λ)+ρk+1(λ). Consequently the ranks of all shifted powers determine the Jordan form uniquely up to permutation of its blocks. On the zero space the rank data and block multiset are empty.

Facts & Assumptions

Given: A finite-dimensional endomorphism T whose characteristic polynomial splits.

[L1]

The space is the direct sum of generalised eigenspaces Gμ, and Nμ=(TμI)Gμ is nilpotent (Split characteristic polynomials decompose into generalised eigenspaces of the algebraic multiplicities).

[L2]

For a nilpotent operator, rankNk12rankNk+rankNk+1 is the number of blocks of size exactly k (Power ranks determine every nilpotent Jordan-block multiplicity).

[L3]

Proof

technique · direct
1.1

Fix an eigenvalue λ. On Gλ, TλI=Nλ. On Gμ with μλ, it is (μλ)I+Nμ, which is invertible because the finite geometric series in Nμ/(μλ) is an inverse up to the nonzero scalar μλ.

L1algebra
2.1

By the direct sum in [L1] and uniqueness in [L4], for every k0 the rank on the non-λ summands is their constant total dimension cλ, while the rank on Gλ is rankNλk; hence ρk(λ)=cλ+rankNλk.

step 1.1L1L3L4
3.1

The constant cλ cancels from the second difference, and [L2] then gives the displayed exact-size block count. Varying k and λ recovers the entire block multiset.

step 2.1L2algebra
4.1

By the definition of Jordan form, a block multiset determines the block diagonal matrix up to block order; for V=0 there are no eigenvalues or blocks.

step 3.1L1

Depends on

Used by

Dependency tree · next 3 levels

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Sources