Eigenspaces of anticommuting endomorphisms #
Let f and g be endomorphisms of a module with f * g + g * f = 0. Then
(f + μ) g = -g (f - μ), so g carries the generalized μ-eigenspace of f into its
generalized -μ-eigenspace, for every exponent. When g = e is invertible, its inverse also
anticommutes with f, and e identifies the two generalized eigenspaces, which therefore have
equal finrank. In particular, for a finite-dimensional vector space over a field, the
eigenvalues of f come in pairs ±μ with equal geometric and algebraic multiplicities, and e
preserves every generalized eigenspace of f at 0.
The basic example is a shape operator S of a complex submanifold, which anticommutes with the
complex structure J: its principal curvatures come in pairs ±κ.
Main declarations #
Module.End.genEigenspace_neg: the generalized eigenspaces of-fare those offat the negated eigenvalue.Module.End.genEigenspace_smul: over a field, the generalized eigenspaces oft • ffort ≠ 0are those offat the rescaled eigenvalue.Module.End.mapsTo_genEigenspace_neg_of_anticommute: an endomorphism anticommuting withfmaps the generalizedμ-eigenspace offinto its generalized-μ-eigenspace.Module.End.map_genEigenspace_of_anticommute: for an invertible such endomorphism this is an equality of submodules.Module.End.genEigenspaceEquivOfAnticommute: the induced linear equivalence between the generalizedμ- and-μ-eigenspaces.Module.End.finrank_genEigenspace_neg_of_anticommute: the two generalized eigenspaces have the same dimension.Module.End.hasUnifEigenvalue_neg_iff_of_anticommute:-μis a (generalized) eigenvalue exactly whenμis.
References #
- J. Milnor, Morse Theory, Princeton University Press, 1963, Section 7.
The generalized eigenspaces of -f are the generalized eigenspaces of f at the negated
eigenvalue.
Over a field, the generalized eigenspaces of a nonzero multiple t • f are the generalized
eigenspaces of f at the eigenvalue divided by t.
An endomorphism g anticommuting with f maps the generalized μ-eigenspace of f into
its generalized -μ-eigenspace.
An invertible endomorphism e anticommuting with f maps the generalized μ-eigenspace of
f onto its generalized -μ-eigenspace.
An invertible endomorphism e anticommuting with f restricts to a linear equivalence
between the generalized μ- and -μ-eigenspaces of f.
Instances For
If an invertible endomorphism anticommutes with f, the generalized μ- and
-μ-eigenspaces of f have the same finrank. For a finite-dimensional vector space over a
field, these are the geometric multiplicities of μ and -μ when k = 1, and their algebraic
multiplicities when k = ⊤.
If an invertible endomorphism anticommutes with f, then -μ is a generalized eigenvalue
of f exactly when μ is.