The dimension-free Davis–Kahan sin Θ theorem #
Let A and B be bounded operators on an inner product space E, let U be invariant under A
and W invariant under B, with B symmetric. If the quadratic form of A on U lies above
that of B on W with a margin g,
(c + g) ‖u‖² ≤ re ⟪A u, u⟫ for u ∈ U and re ⟪B w, w⟫ ≤ c ‖w‖² for w ∈ W,
then g ‖P_W P_U‖ ≤ ‖B - A‖. Taking W = Vᗮ for a B-invariant subspace V bounds the directed
gap ‖P_{Vᗮ} P_U‖, the operator norm of the directed sine from U towards V: for g > 0, the
A-invariant subspace U sticks out of the B-invariant subspace V by at most ‖B - A‖ / g,
as long as the part of A on U stays separated by g from the part of B on Vᗮ. With the
separation hypotheses in both orientations, the sharp gap identity
Submodule.projectionGap_eq_max turns the two directed bounds into the bound
g ‖P_U - P_V‖ ≤ ‖B - A‖ on the gap between U and V.
No completeness, finite dimension, or spectral theorem is used; the hypotheses are quadratic-form
bounds, which on invariant subspaces of symmetric operators on finite-dimensional spaces are
equivalent to spectral containment (LinearMap.IsSymmetric.pointSpectrumIn_Iic_iff,
LinearMap.IsSymmetric.pointSpectrumIn_Ici_iff). The theorem is a consequence of the separated
Sylvester bound
ContinuousLinearMap.mul_norm_le_norm_sylvester_apply_of_re_inner_le_of_le_re_inner.
Main results #
Submodule.mul_norm_starProjection_comp_starProjection_le_norm_sub: the directedsin Θboundg ‖P_W P_U‖ ≤ ‖B - A‖.Submodule.mul_directedProjectionGap_le_norm_sub: the same bound for the directed gap‖P_{Vᗮ} P_U‖between anA-invariant subspaceUand aB-invariant subspaceV.Submodule.mul_projectionGap_le_norm_sub: under the separation hypotheses in both orientations,g ‖P_U - P_V‖ ≤ ‖B - A‖.Submodule.norm_starProjection_comp_starProjection_le_norm_sub_div,Submodule.directedProjectionGap_le_norm_sub_div,Submodule.projectionGap_le_norm_sub_div: forg > 0, the same bounds in the form‖·‖ ≤ ‖B - A‖ / g.
References #
- C. Davis, W. M. Kahan, The rotation of eigenvectors by a perturbation. III, SIAM J. Numer. Anal. 7 (1970), 1–46.
- R. Bhatia, C. Davis, A. McIntosh, Perturbation of spectral subspaces and solution of linear operator equations, Linear Algebra Appl. 52/53 (1983), 45–67.
- R. Bhatia, Matrix Analysis, Graduate Texts in Mathematics 169, Springer (1997), §VII.3.
Acknowledgements #
Material in the Sylvester and sin Θ lineage was adapted from the
Spectra Formalization Project
(Adam Bornemann; Apache-2.0) at upstream revision 8dbaaf6728d1342ae16acf79fd7eef7c59b37e63.
The dimension-free directed Davis–Kahan sin Θ theorem. Let U be invariant under A
and W invariant under the symmetric operator B. If the quadratic form of A on U is at
least c + g and that of B on W is at most c, then g ‖P_W P_U‖ ≤ ‖B - A‖. For g > 0
this bounds ‖P_W P_U‖ by ‖B - A‖ / g. Neither completeness nor finite dimension is assumed.
The directed Davis–Kahan sin Θ theorem in division form: for g > 0, under the hypotheses
of mul_norm_starProjection_comp_starProjection_le_norm_sub, ‖P_W P_U‖ ≤ ‖B - A‖ / g.
The directed Davis–Kahan sin Θ theorem for the directed gap. Let U be invariant
under A and V invariant under the symmetric operator B. If the quadratic form of A on U
is at least c + g and that of B on Vᗮ is at most c, then the directed gap
‖P_{Vᗮ} P_U‖ from U to V satisfies g ‖P_{Vᗮ} P_U‖ ≤ ‖B - A‖.
The directed Davis–Kahan sin Θ theorem for the directed gap in division form: for g > 0,
under the hypotheses of mul_directedProjectionGap_le_norm_sub, the directed gap from U to V
is at most ‖B - A‖ / g.
The dimension-free Davis–Kahan sin Θ theorem for the gap. Let U be invariant under
the symmetric operator A and V invariant under the symmetric operator B. Suppose that the
quadratic form of A on U is at least c + g while that of B on Vᗮ is at most c, and
that the quadratic form of B on V is at least c' + g while that of A on Uᗮ is at
most c'. Then the gap between U and V satisfies g ‖P_U - P_V‖ ≤ ‖B - A‖.
The Davis–Kahan sin Θ theorem for the gap in division form: for g > 0, under the
hypotheses of mul_projectionGap_le_norm_sub, ‖P_U - P_V‖ ≤ ‖B - A‖ / g.