The infimum of the Rayleigh quotient of a continuous linear operator T over nonzero
vectors. For self-adjoint T, this is the lower endpoint of spectrum ℝ T.
Instances For
The supremum of the Rayleigh quotient of a continuous linear operator T over nonzero
vectors. For self-adjoint T, this is the upper endpoint of spectrum ℝ T.
Instances For
For a self-adjoint operator T, ⟨(t·I − T)x, x⟩ equals the real number
t‖x‖² − ⟨Tx,x⟩_ℝ cast into ℂ.
The Rayleigh quotient is bounded above by ‖T‖, so its range over nonzero vectors
admits a supremum.
The Rayleigh quotient is bounded below by −‖T‖, so its range over nonzero vectors
admits an infimum.
Pointwise bound: Re⟨Tx, x⟩ ≤ rayleighSup T · ‖x‖².
Pointwise bound: rayleighInf T · ‖x‖² ≤ Re⟨Tx, x⟩.
Spectral inclusion for self-adjoint operators: spectrum ℝ T ⊆ [rayleighInf T, rayleighSup T].
This is one direction of the Rayleigh quotient characterization of the spectrum
(Melrose Prop 16.2).
Quadratic expansion of ⟨P(x + tPx), x + tPx⟩ for positive P: expressed in t as a
quadratic polynomial whose coefficients are Re⟨Px,x⟩, 2‖Px‖² and Re⟨P²x, Px⟩.
For a positive operator P, the Cauchy-Schwarz-type bound ‖Px‖² ≤ ‖P‖ · Re⟨Px, x⟩.
This is the key inequality used to show that rayleighInf lies in the spectrum.
The infimum of the Rayleigh quotient of a self-adjoint operator on a nontrivial complex Hilbert space belongs to its real spectrum (Melrose Prop 16.2 / 16.3).
Negation symmetry: rayleighInf (-T) = -rayleighSup T.
The supremum of the Rayleigh quotient of a self-adjoint operator on a nontrivial complex Hilbert space belongs to its real spectrum, obtained from the infimum statement via negation.
Full Rayleigh quotient characterization (Melrose Prop 16.1–16.3): for a self-adjoint
operator T on a nontrivial complex Hilbert space, both rayleighInf T and rayleighSup T
lie in spectrum ℝ T, and spectrum ℝ T is contained in [rayleighInf T, rayleighSup T].