Rayleigh-Ritz theorem
Let be a Hermitian matrix. Then itseigenvectors
are the critical points (vectors) of the ”Rayleigh quotient”,which is the real function
and its eigenvalues are its values at such critical points.
As a consequence, we have:
and
Proof:
First of all, let’s observe that for a hermitian matrix, the number is a real one (actually, ,whence is real), so that theRayleigh quotient is real as well.
Let’s now compute the critical points of theRayleigh quotient, i.e. let’s solve the equations system . Let’s write , and beingrespectively the real and imaginary part of . We have:
so that we must have:
Using derivatives rules, we obtain:
Applying matrix calculus rules, we find:
and since ,
In a similar way, we get:
Substituting, we obtain:
and, after a transposition, equating to the null column vector
,
and, since is real,
Let’s then evaluate :
Applying again matrix calculus rules, we find:
and since ,
In a similar way, we get:
Substituting, we obtain:
and, after a transposition, equating to the null column vector,
and, since is real,
In conclusion, we have that a stationary vector forthe Rayleigh quotient satisfies the complex eigenvalue equation
whence the thesis.
Remarks:
1) The two relations and can also be obtained in a simpler way.By Schur’s canonical form theorem, any normal (and hence any hermitian)matrix is unitarily diagonalizable, i.e. a unitary matrix
exists suchthat with . So, since all eigenvalues of a hermitian matrix arereal, it’s possible to write:
whence
But, having defined , wehave:
so that
In a much similar way, we obtain
2) The above relations yield the following noteworthing bounds for thediagonal entries of a hermitian matrix:
In fact, having defined
and observing that , we have: