Spectral properties of the LDL^T matrix factorization Assume that a square, symmetric matrix $A$ can be factored into $A=LDL^T$ where $L$ is unit lower triangular and $D$ is diagonal. For indefinite $A$, $D$ may have $2x2$ blocks on the diagonal. How much information about the spectrum of $A$ can we obtain from $D$?
For example, it is known by Sylvester's law of matrix inertia that the inertia of $D$ is the same as that of $A$ (they have the same number of positive and negative eigenvalues). This is interesting, but I am wondering what other information is hidden in $D$.
 A: Well, for the closely related Cholesky factorization, there is the following:
Fast Accurate Eigenvalue Computations Using the Cholesky Factorization (1997) (by Roy Matthias), which says that the eigenvalues are very close to the squares of the diagonal elements of the Cholesky factor. (the paper is available on CiteSeer).
A: For indefinite $2 \times 2$ Hermitian matrices, Euclidean : spherical :: LDL : spectral.
Or in plain English, Euclidean geometry is to spherical geometry as the LDL decomposition is to the spectral theorem.
Reason: An indefinite Hermitian matrix describes a circle or a line, either on a plane (with a point at infinity) or a sphere. The LDL decomposition finds the centre and radius of the circle/line when on a plane, while the spectral theorem does so when on a sphere. The LDL decomposition might fail to exist because a line (unlike a circle) doesn't have a well-defined radius or centre point, while the same complication does not affect the spectral theorem.
The circle-on-plane is obtained from the circle-on-sphere by stereographic projection. So your question boils down to, in the indefinite 2x2 Hermitian case:

*

*Given the radius of the stereographic projection of a circle from a sphere to a plane, what can we learn about the original circle on the sphere?

Some thoughts are that the following can increase the radius of the projected circle: Either moving the original circle closer to the centre of stereographic projection, or increasing its radius on the sphere.
Hopefully, that might help a bit.
A: Not an answer, but just thinking loudly (can I say like this in English?)
Consider
A=
$ a ~~ b $
$ b ~~ a $
Then eigenvalues are equal to a-b, a+b (it is easy to check since trace and determinant are correct).
Then 
L = 
$ 1~~~~~~ 0 $
$ b/a~~1 $
D= 
$ a ~~~~ 0$
$ 0 ~~~~ a - b^2/a$
(It is easy in 2x2 case since determinant(A) = $d_1d_2$ ).
So we see:
eigenvalues are:
$ a \pm b$
and elements of D are $a$ and $a-b^2/a$
Well, do they look similar ?
Stupid case when they are similar is b=0.
Another case is more interesting  - take b=a - very degenerate but will be positve under small perturbation a=b+small. 
So in this case eigs are : $2a, 0$, and elements of D are $a$ and $0$ .
So we see that the smallest number (i.e. $0$) is the same. 
Probably that is the phenomena which I heard about i.e. something similar holds true for NxN matrices. 
Probably paper mentioned in Igor's answer is something related.
