Lucky Hans wrote:
Let P be a random orthogonal projection on R^d, chosen according to the "uniform distribution" on the set of rank k orthogonal projections. Are the squares of any two distinct entries on the diagonal uncorrelated?
(It probably doesn't matter but I assume that k is at least 2 and d at least 2k.)
Any ideas?
Obviously

.
Let's do a simple calculation with d=4 and k=2, which has a reasonably nice coordinate system to work with.
The Haar measure on SO(4) is of course induced by

. So upon identifying

, we might as well take 1,i as the two orthonormal vectors, and have

where

are random unit quaternions and

is the projection to

. Now, writing

,

, we get

Switching to (spherical) polars, (and for brevity

,

, etc.)

(

,

)
So
![\begin{aligned}
P_{1,1}&=\lvert P_2(UU')\rvert^2\\
&=\lvert zz'+\bar{w}w'\rvert^2\\
&=\big\lvert (c_1+\mathrm{i}s_1c_2)(c_{1'}+\mathrm{i}s_{1'}c_{2'})+s_1s_2(c_3-\mathrm{i}s_3)s_{1'}s_{2'}(c_{3'}+\mathrm{i}s_{3'})\big\rvert^2\\
&=[c_1c_{1'}-s_1s_{1'}c_2c_{2'}+s_1s_2s_{1'}s_{2'}c_{3-3'}]^2+
[c_1s_{1'}c_{2'}+c_{1'}s_1c_2+s_1s_2s_{1'}s_{2'}s_{3-3'}]^2\\
P_{2,2}&=\lvert P_2(U\,\mathrm{i}U')\rvert^2\\
&=\lvert zz'-\bar{w}w'\rvert^2\\
&=\big\lvert (c_1+\mathrm{i}s_1c_2)(c_{1'}+\mathrm{i}s_{1'}c_{2'})-s_1s_2(c_3-\mathrm{i}s_3)s_{1'}s_{2'}(c_{3'}+\mathrm{i}s_{3'})\big\rvert^2\\
&=[c_1c_{1'}-s_1s_{1'}c_2c_{2'}-s_1s_2s_{1'}s_{2'}c_{3-3'}]^2+
[c_1s_{1'}c_{2'}+c_{1'}s_1c_2-s_1s_2s_{1'}s_{2'}s_{3-3'}]^2
\end{aligned} \begin{aligned}
P_{1,1}&=\lvert P_2(UU')\rvert^2\\
&=\lvert zz'+\bar{w}w'\rvert^2\\
&=\big\lvert (c_1+\mathrm{i}s_1c_2)(c_{1'}+\mathrm{i}s_{1'}c_{2'})+s_1s_2(c_3-\mathrm{i}s_3)s_{1'}s_{2'}(c_{3'}+\mathrm{i}s_{3'})\big\rvert^2\\
&=[c_1c_{1'}-s_1s_{1'}c_2c_{2'}+s_1s_2s_{1'}s_{2'}c_{3-3'}]^2+
[c_1s_{1'}c_{2'}+c_{1'}s_1c_2+s_1s_2s_{1'}s_{2'}s_{3-3'}]^2\\
P_{2,2}&=\lvert P_2(U\,\mathrm{i}U')\rvert^2\\
&=\lvert zz'-\bar{w}w'\rvert^2\\
&=\big\lvert (c_1+\mathrm{i}s_1c_2)(c_{1'}+\mathrm{i}s_{1'}c_{2'})-s_1s_2(c_3-\mathrm{i}s_3)s_{1'}s_{2'}(c_{3'}+\mathrm{i}s_{3'})\big\rvert^2\\
&=[c_1c_{1'}-s_1s_{1'}c_2c_{2'}-s_1s_2s_{1'}s_{2'}c_{3-3'}]^2+
[c_1s_{1'}c_{2'}+c_{1'}s_1c_2-s_1s_2s_{1'}s_{2'}s_{3-3'}]^2
\end{aligned}](/CBB/latexrender/pictures/f858059506465aac7eef2735c01ec484.png)
So now take expectations of

, and remember the (normalised) measure on

is given by

and you should see the covariance is nonzero. (You can cheat using Weyl's integration formula instead of passing to the explicit description of Spin(4).)