Properties of the image reconstruction filter in rendering

The function $h_j$ is going to be a low-pass filter of some type. Its role is to turn the infinite-resolution image $f$ into a band-limited one so that it can be sampled to produce pixel values without aliasing. Typical shapes for $h_j$ in practice could be like a box, tent, bicubic, or Gaussian function.

Such a filter would generally be expected to have the following properties:

• Defined over the image plane, $h_j: mathbb{R}^2 to mathbb{R}$
• Is an area density, i.e. has units of inverse area (and scales accordingly under changes of coordinates)
• Compactly supported, with its region of support commensurate with the pixel spacing (typically having a radius of 1–2 pixels in all directions)
• Smooth, or at least piecewise smooth
• Finite-valued
• Integrates to 1, $int_{mathbb{R}^2} h_j(x) , dx^2 = 1$
• The filters for different pixels $j$ differ only by translation, $h_j(x) = h(x - x_j)$ where $h$ is the filter centered at 0, and $x_j$ is the center of the $j$th pixel.
• Symmetric, $h(-x) = h(x)$
• Factors into 1D filters along the x and y axes, $h(x, y) = h(x)h(y)$

(The last three properties might not be true for some exotic cases, such as rendering to a curved or nonlinearly warped display, but would be expected to hold for rendering an ordinary 2D image.)

You'll note one property I didn't mention was $h_j geq 0$. That's because it is actually convenient to use filters with negative lobes sometimes, as they can improve image sharpness. See for example the Mitchell–Netravali filters. Nor do we necessarily have $h_j leq 1$ everywhere. Actually the values of $h_j$ depend on the coordinate system, since it's an area density, so a statement like $h_j leq 1$ is meaningless without specifying some particular coordinates.

Regarding your properties, for (a), yes the norm of the filter should be bounded. As mentioned, the filter integrates to 1. Without negative lobes, the 1-norm of the filter should be exactly 1. The 1-norm of a filter with negative lobes would be expected to be somewhat greater than 1 but still finite.

For property (b), I'm not 100% sure but I think that this is indeed guaranteed by the fact that $h_j$ is (piecewise) smooth and has a support that doesn't get arbitrarily small. The size of the filter is on the order of the pixel spacing (otherwise it doesn't work for antialiasing), so the variance within a single pixel's filter footprint can't be much more than (variance of entire image * number of pixels). You could probably formalize that with Chebyshev's inequality or some such.

I am replying to the last edit of the question.

You can show that $|h_j * f |^2_2 leq |h_j|^2_1|f|^2_2$ from Young's theorem. Provided that $|h_j|_1 leq 1$ you have: $|h_j * f |^2_2 leq |f|^2_2$. Additionally for $g_j$ I believe you want to clamp the indicator function to ${h_j > 0 wedge f > 0}$. Then $int_{{h_j>0 wedge f>0}} aleq int_{{f>0}}a$ (since the integrands are always non-negative: $ageq 0$). This basically proves that the inequality holds for the left terms of the quadratic expansions, the middle terms are both negative, so those may be ignored. The only thing left to prove is: $(frac{1}{mu({h_j>0 wedge f>0})}int h_jf)^2 leq (frac{1}{mu({f>0})}int f)^2$, which is the case if $h_j leq 1$ everywhere. Basically, as long as your filter $h_j$ preserves the minimum and maximum of the image, you're good (this is not an unreasonable requirement for a filter, note however, that there are filers that do not preserve min-max).

Edit: My bad, the middle terms may not be ignored (at least the one on the right of the inequality). Which means you are left to prove that:

$$frac{(int h_jf)^2}{mu({h_j>0 wedge f>0})} geq frac{(int f)^2}{mu({f>0})}$$, which will be a problem.

I guess one has to use tighter bounds to relate the mixed term with the squared terms.

Edit 2:

Let's consider the expression as a whole then:

$$int left(h_jf - frac{int h_jf}{mu({h_j > 0 wedge f > 0})} right)^2 leq alpha int left(f - frac{int f}{mu({f > 0})} right)^2$$ $$ 0 leq alphaint (f)^2 - int (h_jf)^2 +alphafrac{(int f)^2}{mu^2({f > 0})} - frac{(int h_jf)^2}{mu^2({h_j > 0 wedge f > 0})} + frac{2(int h_jf)^2}{mu({h_j > 0 wedge f > 0})} - alphafrac{2(int f)^2}{mu({f > 0})}$$ $$ 0 leq alphaleft(int (f)^2 - frac{(1-2mu({f > 0}))(int f)^2}{mu^2({f > 0})}right) - left( int (h_jf)^2 - frac{(1-2mu({h_j > 0 wedge f > 0}))(int h_jf)^2}{mu^2({h_j > 0 wedge f > 0})}right) $$

$$0 leq left(int(sqrt{alpha}f)^2-int (h_jf)^2right) - left(frac{alpha(1-2mu({f > 0}))(int f)^2}{mu^2({f > 0})} - frac{(1-2mu({h_j > 0 wedge f > 0}))(int h_jf)^2}{mu^2({h_j > 0 wedge f > 0})}right) $$

$$0 leq left(int(sqrt{alpha}f)^2-int (h_jf)^2right) - left(a left(int sqrt{alpha}fright)^2 - bleft(int h_jfright)^2right)$$

Note also that $left(int uright)^2 leq int u^2$. Then with an appropriate $alpha$ and $h_j$ bounded it should hold. You may want to study the $a,b$ tems also.