The Magic Kernel
johncostella.com
johncostella.com
Happy to answer questions or address criticisms.
The trendiest thing lately is image supersizing using neural networks. That must use far more processing power than your approach. Is this overkill? A different approach for a different use.
Randomly Googled link, in case anyone is curious: https://openaccess.thecvf.com/content_cvpr_2017_workshops/w1...
Yes, I have seen other methods for guessing or dropping in extra detail. (Indeed, my old "UnBlur" method of deblurring effectively makes a best guess as to what an image looked like before it was blurred, which in the presence of noise is always a selection of one particular possible solution.) There's nothing wrong with that — it's just a different operation.
Also, I'm not sure if I agree with this claim regarding partition of unity:
> This remarkable property, that prevents “beat” artifacts across a resized image, is not shared by any other practical kernel that I am aware of ...
Lanczos is surely a weird filter having many less than desirable properties, but IIRC cubic polynomial filters like Mitchell-Netravali and Catmull-Rom satisfies partition of unity, and both of them are popular in today's image processing. Even the bilinear filter, which can be box or triangle filter depending on whether one is minifying or magnifying, satisfies the partition of unity property. Did I get something wrong?
Edit: the bilinear filter actually does not satisfy partition of unity because it's scaled down, but a properly scaled box filter or triangle filter satisfies partition of unity.
[1] http://bigwww.epfl.ch/publications/blu9903.pdf [2] http://hhoppe.com/proj/filtering/
Yes, the "beat" statement survives from a much earlier version of the page, and is not quite right. I'll fix that.
Well, the observation in the paper
> the rectangular window function can itself be thought of as the nearest neighbor kernel, with Fourier transform sinc f; and the convolution of the rectangular window function with itself—the "tent" function—is simply the linear interpolation kernel, with Fourier transform sinc² f. The first of these has discontinuities at its endpoints, and significant spectral energy outside the first Nyquist zone. The second is continuous everywhere, and has significantly less spectral energy outside the first Nyquist zone, but it still has discontinuous first derivative at its endpoints and midpoint. The third kernel in this fundamental sequence, the Magic Kernel, is continuous and has continuous first derivative everywhere, and has even less spectral energy outside the first Nyquist zone.
corresponds quite precisely to the construction of the uniform cardinal B-splines by repeated convolution of a boxcar filter. The "succession of kernels, each obtained by convolving rect x with itself the corresponding number of times" that Costella describes in his paper is quite precisely the uniform cardinal B-splines. (The terminology around B-splines is unfortunately very confused, with different authors using "spline", "B-spline", and "cardinal B-spline" with different meanings, so I'm doing the best I can here.)
This is also an efficient way to implement the Magic Filter in practice if addition is cheaper than multiplication:
>>> x = [0, 0, 0, 1, 0, 0, 0, 0, 2, 0, 0, 0, 3, 0, 0, 0, 0, 0]
>>> for i in range(len(x)-3): x[i+2] += x[i+3]; x[i+1] += x[i+2]; x[i] += x[i+1]
...
>>> x
[1, 3, 3, 1, 0, 2, 6, 6, 2, 3, 9, 9, 3, 0, 0, 0, 0, 0]
You can see that the sequence has been convolved with the Magic Kernel. Each of the addition operations computes the two-sample boxcar filter on a sequence of input samples, and the resulting sequence is pipelined to the following addition operator, so the final sequence you get is the desired convolution.If you want to do this at a different scale, what you have is a Hogenauer filter or CIC filter, which requires an addition and a subtraction per sample per order, six in this case. Commonly they use a FIR sharpening filter, though usually just in direct form.
The multidimensional splines you get by doing this kind of interpolation successively in more than one dimension are commonly called "box splines", because you get them by convolving "boxes" instead of the one-dimensional boxcar function. This is the normal way to do Gaussian blur in image processing, for example.
If you want to use B-splines of a given degree to approximate ideal interpolation with a sinc kernel as closely as possible with a given support, avoiding any blurring, that's a solvable problem; https://www.cs.tut.fi/~gotchev/DIPII/lecture3.pdf is a set of lecture notes on the topic.
If you're interested in this kind of thing you might enjoy my notes from a couple years ago: https://dercuano.github.io/notes/sparse-kernel-cascade-gabor... https://nbviewer.jupyter.org/url/canonical.org/~kragen/sw/de... https://dercuano.github.io/topics/sparse-filters.html.
[0]: I tried again but without forcing HTTPS to confirm the issue after seeing that you're around in the comments. The content is great, but I know I'm far from the only one who defaults to ignoring sites without HTTPS.
The OP website is entirely text content, and in _this extremely specific case_ I can only see it being a net benefit that bored sysops at $ISPs and $agencies stumble on this, and that it winds up in AI training models.
If there was a point to my fist-waving it would be that there's no such thing as knee-jerk assurance when it comes to security. Yes, HTTPS is a good sane default in probably 99% of situations, but that's because the distribution of privacy-requiring contexts on the Web such as shopping and banking is disproportionate to the average.
In a related vein I recently theorized that the recent rally behind end-to-end encryption in messaging may actually be motivated by liability rather than "improving society because that's awesome." https://news.ycombinator.com/item?id=25522220
Granted, the site was interesting enough that I clicked around until I made my way back to the article you were linking to in the first place, but the link itself at least failed to fulfill its purpose :P
Just paste the address in your address bar !
That's valid, and just as valid as users (especially in technical circles!) saying "I won't visit HTTP-only sites".
Hence why I didn't frame my request as "the site sucks because it has no HTTPS" but just "I (and others) simply wouldn't visit the site". I'm just trying to spread awareness, no more.
(The rest of those objections boil down to "I don't use HTTPS hence this QA point is irrelevant").
Edit: Thank you for the site though, the weekly digest is absolutely hilarious :D
But isn't that often false, since in many places there are few choices of which ISP connects your home? Am I supposed to just move somewhere else?
Starting with http://www.johncostella.com/magic/small.png when doubling 3 times I get this result in Photoshop CS2 https://i.ibb.co/9tCLPGS/PSCS2triple.png and when doubling 3 times in GIMP’s cubic the result is https://i.ibb.co/p2b0Trq/GIMPtriple.png
This is the result when using GIMP to go straight from 57x43 to 456x344: https://i.ibb.co/r0SXVY2/GIMpstraight.png and Photoshop CS2: https://i.ibb.co/Sn1xt3Y/PSCS2straight.png
Which one is the correct representative of the bicubic filter?
The Lanczos images in the paper should be correct.
The Sharp+ is just extra sharpening. It's included in the executable, but isn't fundamentally anything more than extra sharpening over what tries to be as-close-to-ideal resizing as possible.
There is an article [0] that points this out, although later it goes into recommending odd filters, which insidiously break many applications where you would want to use downscaling by shifting the image by a fraction of a pixel.
[0] https://cbloomrants.blogspot.com/2011/03/03-24-11-image-filt...
I recommend you check out the paper http://johncostella.com/magic/mks.pdf for developments since the original 2006 "magic" kernel. :)
Fourier properties
of the Magic Kernel Sharp algorithm, and discovered that it possesses high-order zeros at multiples of the sampling frequency, which explains why it produces such amazingly clear results: these high-order zeros greatly suppress any potential aliasing artifacts that might otherwise appear at low frequencies..."
[...]
>"Following that work, I analytically derived the
Fourier transform
of the Magic Kernel in closed form, and found, incredulously, that
it is simply the cube of the sinc function.
This implies that the Magic Kernel is just the
rectangular window function convolved with itself twice
-which, in retrospect, is completely obvious. This observation, together with a precise definition of the requirement of the Sharp kernel, allowed me to obtain an analytical expression for the exact Sharp kernel, and hence also for the exact Magic Kernel Sharp kernel, which I recognized is just the third in a sequence of fundamental resizing kernels. These findings allowed me to explicitly show why Magic Kernel Sharp is superior to any of the Lanczos kernels. It also allowed me to derive further members of this fundamental sequence of kernels, in particular the sixth member, which has the same computational efficiency as Lanczos-3, but has far superior properties."
Paper: http://www.johncostella.com/magic/mks.pdf
PDS: My thoughts: Absolutely fascinating! (Also, that the the "Magic Kernel is just the rectangular window function convolved with itself twice" -- was not obvious to me, so it's good you included that!)
I also realized while writing it that the original doubling "magic" kernel (the 1/4, 3/4) was just the linear interpolation kernel for a factor of 2 with "tiled" positions, which I added to the page after writing the paper. I have since seen that others had previously made that comment (which I missed, but they are completely right). It's interesting that the infinitely repeated application of this "second" order kernel, i.e. what I now call m_2(x), originally led me (i.e. in 2011) to the "next" one, i.e. m_3(x). I still haven't fully sorted through how that works, but it's lucky that it did.
I'm always curious when/where/how we see Fourier Transforms of any sort -- because we see them in so many diverse fields, and in so much diverse Mathematics to consider them almost ubiquitous and fundamental for any meaningful understanding in many areas of Physics...
Here we see them in Image Processing...
Again, an absolutely brilliant work!
> Computationally, however, nothing short of Fast Fourier Transforms or hardware acceleration can make a large blurring job efficient: for large values of blur, the support of any blur kernel is large, and not practical for some at-scale applications.
The standard way to do Gaussian blur is to approximate it as a B-spline, specifically a cascade of simple moving average filters, also known as a Hogenauer filter or CIC filter in the time domain. Typically a cascade of three filters is used, precisely as Costella describes. This is both simpler and faster than doing the task with a Fourier transform, and moreover it is an online algorithm — it produces output samples at some processing lag behind the input samples.
As you can easily verify, the following program uses this approach to convolve its input buffer with a Gaussian kernel with support of 766 samples, constructed in just the way Costella describes (as a B-spline), in a single pass over the input buffer, with only six additions and subtractions per sample, not counting the additions and subtractions used for addressing.
#include <stdio.h>
enum {lag = 256, image_size = 4096};
unsigned long buf[image_size] = {0};
int
main(int argc, char **argv)
{
buf[image_size/2] = 1;
for (size_t i = 0; i < image_size - 3 * lag - 3; i++) {
buf[i + 3 * lag + 2] += buf[i + 3 * lag + 1];
buf[i + 3 * lag + 1] += buf[i + 3 * lag];
buf[i + 3 * lag] += buf[i + 3 * lag - 1];
buf[i + 2 * lag] -= buf[i + 3 * lag];
buf[i + lag] -= buf[i + 2 * lag];
buf[i] = buf[i + lag] - buf[i];
}
for (size_t i = 0; i < image_size - 3 * lag - 3; i++) {
if (i) printf((i%8) ? ", " : ",\n");
printf("%6ld", buf[i]);
}
printf("\n");
return 0;
}
Removing the printf calls, this takes about 162'677 instruction executions to run, according to Valgrind, which is 39 instructions per pixel. But most of that is still startup and shutdown; increasing the image size by another 4096 increases the number to 232'309 instructions, only 69632 more instructions, or 17 instructions per sample. (printf takes almost two orders of magnitude more time than the blur call.)Adding an outer loop reveals that on my nine-year-old laptop it takes 6.5 μs to run over the whole buffer, or 1.6 nanoseconds per sample. In theory this performance does not depend on the lag and thus the blur radius, but I've only tested a single lag.
The output samples are in some sense scaled by 2²⁴ = 16777216, or by 2¹⁶ = 65536 if you're interpolating a signal that's being upsampled by zero insertion by a factor of 256. This scale factor does depend on the lag (it is the cube of the lag).
This version computes the results in place starting from output that is already in memory, but you can also use a ring buffer with a capacity of at least 3lag + 2 = 770 samples. If you're downsampling, an alternative is to decimate the samples as soon as they've passed through the cascade of three integrators at the top of the loop, thus reducing both the amount of memory needed and the number of operations to do.
Overflow of intermediate results can happen, but it is not a problem as long as the final output is within range, because exact integer addition mod k is a group. If you were doing this in floating point, you might prefer to interleave the integrators with the comb filters to prevent intermediate overflow and consequent loss of precision leading to numerical instability.
Only the parts of the result buffer over which all six pipeline stages have passed contain valid results. The simplest solution to this is padding, but you can also use special logic to run the integrators but not the combs over the beginning of the input.
I would argue that 17 instructions or 1.6 nanoseconds per sample is always "efficient" and "practical" for nearly all "at-scale applications". If you were blurring a 3840×2160 display at 120 fps, one gigapixel per second, it would take 13 milliseconds of my laptop CPU cores per second for each of the R, the G, and the B; you could do it on about 6 cores of a modern CPU, without a GPU.
GCC unrolled the loop twice, so it was 34 instructions that processed two samples per iteration. The instructions are mostly things like this:
addq (%rax), %rbp
subq %rdi, %rcx
addq %rbx, %rdi
subq %rcx, %rdx
movq %rcx, -2064(%rax)
movq -2056(%rax), %rcx
That should clarify a bit how one core of my mere 2.8GHz Core i7 is managing to run over ten billion instructions per second.Godbolt link for those who want to play: https://godbolt.org/z/MfEqYn3Pd
Gaussian blur gets used for this a lot precisely because it's so easy to compute this way — it's the only convolution kernel that's anisotropic and separable. So people press it into service doing things like camera bokeh that it's not really very good at.
But in fact what I described above is the Magic Blur algorithm, just in a slightly different guise, and it can probably take advantage of existing hardware libraries in the same way. However, I don't know what your hardware libraries are doing in the blur case!