"Quality of image" has a lot of parameters, including resolution, noise, systematic errors, etc. I am not aware of a global "quality of image" metric.
One other consideration, not related to your comment: imagine if we had an x-ray lens through which we could take confocal images of a protein molecule or crystal, output as a voxel array. Would we really still prefer to measure diffraction patterns rather than the equivalent real space image, even assuming we had some perfect way to solve the phase problem? Or conversely, should we try to do fluorescence imaging in diffraction mode, due to its purported information efficiency? JPK -----Original Message----- From: herman.schreu...@sanofi.com [mailto:herman.schreu...@sanofi.com] Sent: Friday, November 10, 2017 10:22 AM To: Keller, Jacob <kell...@janelia.hhmi.org>; CCP4BB@JISCMAIL.AC.UK Subject: AW: [ccp4bb] AW: Re: [ccp4bb] Basic Crystallography/Imaging Conundrum At the bottom line, it is the quality of the image, not only the amount of pixels that counts. Adding more megapixels to a digital camera with a poor lens (as some manufacturers did), did not result in any sharper or better images. Herman -----Ursprüngliche Nachricht----- Von: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] Im Auftrag von Keller, Jacob Gesendet: Freitag, 10. November 2017 15:48 An: CCP4BB@JISCMAIL.AC.UK Betreff: [EXTERNAL] Re: [ccp4bb] AW: Re: [ccp4bb] Basic Crystallography/Imaging Conundrum It seems, then, to be generally agreed that the conversion between voxels and Fourier terms was valid, each containing the same amount of information, but the problem was in the representation, and there was just trickery of the eye. I was thinking and hoping this would be so, since it allows a pretty direct comparison of crystal data to microscopic imaging data. I guess a litmus test would be to decide whether a voxel version of the electron density map would work equivalently well in crystallographic software, which I suspect it would. If so, then the same techniques--so effective in extracting information for the relatively information-poor crystal structures--could be used on fluorescence imaging data, which come in voxels. Regarding information-wealth, in Dale's example, the whole hkl set was 4.1 MB. One frame in a garden-variety XYZT fluorescence image, however, contains about 2000 x 2000 x 100 voxels at 16-bit, i.e., 400 million bits or 50 MB. In some data sets, these frames come at 10 Hz or more. I suspect that the I/sigma is also much better in the latter. So, with these data, and keeping a data:parameters ratio of ~4, one could model about 100 million parameters. This type of modelling, or any type of modelling for that matter, remains almost completely absent in the imaging world, perhaps because the data size is currently so unwieldy, perhaps also because sometimes people get nervous about model biases, perhaps also because people are still improving the imaging techniques. But just imagine what could be done with some crystallography-style modelling! Jacob Keller -----Original Message----- From: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] On Behalf Of Tristan Croll Sent: Friday, November 10, 2017 8:36 AM To: CCP4BB@JISCMAIL.AC.UK Subject: Re: [ccp4bb] AW: Re: [ccp4bb] Basic Crystallography/Imaging Conundrum Or a nice familiar 2D example: the Ramachandran plot with 7.5 degree binning, as a grid (left) or with bicubic smoothing (right). Different visualisations of the same data, but the right-hand image uses it better. On 2017-11-10 08:24, herman.schreu...@sanofi.com wrote: > In line with Dale's suggestions, I would suggest that you reformat > your voxel map into the format of an electron density map and look at > it with coot. I am sure it will look much better and much more like > the electron density we are used to look at. Alternatively, you could > display an bona fide electron density map as voxel blocks and I am > sure it will look similar to the voxel map you showed in your first > email. > > Best, > Herman > > -----Ursprüngliche Nachricht----- > Von: CCP4 bulletin board [mailto:CCP4BB@JISCMAIL.AC.UK] Im Auftrag von > Dale Tronrud > Gesendet: Freitag, 10. November 2017 08:08 > An: CCP4BB@JISCMAIL.AC.UK > Betreff: [EXTERNAL] Re: [ccp4bb] Basic Crystallography/Imaging > Conundrum > > Ethan and I apparently agree that anomalous scattering is "normal" > and Friedel's Law is just an approximation. I'll presume that your > "unique" is assuming otherwise and your 62,500 reflections only > include half of reciprocal space. The full sphere of data would > include 125,000 reflections. Since the cube root of 125,000 is 50 you > get a range of indices from -25 to +25 which would give you 2 A > resolution, which is still far from your hope of 1 A. > > For your test case of 1 A resolution with 50 A cell lengths you > want your indices to run from -50 to +50 giving a box of reflections > in reciprocal space 101 spots wide in each direction and a total of > 101^3 = > 1,030,301 reflections. (or 515,150.5 reflections for your Friedel > unique with the "half" reflection being the F000 which would then be > purely real valued.) > > Assuming you can fit your structure factors into 16 bits (You had > better not have many more than 10,000 atoms if you don't want your > F000 to overflow.) the information content will be 1,030,301 * 2 * 16 > bits (The "2" because they are complex.) giving 32,969,632 bits. > > If you spread this same amount of information across real space you > will have 1,030,301 complex density values in a 50x50x50 A space > giving a sampling rate along each axis of 101 samples/unit cell. > > Complex density values? The real part of the density is what we > call the electron density and the imaginary part we call the anomalous > density. If there is no anomalous scattering then Friedel's Law holds > and the number of unique reflections is cut in half and the density > values are purely real valued - The information content in both spaces > is cut in half and they remain equal. > > By sampling your unit cell with 101 samples their rate is half that > of the wavelength of the highest frequency reflection. (e.q. a > sampling rate of 0.5 A for 1 A resolution data) This is, of course, > the Nyquist Theorem which states that you have to sample at twice the > frequency of the highest resolution Fourier coefficient. > > This is exactly how an FFT works. It allocates the memory required > to store the structure factors and it returns the map in that same > array - The number of bytes is unchanged. It also guarantees that the > calculation is reversible as no information is lost in either > direction. > > So, why does your blocky image look so bad? First you have sampled > too coarsely. You should have twice the sampling rate in each > direction. > > The next point is more subtle. You are displaying each voxel as a > block. This is not correct. The sharp lines that occur at the > boundaries between the blocks is a high frequency feature which is not > consistent with a 1 A resolution image. Your sample points should be > displayed at discrete points since they are not the average density > within a block but the value of the density at one specific point. > > What is the density of the map between the sampled points? The > Fourier series provides all the information needed to calculate them > and you can calculate values for as fine a sampling rate as you like, > just remember that you are not adding any more information because > these new points are correlated with each other. > > If you have only the samples of a map and want to calculate Fourier > coefficients there are many sets of Fourier coefficients that will > reproduce the sampled points equally well. We specify a unique > solution in the FFT by defining that all reflections of resolution > higher than 1 A must be identically equal to zero. When you calculate > a map from a set of coefficients that only go to 1 A resolution this > is guaranteed. > > When you are calculating coefficients from any old map you had > better ensure that the map you are sampling does not contain > information of a higher resolution than twice your sampling rate. > This is a problem when calculating Fcalc from an atomic model. You > calculate a map from the model and FFT it, but you can't sample that > map at 1/2 the resolution of your interest. You must sample that map > much more finely because an atomic model implies Fourier coefficients > of very high resolution. > (Otherwise phase extension would be impossible) This problem was > discussed in detail in Lynn Ten Eyck's 1976 paper on Fcalc FFT's but > is often forgotten. Gerard Bricogne's papers on NCS averaging from > the 1970's also discusses these matters in great depth. > > In summary, your blocky picture (even with double sampling) is not > a valid representation because it is not blurry like a 1 A resolution > map should be. To create an accurate image you need to oversample the > map sufficiently to prevent the human eye from detecting aliasing > artifacts such as the straight lines visible in your blocky picture. > This requires very fine sampling because the eye is very sensitive to > straight lines. When using a map for any purpose other than FFTing > you will need to oversample the map by some amount to prevent aliasing > artifacts and the amount of oversampling will depend on what you are > doing to the map (Again, see Gerard's papers.) Such an oversampled > map will have many more voxels but no more information because the > density values are correlated. > > Dale Tronrud > > On 11/9/2017 4:10 PM, Keller, Jacob wrote: >> Dear Crystallographers, >> >> >> >> I have been considering a thought-experiment of sorts for a while, >> and wonder what you will think about it: >> >> >> >> Consider a diffraction data set which contains 62,500 unique >> reflections from a 50 x 50 x 50 Angstrom unit cell, with each >> intensity measured perfectly with 16-bit depth. (I am not sure what >> resolution this corresponds to, but it would be quite high even in >> p1, I think--probably beyond 1.0 Angstrom?). Thus, there are 62,500 x >> 16 bits (125 KB) of information in this alone, and there is an HKL >> index associated with each intensity, so that I suppose contains >> information as well. One could throw in phases at 16-bit as well, and >> get a total of 250 KB for this dataset. >> >> >> >> Now consider an parallel (equivalent?) data set, but this time >> instead of reflection intensities you have a real space voxel map of >> the same >> 50 x 50 x 50 unit cell consisting of 125,000 voxels, each of which >> has a 16-bit electron density value, and an associated xyz index >> analogous to the hkl above. That makes a total of 250 KB, with each >> voxel a 1 Angstrom cube. It seems to me this level of graininess >> would be really hard to interpret, especially for a static picture of >> a protein structure. (see attached: top is a ~1 Ang/pixel >> down-sampled version of the image below). >> >> >> >> Or, if we wanted smaller voxels still, let's say by half, we would >> have to reduce the bit depth to 2 bits. But this would still only >> yield half-Angstrom voxels, each with only four possible electron >> density values. >> >> >> >> Is this comparison apt? Off the cuff, I cannot see how a 50 x 50 >> pixel image corresponds at all to the way our maps look, especially >> at around >> 1 Ang resolution. Please, if you can shoot down the analogy, do. >> >> >> >> Assuming that it is apt, however: is this a possible way to see the >> power of all of our Bayesian modelling? Could one use our modelling >> tools on such a grainy picture and arrive at similar results? >> >> >> >> Are our data sets really this poor in information, and we just model >> the heck out of them, as perhaps evidenced by our scarily low >> data:parameters ratios? >> >> >> >> My underlying motivation in this thought experiment is to illustrate >> the richness in information (and poorness of modelling) that one >> achieves in fluorescence microscopic imaging. If crystallography is >> any measure of the power of modelling, one could really go to town on >> some of these terabyte 5D functional data sets we see around here at >> Janelia (and on YouTube). >> >> >> >> What do you think? >> >> >> >> Jacob Keller >> >> >> >> +++++++++++++++++++++++++++++++++++++++++++++++++ >> >> Jacob Pearson Keller >> >> Research Scientist / Looger Lab >> >> HHMI Janelia Research Campus >> >> 19700 Helix Dr, Ashburn, VA 20147 >> >> (571)209-4000 x3159 >> >> +++++++++++++++++++++++++++++++++++++++++++++++++ >> >> >>
