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In article <FAEBJHPJNNGCAGDNGLNPMEIOEIAA.gsellani@accesscom.com>, gary <gsellani@accesscom.com> writes >I have to disagree with you on the first count (sampling). Think about this >a bit more before you reply. Input aliasing should not be part of the >discussion. Period. I am focusing (heh heh) on the sample "width", which >leads to the pixel width. > I didn't mention input aliasing in my response because I agree it is not relevant to the analogy you made, however the finite pixel size (or width as you now term it) certainly *IS* equivalent to the pre-filter in the analogue domain of the audio analogy - as is the MTF of the optical system and, in the case of scanners, the MTF of the film and the original camera optics. This is easiest to visualise when you realise that the pixels perform more than just the sampling function. The output of an array of identical pixels is physically and mathematically exactly the same as the output produced by first scanning (convolving) the image with a single pixel of the same shape and size (point spread function) as those in the array and then multiplying the resulting analogue signal map with an array of delta functions (ideal sampling). In spatial frequency terms this is the same thing as multiplying the spatial spectrum of the image with the spatial frequency response of the pixel (ie. its MTF, the fourier transform of the point spread function of the pixel) and then convolving the result with an array of delta functions at a pitch equal to the spatial sampling frequency. In other words the array of identical finite extent pixels is exactly the same as scanning a single pixel and an array of infinitely fine samples. Visualised in this way it is *obvious* that the pixel MTF is prefilter of an ideal 2 dimensional sampling function. This is EXACTLY the same as the one dimensional audio case, where the signal is first filtered and the sample is (to all intents and purposes) instant. The audio filter applied to the audio spectrum is mathematically EXACTLY the same as a time convolution of the audio waveform with a function of a certain shape and time extent - just the FT of the frequency response of the filter. Consequently, the output of each pixel in the array CAN be considered to be an infinitely fine sample - it is the output produced by placing the pixel in EXACTLY that spatial position. A nanometer left or right produces a different output, just the same as introducing sampling lead or lag on the audio waveform would. Before anyone asks the obvious question of where, within the extended pixel area, these infinitely fine samples occur - it is irrelevant. Since the pre-filter of the imaging system is intimately tied to the sampling process, changing the exact theoretical point of sampling is balanced by an equal and opposing change in the phase of the filter. This is just the same as changing the sampling time on an audio waveform, while simultaneously changing the phase of the pre-filter to perfectly compensate. Thus an array of extended pixels with the actual sample points being considered in the top left corner of each pixel is mathematically exactly equivalent to an array of identical pixels with the sampling points in their centres - the phase change in the delta functions is matched by an equal and opposite change in the phase of the spatial filter. Incidentally, should anyone question the value of this apparently academic exercise in imaging analysis, it is by separating the visualisation of the sampling and filtering function of the detector array that leads to the conclusion, so aptly exploited by Fuji (and others in different fields), that a pixel shape other than the conventional rectangle yields better image resolution, and that this can be sampled more accurately by matching the sampling density (pixel positions) to the information content of the resulting filtered image spectrum. That is why a SuperCCD camera from Fuji actually needs much more than the same number of pixels on a conventional display to reproduce all of the information that the camera resolves. > Now it is true that imaging does not have a >pre-filter, but so what. Dogs have tails, but this is not relevant either. Not at all, imaging DOES have a prefilter - usually at least two (and several more if the image reconstruction from the sampled data is considered): 1. The optical system (which I have ignored in the discussion above, but which IS band limited, although not in a brick wall form), and 2. The pixel size and shape in terms of its electro-optic response (few devices have a flat response across the active pixel area, although they can be approximated as such), both of which alter the MTF of the sensor itself. The most significant differences between the audio analogy and the imaging case are: 1. In audio the analogue prefilter is single sided since the analogue circuits can only respond to their input after it has been received, whilst in the imaging case all of the samples occur simultaneously and the filter is nominally symmetric about the spatial frequency axis in all orientations. Of course, if the optical system includes certain distortions, such as coma, then the implied filter becomes slightly asymmetric also. In modern high performance audio systems the asymmetric filter is replaced by oversampling and application of a symmetric FIR digital filter, making it even more similar to the imaging case in this respect. 2. Being completely separate functions in the audio analogy, the filter can be tailored to meet the constraints of the sampling system, with a brick wall filter. In imaging this is not so easy to implement, although it is possible, and the filter is normally determined by the constraints of the optical MTF and the shape and size of the pixel itself. -- Kennedy Yes, Socrates himself is particularly missed; A lovely little thinker, but a bugger when he's pissed. Python Philosophers - Turn off HTML mail features. Keep quoted material short. Use accurate subject lines. http://www.leben.com/lists for list instructions.
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