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The ultimate way of using CCDs to achieve the highest polarimetric accuracy for a single star is to consider a design whereby the source is isolated in the telescope focal plane, and then the radiation passed through the modulator and an imaging system so that the telescope aperture is focussed on the chip This has the advantage of the illuminated patch being xed, even if there is image movement in the telescope focal plane A further advantage of the system is that any patchy polarizing effects of the telescope mirrors contributing to the instrumental polarization can be explored by observing standard unpolarized stars and, in the subsequent data reductions, applying appropriate corrections to each pixel within the perture image A prototype aperture imaging polarimeter of this kind was tested by Clarke & Naghizadeh-Khouei (1997) By using a Savart plate, the instrument was designed to produce two images of the telescope aperture on the same CCD chip Switching the orthogonally resolved polarizations was achieved by a rotatable half-wave plate For each stellar polarimetric measurement some 3000 pixels were used, and nal accuracies in NSPs of 00001 were readily achieved An example of measurements of a standard unpolarized star is shown in Figure 83 When the data are grouped together in zones across the image of the aperture, mean values of the measurements clearly indicated that the telescope mirror introduced small amounts of polarization with the outer annuli being the most affected in this way Also in Figure 83, a histogram of the p / values is depicted relative to the Rice distribution for p o D 0; the small disparity of the data relative to the theoretical distribution curve relates to a mirror-induced polarization Another novel approach to spatial imaging for recording stellar polarizations is by a method pioneered by Treanor (1968) Using a very simple arrangement, he.

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where de nes the angular position around the annulus The principle was applied to star elds with many stars being recorded simultaneously on a single photographic plate The technique appeared to have been abandoned because of the poor quantum ef ciency of emulsion photography, and other problems associated with calibrations and data reduction procedures With the advent of CCD detectors, Treanor s idea has been reconsidered by Clarke & Neumayer (2002) and a system has been developed by Steele, Bates, Carter, et al (2006) for use on an automated telescope for immediate optical follow up of gamma-ray burster events As well as undertaking polarimetry of stellar elds, the technique can be applied to individual stars Using a large number of pixels near to full well capacity, a very large number of photons can be accumulated to achieve high accuracy for the measured value The modulator may be simply a rotating tilted disc of high quality sheet polarizer A rotating Rochon prism with its weak spectral dispersion, might also be used to provide high accuracy, low spectral resolution spectropolarimetry, the annuli having a radial spread according to wavelength Oliva (1997) has designed a specially constructed wedged double Wollaston prism For the simple case of recording the polarization of star elds, by using the appropriate optics, it can be placed at the image of the telescope aperture By re-imaging the eld on a CCD chip, four images are produced simultaneously corresponding to the polarization directions 0 , 90 , 45 and 135 , from which both q and u can be determined Thus all the linear polarization characteristics can be measured from a single CCD frame By placing it at a pupil image within a spectrometer, single frame spectropolarimetry may also be undertaken.

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The personal best position is excluded from the velocity equation, since a hill-climbing procedure is followed where a particle s position is only updated if the new position results in mproved performance Let the tuple (w, c1 , c2 ) represent the values of the inertia weight, w, and acceleration coe cients c1 and c2 Particles that nd themselves in phase 1 exhibit an attraction towards the global best position, which is achieved by setting (w, c1 , c2 ) = (1, 1, 1) Particles in phase 2 have (w, c1 , c2 ) = (1, 1, 1), forcing them to move away from the global best position Sub-swarms switch phases either when the number of iterations in the current phase exceeds a user speci ed threshold, or when particles in any phase show no improvement in tness during a userspeci ed number of consecutive iterations In addition to the velocity update as given in equation (1676), velocity vectors are periodically initialized to new random vectors Care should be taken with this process, not to reinitialize velocities when a good solution is found, since it may pull particles out of this good optimum To make sure that this does not happen, particle velocities can be reinitialized based on a reinitialization probability This probability starts with a large value that decreases over time This approach ensures large diversity in the initial steps of the algorithm, emphasizing exploration, while exploitation is favored in the later steps of the search Cooperation between the subgroups is achieved through the selection of the global best particle, which is the best position found by all the particles in both sub-swarms Particle positions are not updated using the standard position update equation Instead, a hill-climbing process is followed to ensure that the tness of a particle is monotonically decreasing (increasing) in the case of a minimization (maximization) problem The position vector is updated by randomly selecting consecutive components from the velocity vector and adding these velocity components to the corresponding position components If no improvement is obtained for any subset of consecutive components, the position vector does not change If an improvement is obtained, the corresponding position vector is accepted The value of changes for each particle, since it is randomly selected, with U (1, max ), with max initially small, increasing to a maximum of nx (the dimension of particles) The attractive and repulsive PSO (ARPSO) developed by Riget and Vesterstr m [729, 730, 877] follows a similar process where the entire swarm alternates between an attraction and repulsion phase The di erence between the MPPSO and ARPSO lies in the velocity equation, in that there are no explicit sub-swarms in ARPSO, and ARPSO uses information from the environment to switch between phases While.

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A fundamental part of any graphics software is the coordinate system used to specify the location of objects drawn on a drawing surface The desktop NET Framework supports seven distinct drawing coordinate systems in the GraphicsUnit enumeration Among the supported coordinate systems are Pixel, Inch, and Millimeter While the NET Compact Framework supports this same enumeration, it has only one member: Pixel This means that when you draw on a device screen, you are limited to using pixel coordinates One xception involves fonts, whose height is always specified in Point units This brings up another difference between the desktop NET Framework and the NET Compact Framework: available coordinate transformations The desktop provides a rich set of coordinate transformations scrolling, scaling, and rotating through the Matrix class and the 3 3 geometric transform provided in the SystemDrawingDrawing2D namespace The NET Compact Framework, by contrast, supports no coordinate mapping That means that, on handheld devices, application software that wants to scale, scroll, or rotate must handle the arithmetic itself because neither the NET Compact Framework nor the underlying operating system provides any coordinate transformation helpers What the NET Compact Framework provides, as far as coordinates go, is actually the same thing that the underlying Windows CE system provides: pixels, more pixels, and only pixels While it might be lean, the set of drawing services provided in the NET Compact Framework is surprisingly complete That is, almost anything you can draw with the desktop NET Framework can be drawn with the NET Compact Framework The key difference between the two implementations is that the desktop provides a far wider array of tools and helpers for drawing Programmers of the desktop NET Framework are likely to have little trouble getting comfortable in the NET Compact Framework, once they get used to the fact that there are far fewer features But those same programmers are likely to be a bit frustrated when porting desktop NET Framework code to the NET Compact Framework world and are likely to have to rewrite and retrofit quite a few of their applications drawing elements.

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