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The top-level application class is called WmvcApp A user application will derive its toplevel application class from WmvcApp The basic structure of the Wmvc framework is shown in Figure 5-10 The class diagram for WmvcApp shows the most important services it provides WmvcApp allows the user app class to build an application easily The app will define the elements of the menu bar, tool bar, and drawing panes The user app defines menus by creating JMenu objects, and then adding items to those menus using the Wmvc menu controllers, and finally adding the menus to the menu bar with WmvcAppaddMenu Tool bar items are defined and added to the tool bar using Wmvc controller objects WmvcApp provides a JPanel for the app to define whatever is needed for views WmvcApp provides the basic functionality needed to build simple "standard" applications Although it is not that complicated, it simplifies the job of the programmer The details of defining a tool bar and a JPanel are hidden WmvcApp has another job - to support the MVC model While the structure of an MVC program is clear, the MVC structure must really hang off of something In the Wmvc framework, the WmvcApp class provides the foundation to build the MVC structure on Because all the views must access the model WmvcApp provides the services setModel() and getModel() to give them access to the model It provides a class method to get access to the WmvcApp object itself WmvcApp does not provide direct support for views Instead, views are created in the derived WmvcApp class directly The Thermometer example later will help make this clear The details of creating the tool bar and drawing canvas are found in the WmvcAppjava code In addition to the services already discussed, WmvcApp provides a standard way to.

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The outer plates are identical, with their axes set parallel to each other; the centre plate is of half-wave retardation, made of the identical material but with its axis set at some angle relative to the outer plates The solution for an achromatic half-wave plate, for example, uses three alf-wave plates, the middle element set with its fast axis at 57 to the outer plates Although Pancharatnam designs have excellent properties in terms of the achromatization of the phase delay, they have a drawback in that the effective reference axis is not parallel to the fast axes of any of the individual plates, and this is exacerbated by the fact that it varies with wavelength, oscillating by a few degrees over the spectral range for which the achromatism of the phase delay is designed In the measurement of the polarization of the light from stars, this axial dispersion results in changes in the orientation of the instrumental reference frame used for the determination of the Stokes parameters according to the operating wavelength passband; the measurements are later transformed to equatorial coordinates In practice, the dispersion of the instrumental frame is calibrated from observations of standard stars, but the whole transformation process is susceptible to errors when very high accuracy polarimetry is pursued By using a Pancharatnam design with elements which themselves are achromatic, a device that may be described as being superachromatic ensues In addition to its chief function of introducing a relative phase delay, a wave plate also acts as a weak partial polarizer and this may have repercussions in the pursuit of high accuracy polarimetry Re ection losses at the entrance and exit faces depend on the refractive indices of the plate As the device is made of birefringent material, the re ection losses, and hence the transmittances, Tf , Ts , for the fast and slow orthogonal axes de ning the phase delay, have different values A common design for a polarimetric modulator comprises a rotatable wave plate prior to a xed polarizer The small polarizance that the wave plate possesses introduces a spurious signal that may affect the determined Stokes parameters (see Clarke, 2005) The polarizance can be reduced, but not removed completely, by applying anti-re ection coatings to the wave plate surfaces The true nature of a wave plate may be summarized by the Mueller matrix: 2 Tf C Ts 6 Tf Ts 6 4 0 0 or 2 k1 6 k2 6 40 0 k2 k1 0 0 0 0 k3 cos k3 sin 3 0 0 7 7, k3 sin 5 k3 cos .

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