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In this chapter, the uses of lenses to form the Fourier transform or the image of an incoming coherent wave are discussed. Both issues are discussed from the point of view of diffraction. Imaging can also be discussed from the point of view of geometrical optics using rays as discussed in 8. The results obtained with diffraction are totally consistent with those of geometrical optics. This chapter consists of seven sections. Section 9.2 discusses phase transformation with a thin lens, using its physical geometry. The phase function obtained is used in Section 9.3 to show how lenses form an output eld, which is related to the Fourier transform of the input eld in various geometries. This leads to the linear ltering interpretation of imaging in Section 9.4. The theory discussed up to this point is illustrated with phase contrast microscopy in Section 9.5 and scanning confocal microscopy in Section 9.6. The last section highlights operator algebra for complex optical systems.

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Table 15.8 The Specifications for the Tag Attributes DESCRIPTION Used to specify the name to be used within the tag Used to specify the tag requirement. The values that this attribute accepts are true, false, yes, or no

of his experiments was Polaroid, a plastic sheet with tiny polarizing crystals embedded in it. By 1937, Land s garage laboratory had become the Polaroid Corporation. His hunch had paid off. Because re ection polarized light, the glare that irritated motorists or ruined photographs could be cut down dramatically by placing a piece of Polaroid material in the way. The material mostly let through light polarized in one direction; by rotating it to 90 degrees from the polarization of the re ected light, Polaroid could remove glare from practically any surface. Polarization was given a whole new lease of practical life much later in the century with the development of the liquid crystal. The liquid crystal rotates polarized light through 90 degrees unless there is an electrical current across it. The crystal is sandwiched between two polarizing lters at 90 degrees to each other. Normally that would mean that no light would get through the result would be black. But the liquid crystal s 90-degree twist takes the light that passes through the rst lter and gives it just the right twist to get through the second, giving a patch of light colour. When the power is on, the twist isn t applied, the light from the rst lter is cut out by the second and the result is an area of black. Polarizing materials continue to be important to this day, but in the second half of the twentieth century the technology of light was transformed from a specialist industry to an essential part of everyday life. Along the way, one man would make as great a contribution as Maxwell and Einstein to light s complex history.

public AddressEntityBean implements EntityBean { private DataSource datasource; private AddressDAO addressDao; .... public void setEntityContext(EntityContext ctx) { try { InitialContext i_ctx = new InitialContext(); String database = i_ctx.lookup("database_type"); dataSource = i_ctx.lookup("jdbc/pooledSource"); } catch(Exception e) { } } }

The TLD file is an XML file that contains the tag library description. It contains a list and description of all the custom tags in the library that are used as a reference to validate the existence of the respective tags. The components of a TLD file can be broadly classified into two groups. The first group comprises the elements of the root tag of the TLD file or the taglib tag written as <TAGLIB>. The second group placed within the taglib tag comprises the elements that are a part of the tag element written as <TAG>. Table 15.6 lists the elements of the TLD file at the taglib level.

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