Download Advanced Optical Imaging Theory by Min Gu PDF

By Min Gu

ISBN-10: 3662142724

ISBN-13: 9783662142721

Optical microscopy and linked applied sciences complicated speedy after the creation of the laser. The recommendations have motivated extra improvement of optical imaging concept, together with three-dimensional microscopy imaging conception in spatial and frequency domain names, the idea of imaging with ultrashort-pulse beams and aberration concept for high-numerical-aperture targets. This publication introduces those new theories by way of smooth optical microscopy. It comprises seven chapters together with an creation. The chapters are prepared to reduce cross-referencing. Comparisons with classical imaging concept are made while the hot imaging conception is brought. The publication is meant for senior undergraduate scholars in classes on optoelectronics, optical engineering, photonics, biophotonics and utilized physics, when they have accomplished glossy optics or an analogous topic. it's also a reference for different scientists drawn to the field.

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If, on the other hand, r2 = 0 in Eq. 1), then the diffraction pattern on the axis becomes ika ) sin (ka ( -4z . ~) . 5) This equation gives rise to an aperiodic oscillation of a constant amplitude with respect to the propagation distance. 6]. 6) so that Eq. 1) can be expressed as 24 2. 7) Here N is the Fresnel number defined in Eq. 6) which includes a constant should be noted that N is a function of the distance z. TC. It ya Fig. 1 plane. 5 Fresnel Diffraction by Different Apertures 25 The intensity of the diffraction pattern is the modulus squared of Eq.

VI). Thus, a narrower APSF results in less cross-talk between the APSFs originating from different positions (x~> y 1). As a result, a high resolution image can be obtained. If the size of a lens is quite large, the 2-D amplitude point spread function becomes h(x, y) = (kx)(ky), which is a point. In this case, there is no cross-talk between the point spread function in the image plane. Thus the image of an object is exp[- ikM 2~ (x~. + y~)(l+ M)]o(- Mx . ,-MyJ . 13) Eq. 13) implies that the image of an object is a magnified and inverted replica of the object in the image plane, if a lens is much larger than the object.

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