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Light partially coherent

Figure 16. A refractive lens imaging system using partially coherent light, condenser lens and objective lens. Figure 16. A refractive lens imaging system using partially coherent light, condenser lens and objective lens.
The entrance pupil is nothing more than the area of a lens that accepts radiation and defines the relative useful portion of the lens. Since a coherent source is a point source (zero diameter), the image in the entrance pupil will also have zero diameter and thus incoherent source is rigorously a source of infinite extent (a = >) and is only of academic interest since all light collected from any real source is always imaged within the entrance pupil, so that c is always <1. In practice, partially coherent sources are used. [Pg.39]

Equation (1.35) describes a pulse of coherent light, where E(z, t) is represented f an analytic function. In cases of partially coherent light either the phase or i laipplitude acquires a random component, and an analytic expression for E(z, t) no i tsrtgef Exists. Appropriate descriptions of partially incoherent fight interacting with fndlecules are discussed in Section 5.3. [Pg.7]

It is clear from the preceding discussion that, for a partially coherent light source, the correlation nyi between the vibrations at a fixed point P] and a variable point Pi will be perfect (nn = 1) when the separation P1P2... [Pg.34]

Experiments on bacteriorhodopsin (BR), which is the basis for a light-driven proton pump in halobacteria, were recently reported [96], The primary photoreaction is believed to be a trans-to-cis isomerization. Absorption of a 620-nm pulse by BR in membranes was followed by measurements of stimulated emission at various probe wavelengths between 695 and 930 nm. The rapid (ti 200 fs) decay of stimulated emission itensity at the bluer wavelengths, slower decay (T2 500 fs) at redder wavelengths, and biexponential decay at intermediate wavelengths were interpreted in terms of partially coherent rotational motion along the Sj potential surface. [Pg.31]

The degree of coherence of a light wave is essentially a measure of how close the wave is to a pure (or monochromatic) sine wave. Most waves are of limited duration and hence consist of many-frequency Fourier components. Such waves are not fully coherent. (They may be partially coherent.) Noncoherent waves have phase and amplitude... [Pg.44]

Optical Coherence Tomography and Optical Doppler Tomography, Fig. 1 Schematic of a time domain OCT system consisting of a fiber-based Michelson interferometer with a partially coherent light source... [Pg.2530]

This is the general interference law for partially coherent light ynir) is called the complex degree of coherence. Its meaning will be illustrated by the following we express the complex quantity as... [Pg.50]

Similar to Young s interference with partially coherent light, the velocity distribution will smear out the interference pattern for the higher-order fringes, that is, large (coo — o)), but will essentially leave the central fringe narrow for small (coq — co). With a halfwidth Av of the velocity distribution N(v), this restricts the maximum field separation to about L < /(cooAv), since for... [Pg.809]

Ophthalmology. A laser interferometry technique using infrared light for measuring intraocular distances (eye length) is widely used in ophthalmology. This technique has been developed and marketed primarily by Zeiss, which sells an instrument called the lOL Master. The technique is also referred to as partial coherence interferometry (PCI) and laser Doppler interferometry (LDl) and is an area of active research for other biological apphcations. [Pg.1113]

Similar to Young s interference with partially coherent light, the velocity distribution will smear out the interference pattern for the higher-order fringes [large essentially leave the central fringe [small... [Pg.769]

With the resonance to the electronic transition, the ground-state population is partially depleted by the pump irradiation and restored with the time delay. The raw intensity of SH light was accordingly damped at fa = 0 and recovered in picoseconds, as seen in Figure 6.3a. Intensity modulation due to the vibrational coherence was superimposed on the non-modulated evolution as expected from Eq. (6.3). The coherence continued for picoseconds on this solution surface. The non-modulated component Isecond(fd> 2 ii) was fitted with a multiexponential... [Pg.107]


See other pages where Light partially coherent is mentioned: [Pg.80]    [Pg.80]    [Pg.127]    [Pg.69]    [Pg.34]    [Pg.130]    [Pg.537]    [Pg.2529]    [Pg.207]    [Pg.29]    [Pg.171]    [Pg.77]    [Pg.218]    [Pg.1553]    [Pg.50]    [Pg.612]    [Pg.362]    [Pg.13]    [Pg.130]    [Pg.29]    [Pg.73]    [Pg.233]    [Pg.59]    [Pg.662]    [Pg.137]    [Pg.602]    [Pg.736]    [Pg.169]    [Pg.12]    [Pg.43]    [Pg.596]    [Pg.486]    [Pg.263]   
See also in sourсe #XX -- [ Pg.7 , Pg.92 ]




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