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64) Down-conversion processes are very important in quantum optics. 7 illustrates schematically two common applications of second-order nonlinear optics, namely second-harmonic generation and parametric amplification. In the former, a powerful pump beam at frequency ω generates a new beam at frequency 2ω by frequency doubling, as shown in Fig. 7(a). 2 Second-order nonlinear effects. The second column lists the frequencies of the light beams incident on the nonlinear crystal, while the third gives the frequency of the output beam(s).

A) What is the wavelength of the signal beam? (b) What wavelength would be generated by difference-frequency mixing of the signal and idler? 10) A potassium dihydrogen phosphate (KDP) crystal is used for frequency doubling of the radiation from a Nd : YAG laser operating at 1064 nm. 471. e. is invariant under the transformation r → −r) has to be zero. (b) Isotropic media such as gases, liquids, and glasses may be treated as materials with inversion symmetry on account of their lack of long-range order.

0 nm line of a sodium lamp operating at 100 ◦ C in the following two cases: (a) the line is Doppler-broadened; (b) the line is pressure-broadened with a full width at half maximum of 5 GHz. 8 nm. 6 and a nonlinear susceptibility of ∼10−12 m V−1 . Estimate the optical intensity at which the magnitude of the second-order nonlinear polarization is the same as that of the linear polarization. 8) A signal beam at 1400 nm is generated by parametric down conversion using a pump beam of wavelength 800 nm.

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Structural Design Manual McDonnel Douglas Corporation

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