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5.4 The observations w = (WI . . W N ) are Poisson distributed and have expectations . ~ = yaexp(-pz,), where O = (aP)T with a,P > 0 are the unknown parameters and y > 0 is a known scale factor.

ln B V ( arctan C 2pN)t13 where s 2 2 1 2r21 r43 cos Dw r21 r43 , B 2r21 r43 (1 cos Dw) N is an integer It can be shown that the solutions of equation G 0, which was determined by Eqs (11), transit to Eqs (15) if al ! 1 The solutions (15) of the dispersion equation (13) include the branches with different values of N The number N can be regarded as an analogue of the serial number of a longitudinal mode generated by the joint scattering in the nonlinear layer It is possible to see from Eq (15) that the oscillation threshold of the phase conjugated wave and its frequency are strongly dependent on the transmission coef cients of the feedback loop (Dw, r21, r43) and the number N (Fig 104).

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If you set the XREFCTL system variable to 1 (by default, it s set to 0), a copy of all xref activity for your current drawing is saved in an ASCII text file. You can read the log to troubleshoot problems that may occur. Figure 19-15 shows part of an xref log file. The log file goes in the same folder as your drawing and uses your drawing name with the .xlg filename extension. This file can become long. Therefore, once in a while, you should delete all or part of the file.

The default setting of 50 percent allows you to clearly see the background at the same time as the clone source and in most cases determine where to place your first stroke Overlay Blending mode: If you find it hard to distinguish between the overlay and the original image, you can set the blending mode of the overlay to lighten or darken it so it is more easily distinguishable Clipped: By default, the clone source overlay is clipped to the area indicated by your Brush tool This is great for fix-ups where you aren t cloning specific items, but you ll find yourself toggling this option back and forth frequently as you work with specific objects Auto Hide: This option shows the overlay when your mouse button is released and hides the overlay as you paint in cloned areas.

For the reciprocal feedback loop (Dw 0, r21 r43) the minimal generation threshold is achieved for the mode with N 1 having nonzero frequency detuning V (Fig 104) The detuning indicates a general peculiarity of SRS: The pump wave diffracts on the slow-moving grating into the scattering wave with a small frequency shift comparable to a scattering line width Note that the threshold is in nite Gth ! 1 for the equal intensity of the pumping waves r21 r43 ! 1 In the presence of the phase nonreciprocity of the feedback loop (Dw = 0, r21 r43) the generation threshold can be considerably less than that for the reciprocal feedback The smallest threshold can be achieved for p/2 phase nonreciprocity (compare curves 1 and 3 in Fig 104) This fact can be explained as follows.

The p/2 phase nonreciprocity provides an optimal phase shift between the optical interference eld E1 E3 (or E2 E4 ) and the index grating induced by the interference eld of another pair of the optical waves dn24 (or dn13) As a result, the parametric interaction of two pairs of waves by mutual scattering on the grating is more effective than without any phase shift The threshold decrease in the scheme with the nonreciprocal feedback loop is particularly important in the case of equal-intensity pump waves (r21 r43 1) when the re ection coef cient of the phase conjugate mirror based on the joint SRS can be close to unity [14, 25] In this case the frequency of the phase conjugated.

Figure 5.18. Simultaneous identi cation and sequencing of regulatory sites in DNA. If identical samples are used for both DNA footprinting and sequencing (see Section 5.4.2), these can be electrophoresed on the same polyacrylamide gel. The regulatory sequence determined for the example shown is ATC (complementary to TAG), although in reality, regulatory sequences are usually longer than this.

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