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The second spatial lter (SF2) is more simple than the spatial lter (SF1) in the phase conjugate feedback path since we simply use the cut edge of the output extracting mirror Using the mirror edge as a lter is advantageous since it is placed very near to the pseudo-far- eld plane, where the spatial mode separation is at maximum In contrast to the rst spatial lter (SF1), the second has only one ltering edge which, however, is found to be suf cient to secure that external feedback is coupled into one array mode only Figure 916 shows the far- eld intensity distribution (left-hand side) and the spectral distribution (right-hand side) of the laser diode array when different amounts of feedback are applied with spatially ltering in both the external feedback path and the phase conjugate feedback path; Figure 9.

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16a shows the freely running multimode output of the laser; Figure 916b shows the single-lobe but multimode frequency output when the spatially ltered external feedback is applied but no phase conjugate feedback is present (no FSPCF); Figure 916c shows the single-mode laser operation with the FSPCF applied but no external feedback; Figures 916d g show the laser output with FSPCF applied and increasing amount of spatially ltered external feedback It is clearly observed, from the curves in Fig 916, that the con guration of double spatial ltering leads to spectral and temporal stability of the single-mode output even when the output is re ected back into the laser system Furthermore, it is observed that the relative intensity of the two lobes in the spatial pro le can at the same time be varied continuously by varying the amount of external feedback.

Lock, Then Walk (Continued)

where S is the radial distance from the optical axis (S2 x2 y2 ), the rst term to the right of the equal sign is the defocusing, and the second term is the asphericity (primary aberration). The defocusing coef cient a should be chosen so that the minimum fringe spacing on the pupil aperture is as large as possible. The fringe spacing is de ned by the wavefront slope, so the maximum wavefront slope has to be minimized. This condition is satis ed if (see Fig. 12.2) 3 a bS2 2 max 12:2

A too-high external feedback intensity, however, destroys the single frequency but maintains the diffraction-limited output pro le In summary, it is shown that the single-mode output from a laser diode array with phase conjugate feedback has stable long-time operation with respect to output power and center wavelength However, the laser system is not robust against external feedback External feedback of the same order of magnitude as the phase conjugate feedback (ie, around 1% of the total output) is capable of destroying the single-mode operation of the laser diode array The destruction of the single-mode operation is due to external feedback into several array modes leading to mode competition.

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In a con guration with spatial ltering in both the output beam and the phase-conjugate feedback path, it is shown that the system is robust against external feedback, and the output is stabilized with good spatial and temporal coherence even in the presence of external feedback up to approximately 1%..

Next, you need to register the Album class with the controller by passing Album.class to the controller s setCommandClass method. By default, a new instance of Album is created each time the form is loaded. You can override the SimpleFormController s formBackingObject method if you want to customize this behavior so that you can, for example, reload an existing album in the form for editing. The following code shows an example of how this method is overloaded to retrieve an existing album from the database in case an ID parameter is passed to the form. This listing also shows how the Album class is registered as a command class in the constructor.

Timing (key milestones, closure):

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