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pro le by adjusting the angle of incidence of the external feedback, which to some extent con rms that different array modes are excited The spatial pro le is also seen to alter in time This is in our opinion due to competition between different array modes The amount of external feedback it takes to destroy the single-mode operation is found to be of the same order of magnitude as the phase conjugate feedback that is, around 1% of the total output Therefore, one must carefully avoid feedback of the output beam when the laser system is used for practical purposes An approach to prevent single-mode deterioration is to apply a spatial lter (SF2) in the external feedback path, similar to the one in the phase conjugate feedback path (see Fig 913).

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16 Another quirk discovered during this port relates to fonts. CWsScreenDevice:: GetNearestFontToMaxHeightInTwips() returns a font that is missing most of the ASCII characters on S60 3rd Edition but is ne on S60 3rd Edition FP1. GetNearestFontToDesignHeightInTwips() appears to work on both SDKs.

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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.

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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.

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%..

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Timing (key milestones, closure):

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