By Optical Society of America
A brand new quantity within the field's bestselling concepts reference--an completely new opus concentrating on x-ray, nonlinear, and imaginative and prescient optics. presents an analogous mixture of educational writing with in-depth reference fabric that extraordinary Volumes I & II.
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The track bandwidth needs to be four times the Tyler frequency in order for σθG to be 1/4(λ/D), a condition that provides a Strehl ratio due to tilt of greater than 80 percent. Figure 12 shows the required 3-dB tracking bandwidths to meet this criterion for three combinations of wind and C2n profiles as a function of aperture diameter. Other combinations can be computed easily by using Eq. 29 and the wind profiles that are shown in Fig. 11. The one-axis rms tilt that is induced by the atmosphere is given by Eq.
24 and 25 can be partially corrected with a fast-steering mirror having an RC filter response, H(f, fc), of the form 1 H(f, fc) = ᎏ f 1 + iᎏᎏ fc (26) where fc represents a characteristic frequency [usually the 3 decibel (dB) response]. The uncorrected power in the residual errors can be computed from control theory using the relation σ2θG = ͵ |1 − H( f, f )| F ∞ c 2 ( f)df (27) φG 0 where FφG(f) is the power spectrum (rad2/Hz) of G-tilt induced by optical turbulence. For a steering mirror response function given by Eq.
It is possible to buy very powerful commercial off-the-shelf processing engines, but FIGURE 25 Sodium laser beacon signal versus average power of the pump laser. The lasers are (top to bottom) sum-frequency laser with a micropulsemacropulse format (150-µs macropulses filled with 700-ps micropulses at 100 MHz), a CW laser having six 10-MHz-linewidth lines, a CW laser having a single 10-MHz linewidth, and a pulsed-dye laser having 150-ns pulses at a 30-kHz repetition rate. 2 arcsec. Saturation of the return signal is very evident for the temporal format of the pulsed-dye laser and for the single-line CW laser.