winforms pdf 417 reader

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beam makes its rst four passes through the ampli er, it accumulates wavefront phase errors due to thermal aberrations in the solid-state ampli er slab as well as to residual optical gure errors in the other optics in the ring The SBS cell effectively conjugates the phase of the input beam, producing a wavefront-reversed output Stokes beam with a small frequency shift (,5 GHz for carbon tetrachloride, CCl4) As this output beam retraces the path of the input beam through four additional gain passes, the phase errors cancel and the high-quality wavefront of the injected beam is recovered in the high energy output However, it is important to note that there are additional very distinct advantages to the operation of the ampli er system with the SBS phase conjugator.

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Eight gain passes through the zigzag slab ampli er can be achieved using passive polarization switching in the regenerative ampli er ring The fact that the SBS cell provides interstage gain isolation makes this possible since, if it were replaced with a mirror, the small signal gain through eight consecutive gain passes would result in possible parasitic oscillation from the small re ective losses of AR-coated optical surfaces in the ring or in the output beam When the Pockels cell is located inside the regenerative ampli er ring, the length of the laser pulse to be ampli ed is limited to the transit time inside the ring minus the high-voltage switching time for the Pockels cell Now, with passive polarization switching, this time limit is increased to be the transit time for four ring revolutions.

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Longer pulses can be ampli ed, and the relative timing accuracy requirement between the injected pulse and the Pockels cell voltage pulse is greatly reduced In fact, the replacement of the Pockels cell with a full-aperture Faraday isolator has been shown to allow the ampli cation of laser pulses of over 500 ns in duration [32], as will be described in a following section of this chapter Another advantage is that the SBS phase conjugator very effectively conjugates the rst-order aberration of tilt The combination of this tilt correction and relay imaging greatly reduces the sensitivity of the system performance to small changes of optical alignment in the ring No change in output power or pointing direction during operation is observed for large mirror misalignments in the ring, limited only to those angular excursions that result in vignetting of the beams at the edges of the ampli er slab 5.

325 Single-frequency oscillator The 1053-nm transition in Nd:YLF closely matches the uorescence curve peak in the Nd-doped phosphate glass used in this ampli er system It is desirable to have a single-frequency oscillator input pulse both for generating reproducible smooth temporal input pro les without modulation from multilongitudinal modes and for achieving the best wavefront reversal delity in the SBS phase conjugator [33, 34] Although single longitudinal mode output from an Nd:YLF Q-switched oscillator has been demonstrated by injection locking to a low-power single-frequency master oscillator, this technique requires careful mode matching between the master and slave oscillators and active cavity length stabilization of the Q-switched slave oscillator [35] A simpler method of achieving single-frequency output was chosen for this application by using a variation of the electronic linewidth narrowing technique [36, 37] In this method,.

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are scalars. Since soLis scalar and C-' is symmetric,

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