Patent GB-1031230-A (GB)
Title: Laser structure
IPC: H01S3/102
Filed: 1963-10-03
Abstract: 1,031,230. Lasers. AMERICAN OPTICAL CO. Oct. 3, 1963 [Oct. 3, 1962], No. 38969/63. Heading H3B. A laser is provided with a source of pumping light and a source of control light of a wavelength effective to depump the laser and so control the laser output. Laser 10 is pumped by flash-tube 31 while a control laser 22 is pumped by flash-tube 32. Both flashtubes are controlled by trigger circuit 37. By providing laser 10 with higher pumping energy per unit volume than laser 22, laser 10 is caused to start producing its output before laser 22. Light from laser 22, when it is produced, is focused to a hollow cone by lens 42 having a central mask 44, and enters laser 10 through a small hole in end mirror 17. Since light from laser 22 enters laser 10 off the longitudinal axis it stimulates off-axis modes in laser 10 and the upper laser-active energy level is rapidly depopulated. The axial mode of laser 10 is immediately suppressed and off-axis light stimulated by laser 22 is blocked by mask 45. The instant at which an output is produced by laser 22 may be varied by altering the electrical energy supplied to flashtube 32, altering the triggering time of one flash-tube relative to the other, or by utilizing Q-switching. In Fig. 4 (not shown), a Kerr cell 52 is used to control the output from laser 22, the Kerr cell forming part of the resonant cavity. Alternatively, the Kerr cell may be outside the resonant cavity and act as a modulator. Arrangements utilizing the Pockels or Faraday effects are also referred to. Instead of using an off-axis beam to depump laser 10, an axial plane-polarized beam may be used. Lens 42 is replaced by a polarizer and mask 45 by an analyser. A further modification separates the beams by wavelength separation. Laser 22 is arranged to produce light of a band of wavelengths which is included within but is narrower than, the output band of laser 10. A filter is then used to block light from the narrower band which passes through laser 10. The difference in wavelength spread may be achieved by using neodymium-doped glass for laser 10 and neodymium in a crystal lattice, e.g. calcium tungstate, for laser 22. Another arrangement uses time separation of the beams (Fig. 8). A rotating shutter 70 is provided with radial slits through which the output from laser 10 is focused, the shutter and lenses lying within the resonant cavity of laser 10 so as to form a Q-switching arrangement. Each pulse of pumping light to laser 10 produces an output consisting of a series of short duration light pulses. If, after pumping has been initiated, but before an output is produced, laser 10 receives a pulse from laser 22 it becomes depumped and the first few output pulses from laser 10 are suppressed. Logic elements. An optical NOR gate (Fig. 11, not shown), consists of three lasers of equal dimensions, the outputs from two of them falling on an end face of the third at a large angle to its longitudinal axis. A mask is provided at the output end of the third laser, similar to mask 45. If either of the first two lasers produce an output the third laser is depumped and produces no axial output. Fig. 12 shows an arrangement for controlling the instant of switching on laser 170. The control laser 172 is made very much shorter than controlled laser 170, and its output passes axially through laser 170, so initiating laser action therein in an axial mode. The pump power applied to laser 172 is adjusted so that it produces its output at the desired instant. The device may also be adapted to operate in the manner shown in Fig. 1, laser 172 terminating the output from laser 170. The invention may be applied to pulsed, semi-continuous, or continuous lasers. The laser elements described consist of neodymium glass cores surrounded by glass cladding of lower refractive index. Unclad rods, or clad or unclad fibres may also be used. If a laser fibre is embedded in a common cladding with a plain glass fibre, control light may be directed longitudinally through the glass fibre and coupled to the laser fibre by " cross-talk." The fibres are spaced by a distance of the same order as the laser output wavelength. The time of operation of a control laser in any embodiment may be adjusted by varying the laser threshold level, e.g. by varying the amount of rare-earth dopant used or by selecting different host materials, e.g. flint glass, crown glass or crystalline material. The threshold may also be varied by varying the Q of the laser, e.g. by altering its length, or the reflectivity of its end faces. If the laser material includes two or more closely spaced levels, one of which is normally involved in the laser action, depopulation may be accomplished by supplying light of a wavelength corresponding to another of the closely spaced levels.