| 摘要 |
1,111,058. Lasers. INTERNATIONAL BUSINESS MACHINES CORPORATION. 2 Nov., 1966 [29 Dec., 1965], No. 49049/66. Heading H1C. [Also in Division G2] An optical scanner providing a circular scan comprises a source 10 of linearly polarized light, Fig. 1, a polarization rotator 26, and an analyser 50 receiving the rotator output and passing only that filament 58 of the polarized light beam which is polarized in a given direction, the rotator being electrically controlled so as to produce a variable polarization rotation and thus enable different light filaments to become effective in turn along the scanning path. In the arrangement shown the linear polarization 62 of each light filament emitted by a laser light source is tangential to a circumference about the geometric axis, and the rotator comprises a quarter wave plate 28 and two vertically-spaced and independently energized electro-optic crystals 30, 32 with transparent electrodes 34, 36, 42, 44. The use of two electro-optic crystals is necessary to enable the analyser 50 to differentiate between diametrically-opposed light filaments which have parallel linear polarizations. The light source, Fig. 2, comprises a frusto-conical bi-refringent crystal having its optic axis 16 parallel to the geometric axis 18, the centre of the crystal being formed with two conical cavities 20, 24. This crystal totally reflects linearly polarized ordinary rays 58 of incident light 54 and disperses the extraordinary rays 56. The reflecting laser crystal and a partially transmitting mirror 52 together form the laser resonator. In an alternative arrangement, Fig. 4, a laser comprises a right circular cylindrical crystal rod 80 having its optic axis 84 inclined at 60 degrees to the geometric axis 82, the resonator being formed by separate mirrors 86, 88. As all the light emitted by the crystal is linearly polarized in the same direction, selection of a required light filament after rotation by a rotator 90 comprising an electro-optic crystal 92 and a quarter wave plate 102 is effected by an analyser formed of several analyser segments 106-118 radially oriented with respect to the geometric axis. The crystal 92 may be divided. In a modification laser action is not used, the crystal of Fig. 1, being illuminated from a narrow-band light source 72, Fig. 3, through a collimating lens 74 and a beam splitter 76. End illumination of the crystal 80 is used in the modified Fig. 4 arrangement, Fig. 5 (not shown). In both cases the resonator components are omitted. |
