The surface laser-induced damage threshold (LIDT) of CsLiB(6)O(10) (CLBO) crystal was enhanced twofold with improved crystallinity and ion-beam etching. For crystals with high crystal quality (bulk LIDT, 15.0-19.0 GW/cm(2)), the surface LIDT was 1.4-fold higher than for those with conventional crystal quality (bulk LIDT, 9.0-12.0 GW/cm(2)). In addition, removal of residual surface-polishing compounds by means of ion-beam etching can further enhance the surface LIDT by another 1.5-fold. Thus, CLBO crystals with high crystal quality and ion-beam etching are now more reliable for high-power UV light generation.

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The focusing characteristics of the high dispersion mass spectrograph at Osaka University has considerably been improved. The distinguishing features of this apparatus is that the mass dispersing action of a r -1 magnetic field is utilized. The apparatus has a r -1 magnetic field of 198.1° sector type (22 cm mean radius) as the dispersing field, a toroidal electric field of 118.7° (30 cm mean radius) and a 30° uniform magnetic field (120 cm mean radius) as the focusing fields. The total ion path is about 6.5 m. The principle, the design and the construction of the apparatus was described previouslyThe parameters of the apparatus are shown in Fig. 1 As already reported, in the preliminary experiment, the dispersion on the photographic plate was estimated to be about 14 cm for 1% mass difference and the agreement with the calculation was satisfactory, but, the spectral lines were considerably curved. Recently this curving effect has been removed. The cause of this effect has proved to be a slight magnetization of the slit which restricts an ion beam in the dispersing magnetic field. A movable slit as shown in Fig. 1 was placed in the dispersing magnetic field near the entrance and was adjusted so that the ion beam was passing through the rectangular hole. If it is slightly magnetized by a magnetic field of about 5000 gauss and the magnetic field near the upper and lower ends of the hole is increased by about 50 gauss as compared with that near the center over a region of slit thickness, say about 1 mm, then the difference between the lateral position of the center beam and that of the end beam is estimated to be about 0.16 mm at the image point. This makes the spectral lines considerably curved. Formerly, the slit was made of 18-8 stainless steel (JIS SUS 27) sheet and was slightly magnetized unfortunately. It has been replaced by a non-magnetic material (Mo), and the curving effect has been removed.Further improvements in the sharpness of the spectral lines have been accomplished in the following way. 1 H. MATSUDA, S. FUKUMOTO, Y. KURODA, and M. NOJIRI, Z. Naturforschg. 21a, 25 [1966].Fig. 1. Movable slit in the dispersing magnetic field. Slit hole dimension: 4 mm x 5 mm.Two origins of broadening spectral lines were found out. One is vibrations due to mechanical pumps and the other hum magnetic fields. In order to reduce the stray magnetic field, a number of iron sheets are placed near the magnets. Small vibrations of these sheets caused by the motion of mechanical pumps disturbed magnetic fields considerably. In order to reduce this effect, mechanical pumps have been replaced by sorption pumps during exposures. A considerable 60-cycle hum magnetic level is found in the laboratory where the mass spectrograph is constructed. Even if there is no exciting current, the magnets catch a few milli gauss of hum magnetic flux. In order to reduce the hum magnetic field, a negative feedback method is adopted. The output of a pick up coil of 75 turns which is wound around the magnet pole piece is amplified, phase-inverted and...

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