“…It is not trivial, however, to realize such a laser owing to the mismatches that occur between the emission lines in CO 2 and the absorptions in D 2 0, amounting to 0.32 GHz, 0.68 GHz and 1.5 GHz for R(22), R(12) and P(32) respectively. 1 No problem exists, of course, with a CO 2 TEA pump laser which can have an output several GHz wide due to pressure broadening, but for CW operation recourse must be made to capillary waveguide lasers which (unlike conventional devices) can operate at 100's of torr with consequent gain profiles typically 100's of MHz wide 2 . Waveguide lasers have been constructed in this laboratory from boron nitride (BN) 3 The combination of high thermal conductivity, low coefficient of expansion and ease of machining makes BN an ideal material with a better surface smoothness than that obtainable from beryllium oxide (BeO) or alimina (A1 2 0 3 ) . A typical laser consists of a 1.7 x 1.7 mm channel with 24 cm discharge length.…”