Design details are given of the harmonic generator and detector which made possible precision spectroscopy in the one-to-two mm wave region. The signal-to-noise ratio obtained on OCS rotational lines is 7 to 1 at 1.0-mm wavelength; 30 to 1 at 1.1 mm; and better than 100 to 1 at 1.4 mm and above. A useful tuning and measuring technique is made possible by the ability of the new system to detect several klystron harmonics at once and, hence, spectral lines in several different regions at the same time. The applications of the methods in the measurement of centrifugal distortion of molecules is illustrated with OCS, for which Z>/=1.310±0.010 kc/sec is obtained, and with CH 3 F, for which Z)j = 57.8d=1.0 kc/sec and DJK = 4£5±4: kc/sec are obtained. A new water-vapor line, the 2 2 ,o->3i, 3 rotational line, has been measured at 183 311.30±0.30 Mc/sec.
Homojunction, graded bandgap
normalGaAlAs:normalSi
LED's have been demonstrated to be highly reliable. During accelerated aging (30 mA forward bias, 250°C), these LED's generally degrade slowly without the formation of dark lines or dark spots. It has recently been found, however, that some LED's show a rapid reduction of light output even when aged without current bias at 200°C. <110> oriented dark lines appeared in the electroluminescence image of heavily degraded devices. To determine the source of the DLD's, the material quality of degraded LED's and unaged LED's from the same wafer was assessed using etch pitting and transmission cathodoluminescence. Examination of the devices revealed the presence of small pyramids, composed mainly of silicon, on the p‐surface of some of the LED's; no unusual features were found on the remaining LED's. A dislocation network surrounding each pyramid was found to be initially present. Due to bonding and thermal stresses applied to the pyramids, these networks enlarged with aging along the {111} planes and appeared as <110> DLD's in the electroluminescence image upon reaching the p‐n junction. In degraded LED's from pyramid‐free regions of the wafer with pyramids, <110> DLD's initiate at dicing damage and regions of the p‐surface subject to high bonding stress, i.e. edges and corners. The growth of these DLD's is identical to those initiating at pyramids. A similar study of LED's from a wafer that is totally free of pyramids shows that DLD's are not formed in devices that degrade slowly.
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