Abstract

<p>The oscillator strengths of the <sup>1</sup><i>S</i><sub>0</sub>−<sup>1</sup><i>P</i><sub>1</sub> (1165Å) and the <sup>1</sup><i>S</i><sub>0</sub>−<sup>3</sup><i>P</i><sub>1</sub>, (1236 Å) resonance transitions in krypton and the <sup>1</sup><i>S</i><sub>0</sub>−<sup>1</sup><i>P</i><sub>1</sub> (1296 Å) resonance transition in xenon were determined by the method of total absorption. A 2-m absorbing path and pressures in the range of 0.006–0.064 torr were used. The results were</p><p>Kr: <sup>1</sup><i>S</i><sub>0</sub>−<sup>1</sup><i>P</i><sub>1</sub> (1165 Å) <i>f</i>=0.193±0.009 (39 determinations)</p><p>Kr: <sup>1</sup><i>S</i><sub>0</sub>−<sup>3</sup><i>P</i><sub>1</sub> (1236 Å) <i>f</i>=0.187±0.006 (49 determinations)</p><p>Xe: <sup>1</sup><i>S</i><sub>0</sub>−<sup>1</sup><i>P</i><sub>1</sub> (1296 Å) <i>f</i>=0.194±0.005 (35 determinations).</p>

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