84 investigated in the present study as part of the preparation for a series of experiments on the influence of variations in the electron environment on the lifetime of the b-active tritium nucleus. In the first experiment of the series it is proposed to investigate the chemical shift of the half-life for an atomicmolecular tritium pair. Since the energy of dissociation of molecular tritium is close to that of molecular protium, and since atomic tritium, because of its higher mass and lower mobility, recombines more slowly than atomic protium, the procedure used to obtain atomic tritium can be worked out in experiments with protium ~called hydrogen from now on!. Atomic hydrogen is produced by thermal dissociation in a tungsten furnace, by low-frequency and radio-frequency gas discharges, or by means of a plasma arc. In the present study we have used the rf gas discharge method to obtain atomic hydrogen. The high efficiency of this method helps to minimize the heating of the discharge cell and can be implemented without the intrusion of electrodes in the discharge volume, thereby ensuring high purity of the atomic hydrogen product. The problems associated with the stabilization and detection of atomic hydrogen stem from its high chemical activity, by virtue of which atoms rapidly recombine at the walls of the discharge volume and in mutual collisions. For this reason, most diagnostic techniques applied to atomic hydrogen are based on measurements of secondary effects attributable to the presence of atomic hydrogen. For example, a chemical target of molybdenum oxide has been used as the atomic hydrogen detector in some studies. When hydrogen atoms are incident on such a target, the oxide undergoes reduction, and the target changes color. However, the small range of measurement of the flux density (10–10 atoms/s •cm) and low accuracy (630% error! limit the possibilities of this method. Bass and Broida have measured the optical spectra of hydrogen atoms in the condensed and gaseous phases, but did not establish any relationship between the concentration of hydrogen atoms and the line intensities of the optical spectra. One approach that looks promising is the determination of hydrogen atoms by electron spin resonance ~ESR!. This method utilizes the presence of an unpaired electron due to the paramagnetism of the hydrogen atom, a property that can be exploited for detection by ESR. Only papers in which ESR has been used to measure atomic hydrogen in the condensed phase are known in the literature. Here we report mass spectrometer measurements of atomic hydrogen produced in an rf gas discharge. The experimental apparatus ~Fig. 1! consists of an rf oscillator 1 ~1 MHz, 300 W!, a discharge tube 2, an MI 1201 mass spec-