Abstract
BH is obtained by high‐frequency discharge in 2% B2H6 mixed with He, Ar, or H2. It is selectively excited by a pulsed dye laser to A 1ΙΙ, v′ = 0, J′ = 1, 4, or 7. From these rotational levels, the total collision cross sections are obtained by lifetime measurements at known pressures and temperatures. They decrease as J′ increases. They are smaller for He than for H2 or Ar. The rare gases induce only rotational transfers. H2 also induces a quenching which is much smaller than the rotational transfers. The relative intensities of the satellite lines are measured for J′ = 4 up to ΔJ′ = ±3 : the levels of the same total parity as the initial level are more populated than the levels of the opposite total parity, this propensity decreasing from He to H2 and to Ar. The polarization of the excited lines does not vary appreciably with the pressure.

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