posted on 2013-04-25, 00:00authored byNanase Kohno, Jun Yamashita, Chihiro Kadochiku, Hiroshi Kohguchi, Katsuyoshi Yamasaki
The
vibrational relaxation of OH(X<sup>2</sup>Π) by collisions
with rare gases is very slow due to small molecular interactions.
No measurement of the rate coefficients has been made for relaxation
of relatively low vibrational levels <i>v</i> ≤ 4
of OH by He, and there is only one report of the upper limit for <i>v</i> = 2, <1 × 10<sup>–14</sup> cm<sup>3</sup> molecule<sup>–1</sup> s<sup>–1</sup>. In this article,
we have studied vibrational relaxation of the levels <i>v</i> = 1–4 of OH(X<sup>2</sup>Π) by collisions with He.
A gaseous mixture of O<sub>3</sub> and H<sub>2</sub> in a carrier
gas at 70–130 Torr of He was irradiated at 266 nm, and OH(X<sup>2</sup>Π, <i>v</i> ≤ 4) was generated in the
reaction O(<sup>1</sup>D) + H<sub>2</sub>. A single vibrational level
of OH was detected with laser-induced fluorescence (LIF) via the A<sup>2</sup>Σ<sup>+</sup>–X<sup>2</sup>Π transition.
Time-resolved LIF intensities of OH(<i>v</i>) were recorded,
and kinetic analysis was made by an originally developed integrated
profiles method (IPM). On the basis of the evaluation of the pressure-dependent
rate coefficients of diffusion loss and the effect of impurities on
the kinetics, the rate coefficients of vibrational relaxation for
OH(X<sup>2</sup>Π, <i>v</i> = 1–4) by He have
been determined to be (2.9 ± 1.5) × 10<sup>–17</sup>, (1.4 ± 0.4) × 10<sup>–16</sup>, (5.2 ± 0.5)
× 10<sup>–16</sup>, and (1.6 ± 0.2) × 10<sup>–15</sup> cm<sup>3</sup> molecule<sup>–1</sup> s<sup>–1</sup> for <i>v</i> = 1, 2, 3, and 4, respectively
(the confidence limits are 2σ). The rate coefficients are larger
at higher vibrational levels and smoothly correlate to those reported
previously for <i>v</i> = 10–12.