Abstract

An experimental investigation of the rotational-state dependence of intermolecular interactions for dipole–dipole systems was performed with the aid of light-induced drift. Data are presented of the relative change in collision rate upon excitation, Δν/ν, of HF with respect to polar and nonpolar collision partners (CH3F, CH3Cl, HCl, OCS, and CH4, H2, CO2, respectively). A continuously tunable color-center laser was used to rovibrationally excite HF in the fundamental vibrational band (v=0→1). Both P- and R-branch excitations were studied, with the rotational quantum number ranging from J=0 to 6. By combining Δν/ν for all pairs of P(J) and R(J−1) transitions, the separate v and J dependencies of the collision rate ν are obtained. It is found that for HF–CH3F ν decreases by more than 40%, and for HF–CH4 by only 4%, as J increases from 0 to 6. These data show that the familiar 1/r3 dipole–dipole interaction is highly J dependent. We attribute this to the increased averaging-out of the dipole–dipole interaction as the rotational quantum number increases. A theoretical treatment based upon the first Born approximation for the total cross section of two rotating dipolar molecules is proposed. Comparison between measurements and theoretical results shows good agreement.

Full Text
Published version (Free)

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call