I. State-selected study of ion-molecule reactions using tandem molecular beam photoionization mass spectrometry; II. Absolute spin-orbit-state excitation cross sections for the reactions Ar+(2P3/2 ) + Ar(1S0) and Ar+(2P3/2) + N2(X~, v=0)

摘要

A new ion-molecule reaction apparatus, which consists of a photoionization source, a tandem mass spectrometer, and a radio frequency (rf) octopole reaction cell, is described. Using a quadru- pole mass filter to reject H(,3)(\u27+) background ions formed at the photo- ionization region, absolute total cross sections for the reaction H(,2)(\u27+)((upsilon)(,0)\u27) + H(,2)((upsilon)(,0)\u27\u27 = 0) (---\u3e) H(,3)(\u27+) + H, have been measured as a function of the vibrational state of reactant H(,2)(\u27+), where (upsilon)(,0)\u27 = 0-4, over the center-of-mass collision energy range of 0.04-15eV;Absolute spin-orbit-state-selected total cross sections for charge transfer reactions Ar(\u27+)((\u272)P(,3/2)) + N(,2)((\u27)X, v = 0) and Ar(\u27+)((\u272)P(,1/2)) + N(,2)((\u27)X, v = 0), (sigma)(,3/2) and (sigma)(,1/2), respectively, at the E(,c.m.) range of 0.25-115.3 eV have also been measured using the same apparatus;With the triple-quadrupole double-octopole photoionization tan- dem mass spectrometer, absolute state-selected total cross sections, (sigma)(,v\u27), v\u27 = 0 and 1, for reaction N(,2)(\u27+)((\u27)X, v\u27 = 0,1) + Ar((\u271)S(,0)) (---\u3e) N(,2)((\u27)X,v) + Ar(\u27+)((\u272)P(,3/2,1/2)) (reaction (1)) over E(,c.m.) range of 1.2-140 eV have been;measured. These measurements, together with the relative values for s(,v\u27), v\u27 = 0-2, and spin-orbit-state distributions of product Ar(\u27+) ions determined using the crossed ion-neutral beam photoionization apparatus, allow the determination of the absolute values for (sigma)(,2) and partial state-to-state cross sections, (sigma)(,v\u27(---\u3e)J), v\u27 = 0-2, for reaction (1);Experimental state-to-state cross sections obtained in this study are consistent with those for the reaction, Ar(\u27+)((\u272)P(,3/2)) + N(,2)((\u27)X, v = 0) (---\u3e) Ar((\u271)S(,0)) + N(,2)(\u27+)((\u27)X, v\u27), from the consideration of microscopic reversibility;Using the triple-quadrupole double-octopole apparatus, absolute fine-structure transition cross sections for the reactions Ar(\u27+)((\u272)P(,3/2));+ Ar and Ar(\u27+)((\u272)P(,3/2)) + N(,2)((\u27)X, v = 0) at laboratory collision energies of 25-200 eV have been measured; *USDOE Report IS-T-1261. This work was performed under Contract W-7405-Eng-82 with the U.S. Department of Energy.