A pulsed source for Xe(6s[3/2]1) and Xe(6s′[1/2]1) resonance state atoms using two‐photon driven amplified spontaneous emission from the Xe(6p) and Xe(6p′) states

Energy-Transfer Kinetics Driven by Midinfrared Amplified Spontaneous Emission after Two-Photon Excitation from Xe (s0) to the Xe (6p[1/2]0) State

In optically pumped laser systems, rare gas lasers (RGLs) are a field of great interest for researchers. Gas laser regimes with metastable Ne, Ar, and Kr atoms have been investigated, while studies of RGLs based on metastable Xe are sparse. In this work, when a strong excitation laser (2.92 mJ/pulse, 7.44 × 10⁵ W/cm²) was applied to excite Xe atoms from the ground state to the 6p[1/2]₀ state, an interesting phenomenon emerged: An intense fluorescence of 980 nm (6p[1/2]₁-6s[3/2]₂) was produced. However, when the energy of excitation laser was decreased to 0.50 mJ/pulse (1.27 × 10⁵ W/cm²), the fluorescence of 980 nm became very weak. Besides, lifetime and decay rate constant of the 6p[1/2]₀ state under the condition of E = 2.92 mJ are significantly different from either those measured by other groups or those of E = 0.50 mJ. These phenomena indicate that the high energy of excitation laser should trigger some new kinetic mechanisms. Further works identified that the new kinetic mechanism is the MIR ASE of 3408 nm (6p[1/2]₀-6s'[1/2]₁). The mechanisms are proposed as follows. Substantial 6p[1/2]₀ atoms are produced by laser excitation. Then, the ASE of 3408 nm (6p[1/2]₀-6s'[1/2]₁) is quickly produced to populate substantial 6s'[1/2]₁ atoms. The 6s'[1/2]₁ atoms can readily arrive at the 6p[1/2]₁ states through collision by virtue of the small energy difference (84 cm^-1) and high collision rate constant of the transition from the 6s'[1/2]₁ state to the 6p[1/2]₁ state. As a result, the intense fluorescence of 980 nm is generated.

Production yields of H(D) atoms in the reactions of N2(AΣu+3) with C2H2, C2H4, and their deuterated variants

The production yields of H(D) atoms in the reactions of N(2)(A (3)Sigma(u) (+)) with C(2)H(2), C(2)H(4), and their deuterated variants were determined. N(2)(A (3)Sigma(u) (+)) was produced by excitation transfer between Xe(6s[32](1)) and ground-state N(2) followed by collisional relaxation. Xe(6s[32](1)) was produced by two-photon laser excitation of Xe(6p[12](0)) followed by concomitant amplified spontaneous emission. H(D) atoms were detected by using vacuum-ultraviolet laser-induced fluorescence (LIF). The H(D)-atom yields were evaluated from the LIF intensities and the overall rate constants for the quenching, which were determined from the temporal profiles of the NO tracer emission. The absolute yields were evaluated by assuming that the yield for NH(3)(ND(3)) is 0.9. Although no HD isotope effects were observed in the overall rate constants, there were isotope effects in the H(D)-atom yields. The H-atom yields for C(2)H(2) and C(2)H(4) were 0.52 and 0.30, respectively, while the D-atom yields for C(2)D(2) and C(2)D(4) were 0.33 and 0.13, respectively. The presence of isotope effects in yields suggests that H(2)(D(2)) molecular elimination processes are competing and that molecular elimination is more dominant in deuterated species than in hydrides.

H(D)-atom yields in the quenching of Xe(6s[3∕2]1) by methane, ethane, ethene, ethyne, and their deuterated isotopologues

The yields for the production of H(D) atoms in the reactions of Xe(6s[3/2]1) with simple hydrocarbons and their deuterated variants were determined. Xe(6s[32](1)) was produced by two-photon laser excitation of Xe(6p[1/2]0) followed by concomitant amplified spontaneous emission. H(D) atoms are detected using a vacuum-ultraviolet laser-induced fluorescence (LIF) technique. The H(D)-atom yields were evaluated from the LIF intensities and the overall rate constants for the quenching, which were determined from the temporal profile measurements of the resonance fluorescence from Xe(6s[3/2](1)). HD isotope effects were observed not only in the overall rate constants but also in the H(D)-atom yields. The yields for CH4, C2H4, and C2H2 were determined to be 0.89, 1.43, 1.03, respectively, while those for CD4, C2D4, and C2D2 were found to be smaller; 0.63, 0.86, and 0.79, respectively. The HD yield ratio for CH2D2 was 1.76. The presence of the isotope effects both in the rate constants and the yields suggests that electronic-to-electronic energy transfer processes and abstractive processes are competing.

Collisional deexcitation of optically allowed excited atoms by axially symmetric molecules

The deexcitation process of an atom in an optically allowed excited state by a collision with an axially symmetric molecule is considered. In order to make a precise comparison with experimental data that have recently been obtained, we extend previous work for a Penning ionization process [T. Watanabe and K. Katsuura, J. Chem. Phys. 47, 800 (1967)]. Using the straight-line trajectory impact parameter method, the probability of deexcitation in the incident atom is described by a discrete-continuum excitation transfer mechanism. The effects of the ionization yield eta in molecular target and of the molecular anisotropic property of the optical transition dipole are considered. The cross-section formula sigma is presented by a similar formula for Penning ionization of the atomic target by introducing a stereo factor C(lambda) as sigma = C(lambda)[e(4)mu(2)mu(E, perpendicular)/(4piepsilon(0))(2) (2)hv](2/5). Here, v is the relative velocity of the colliding system and lambda is given by the ratio lambda =(mu(E||)/mu(E perpendicular)), where mu, mu(E perpendicular), mu(E||) are the transition dipole moments of an excited atom, A-->A(*), those of a molecule at energy E for the perpendicular component and the parallel component with respect to molecular axis. Applications to He(*)(2(1)P)+H(2) (or D(2)), Ne(*)[2p(5)((2)P(1/2))3 s (1)P(1)]+ H(2) (or D(2)) systems and systems of the same projectiles on C(6)H(6), (or C(6)D(6)) molecules are made. The results for hydrogen molecules are compared with the experimental data.