J. J. Tiee
Los Alamos National Laboratory
Network
Latest external collaboration on country level. Dive into details by clicking on the dots.
Publication
Featured researches published by J. J. Tiee.
Journal of Chemical Physics | 1983
Gary W. Loge; J. J. Tiee; F. B. Wampler
The B 1Σ+ state of carbon monoxide was created by a two‐photon absorption of 230 nm laser radiation. The B 1Σ+ state was identified by the positions of the Q branch 0–0 absorption band and the vibrational bands of B 1Σ+ → A 1Π fluorescence occurring after excitation. Collision‐induced b 3Σ+ → a 3Π emission in the 350 nm region was also observed. The lifetimes of the B 1Σ+ → A 1Π and the b 3Σ+ → a 3Π emission were obtained as well as the self‐quenching rate constants and the CO (B 1Σ)) quenching rate by N2. In addition to the two‐photon laser induced fluorescence of B 1Σ+ carbon monoxide, a three‐photon resonant (2+1) ionization was observed. Laser power dependence studies indicate that ionization of the B 1Σ+ state was nearly saturated at the laser fluence used, implying that most CO (B 1Σ+) was ionized rather than fluorescing. The measured polarization ratios for circularly to linearly polarized excitation of fluorescence and ionization was much larger than the expected values suggesting that other three...
Chemical Physics Letters | 1979
J. J. Tiee; F. B. Wampler; W. W. Rice
Abstract Laser-induced fluorescence excitation spectra in the gas phase have been obtained for CCl 2 and CFCI radicals. The observed spacings in the excitation spectra reported here agree well with previous absorption work in the matrix.
Chemical Physics Letters | 1980
J. J. Tiee; F. B. Wampler; W. W. Rice
Abstract The rate constants at room temperature have been determined for the reaction of CCl, CCl 2 , and CClF radicals with various added scavengers. We have employed the technique of laser-induced fluorescence to permit the evaluation of these rate constants.
Chemical Physics Letters | 1981
J. J. Tiee; F. B. Wampler; Richard C. Oldenborg; W. W. Rice
Abstract A laser-induced fluorescence technique is used to monitor the HS radical concentration. The rate constants at room temperature have been determined for the reaction of HS radical with various added scavengers.
Chemical Physics Letters | 1983
C.R. Quick; J. J. Tiee
Abstract Laser-induced fluorescence (LIF) detection of OH radicals is used to examine the reaction of CO 2 molecules with translationally hot H atoms generated by ArF laser photolysis of HBr. Prompt formation of rotationally excited OH X 2 Πi(υ″ = 0,1,2), has been observed.
Journal of Chemical Physics | 1979
F. B. Wampler; J. J. Tiee; W. W. Rice; Richard C. Oldenborg
CF2Br2 has been irradiated at room temperature with KrF (248.4 nm) and ArF (193.3 nm) lasers. The fluorescence produced by the KrF laser irradiation appears to consist of only two ν2 progressions, v′2=6 and 5 for the CF2 (1B1−X 1A1) transition. The collision‐free lifetime of the CF2 emission was found to be 59 ns. The fluence dependence of the emission is quadratic. Upon irradiation of CF2Br2 with an ArF laser various emitting species were noted. Emission from CF(A 2Σ+–X 2Π), CF(B 2Δ–X 2Π), CF2(2B1–X 1A1), and Br2(3Πo+u–1Σ+ g) molecules was noted. Laser‐induced fluorescence excitation spectra confirmed the presence of CF2. The ArF laser fluence dependence of CF2(X 1A1) formation was found to be 1.0.
Journal of Chemical Physics | 1983
J. J. Tiee; M. J. Ferris; F. B. Wampler
The collision‐free lifetime of the v=0 level of the A 2Σ+ state of DS has been measured to be 189 ns, and that of HS has been estimated to be ∼0.5 to 2 ns. Absolute quenching rate constants of DS ( A state) by various gases have also been determined.
Journal of Chemical Physics | 1980
J. J. Tiee; F. B. Wampler; W. W. Rice
The ArF (193.3 nm) irradiation of CCl4 and CCl3F has been investigated. The laser photolysis of CCl4 yields emission from CCl (A 2Δ–X 2Π), CCl2(1B1–X 1A1), Cl2[A 3Π (0u+)–X 1Σg+], and other systems. A dye laser was used to obtain the fluorescence excitation spectrum of the CCl radical near the 0–0 band center (A 2Δ–X 2Π). The CCl (A 2Δ) radicals are formed by at least a three photon absorption process and laser fluence dependences are reported for various photofragments. The ArF laser photolysis of CCl3F yields results very similar to those of CCl4. Possible mechanistic channels are presented for both CCl4 and CCl3F photolysis which are consistent with the observed photofragments, laser fluence dependences, and known thermochemical data.
Chemical Physics Letters | 1985
C.R. Quick; J. J. Tiee; Jack M. Preses; R.E. Weston
Abstract Vacuum UV synchrotron radiation was used to produce electronically excited CF 3 radicals by photolysis of CF 3 Cl, CF 3 Br, and CF 3 I. The collision-free fluorescence lifetime of both the UV and visible emission bands of CF 3 was measured to be 14–17 ns using a time-resolved photon-counting detection system. The quenching rates of the UV and visible band emissions by CF 3 precursor molecules are (1–6) × 10 7 s −1 Torr −1 .
Chemical Physics Letters | 1979
J. J. Tiee; F. B. Wampler; W. W. Rice
Abstract The focused ArF laser irradiation of CF 2 Cl 2 at room temperature has been investigated and emission from the CF(A 2 Σ + -X 2 Π), CF(B 2 Δ-X 2 Π), and CF 2 ( 1 B 1 -X 1 A 1 ) systems has been found. Also, under conditions of a high pressure of Ar diluent, C( 1 P 1 - 1 S 0 ) emission has been noted.