Infrared multiphoton dissociation of CF3Br

The CF₂, Br, and F products of 9.2 μ multiphoton dissociation of CF₃Br have been spectroscopically monitored. Primary dissociation leads to CF₃ + Br, while secondary dissociation of CF₃ leads to CF₂ + F. Both the Br and F atoms are found to have average recoil energies close to those of thermal (300 K) atoms. Comparison of these results to calculations based on RRKM theory indicates that CF₃Br dissociates from levels 2–5 photons above the CF₃ + Br threshold.     

IR multiphoton dissociation of CF3I. Pressure effect with inert and reactive gases

The IR multiphoton dissociation of CF₃I has been studied in the presence of isobutane and with isobutane and Ar and CO₂ as inert gases. The dependence of the reaction probability P(Φ) with fluence (ϕ) is confirmed. Modeling of the experimental results shows that for the energy transfer processes the average energy transferred per collision 〈†E〉_d varies with (ϕ).     

Comparative performance of CF3I,CD3I and CH3I in an atomic iodine photodissociation laser

We have compared the performance of CF₃I, CD₃I, and CH₃I in an atomic iodine photodissociation laser over the pressure range 1–200 torr. At pressures below 5 torr, CD₃I produces larger energy outputs, while above 5 torr CF₃I gives superior performance. The crossing of the laser energy output versus pressure curves is explained on the basis of collisional quenching of I(²P_{$\text{1}\text{2}$})(≡I^*) by undissociated alkyl iodide.     

Isotopic selectivity in the sensitized dissociation of SF5Cl and CF3I by multiphoton excitation of SF6

The dissociation of SF₅Cl and CF₃I sensitized by multiphoton excitation of SF₆ by a pulsed CO₂ laser has been studied versus pressure, laser fluence, inert gas and optical frequency. Isotopic effects have been observed between ³²SF₅Cl/³³SF₅Cl and between ¹³CF₃I/¹²CF₃I and selectivity factors as high as α^?1_{$\text{33}\text{32}$} = 1.57 or α_{$\text{13}\text{12}$} = 1.23 obtained.     

Real-time multiphoton ionization detection of iodine atoms produced by infrared multiphoton dissociation of perfluoroalkyl iodides

We report the direct detection of iodine atoms following infrared multiphoton dissociation of perfluoroalkyl iodides. The technique, three-photon resonant two-photon ionization, shows great promise as an actinometer for primary dissociation yield in IRMPD.     

Infrared multiphoton dissociation yields via a versatile new technique: intensity,fluence, and wavelength dependence for CF3I

Intensity, fluence, and wavelength dependence of the collisionless infrared multiphoton dissociation yield for CF₃I have been determined via “titration” of radical photoproducts and molecular-beam-sampling-mass spectrometry. The importance of nonlinear effects in the pumping of this molecule is confirmed.     

The effect of vibrational structure on multiphoton dissociation spectra of CF3Br

Results on IR multiphoton dissociation of rotationally cold CF₃Br molecules are presented and interpreted. Model calculations have been performed extending current theories and using known linear absorption data. Strong dependence of the dissociation spectra on excitation to the first discrete levels has been recognized and discussed.     

IR detection of H atoms produced by IR multiphoton dissociation

Hydrogen atoms produced by irradiation of alkenes with a focused CO₂ TEA laser react with Cl₂, forming vibrationally excited HCl, from which IR emission can be monitored. The application of this experimental technique to the study of H- atom reactions is discussed.     

Photofragmentation of CF3I in the A band

CF₃I is photodissociated in a molecular beam with 248 nm laser lighl. Fragmentation takes place into CF₃ and I(²P_3/2) or I(²P_1/2). The quantum yield for excited I (I* = I(²P_1/2)) formation is determined to be 0.92. The CF₃ fragments are found to be considerably vibrationally excited. Of the available energy in the CF₃ + I* channel 39% (0.69 eV) appears on the average as vibrational energy in the CF₃ radical. The angular distributions in both channels show predominantly parallel character. It can be concluded that at this wavelength 97% of the total absorption is due to the ³Q₀ ← ¹A₁ transition and only 3% to the ¹Q ← ¹A₁ transition. Most of the signal in the CF₃ + I channel originates from an effective crossing between the ³Q₀ and ¹Q states. A coupled channel calculation is performed to obtain a better insight into the dissociation dynamics of the CF₃I molecule. The results indicate that the CF₃ fragments from dissociation of CF₃I at 248 nm may be expected to be vibrationally excited. However, the experimental distribution has a higher average energy and is much broader. An explanation for this phenomenon is suggested.     

UV photolysis of n-C3F7I. Radiative lifetime of metastable iodine atoms

The photolysis of n-C₃F₇I and C₂F₅I has been studied with a frequency doubled dye laser at fixed frequency in the UV by detection of time resolved resonance fluorescence of the metastable iodine formed. The rate coefficient for quenching of I(²P_{$\text{1}\text{2}$}) by n-C₃F₇I has been obtained as k = (4.6 ± 0.3) × 10^?17 cm³ molecule_?1s_?1. This value is by more than an order of magnitude lower than published values. Further proof is given for the value of the radiative lifetime of the metastable atoms which was obtained recently by this experimental method. This answers questions raised by Husain et al. on this subject in this journal.     

Direct dynamics studies for the reactions of CF3CHFCF3 and CF3CF2CHF2 with H atoms

The rate constants of the hydrogen abstraction reactions of CF₃CHFCF₃ + H (R1) and CF₃CF₂CHF₂ + H (R2) have been calculated by means of the dual-level direct dynamics method. Optimized geometries and frequencies of stationary points and extra points along the minimum-energy path (MEP) are obtained at the MPW1K/6-311+G(d,p) level, and the classical energetic information is further corrected with the interpolated single-point energy (ISPE) approach by the G3(MP2) level of theory. Using the canonical variational transition state theory (CVT) with small-curvature tunneling corrections (SCT), the rate constants are evaluated over a wide temperature range of 200-2000 K. The calculated CVT/SCT rate constants are in good agreement with available experimental values. It is found that the variational effect is very small and almost negligible over the whole temperature region. However, the small-curvature tunneling correction plays an important role in the lower temperature range. Furthermore, the heats of formation of species CF₃CF₂CHF₂ (SC₁ or SC₂) and CF₃CF₂CF₂ are studied using isodesmic reactions to further elucidate the thermodynamic properties.     

Molecule coordinate frame anisotropy in dissociative photoionization of CF3I

Lifetimes of long-lived collision complexes of H⁺ + H₂ and some isotopic variants have been determined from classical trajectory calculations. A lifetime range of 0.1–50 ps could be covered, while a typical vibrational period of the complex is 10 fs. The results in agree with the expectation from RRKM theory: independence of τ of the origin of the energy of the complex (translation, vibration, or rotation), and a power law dependence of τ on E/(E + D) with exponent 2. A closer look shows a dependence of τ on total angular momentum J, which is also the main reason for non-exponential decay curves of samples for which J is not specified, and for much of the apparent dependence of τ on mass distributions. Our data show that an induction time is needed before the complex obtains its (statistical) properties.     

Thermal effects in collision-free infrared multiphoton absorption by SF6 and CF3Br

An opto-thermal molecular beam study has been carried out to investigate the multiple-photon laser excitation of SF₆ and CF₃Br. The molecular beam was produced by means of a supersonic expansion through a nozzle at variable temperature. The opto-thermal signal was measured by means of a high-sensitivity superconducting bolometer. The multiple-photon excitation of SF₆ has been measured as a function of the initial ro-vibrational population of the molecule. The experimental results have been compared with both previously published data of molecular beam and gas cell experiments and theoretical calculations. A satisfactory agreement has been found between some of our experimental results and the theoretical spectra obtained by means of the heat-bath feed-back model.     

Broadening Of The CF3I UV Absorption Spectrum BY CO2-Laser-Induced Vibrational Excitation

Absorption of CO₂ laser photons by CF₃I leads to a broadening of the CF₃I UV absorption band near 270 nm. The fwhm is increased by a factor of ≈2.3 for CO₂ laser fluence of 0.4 J/cm². Significant increase in the bandwidth is accompanied by partial decomposition of the CF₃I.     

Vergleich der trifluormethylierungseigenschaften von(CF3)Hg,CF3I und (CF3)2te am beispiel der reaktionen mit cyclohexen,benzol und pyridin

The trifluoromethylation reactions of (CF₃)₂Hg, CF₃I and (CF₃)₂Te with cyclohexene, benzene and pyridine are compared under similar conditions. Photochemical as well as thermal reactions result in an increase of the reactivity in the series (CF₃)₂Hg < CF₃I ? (CF₃)2Te. The yields and the kind of products vary depending on the time of irradiation and the temperature. In all cases the best yields are obtained from the thermal reactions with (CF₃)₂Te. With cyclohexene only trifluoromethylated addition products are observed. The substitution reactions with pyridine yield a mixture of isomeric trifluoromethylpyridines. (CF₃)₂Hg and CF₃I react with benzene to yield only benzotrifluoride C₆H₅CF₃. The main product of the reaction of (CF₃)2Te with benzene is also benzotrifluoride; in addition to this the disubstituted bis(trifluoromethyl)benzene isomers and trifluoromethyl- cyclohexadienes are formed. ¹H, ¹⁹F n.m.r. and mass spectra are described.     

Direct observation of the ν6 band in the IR spectrum of CF3I dissolved in liquid xenon

The IR spectrum of CF₃I dissolved in liquefied xenon at 185 K shows a very weak peak at 265.2 cm^?1 due to the ν₆ fundamental vibration. The separation, $\text{ν}$₃  $\text{ν}$₆, 19.3 cm^?1 is the same as that deduced from the microwave spectrum of CF₃I in the gas phase.     

The production of Te atoms by the multiphoton dissociation of diethyltelluride

Detection of Te atoms in the ground ³P^2,1,0 states has been accomplished using two-photon laser-induced fluorescence (LIF) and “2 + 1” multiphoton ionization (MPI). Te atoms were produced by multiphoton dissociation of (C₂H₅)₂Te in the region 358–395 nm. The LIF and MPI experiments utilize selective excitation of the 6p ³P_J′←5p ³P_J″ and 7p ³P_J′←5p ³P₂ transitions by two-photon absorption. Line strength intensities for the individual J′ ← J″ fine structure pairs of the 6p ³P_J′ ← 5p ³P_J″ two-photon transitions were calculated and compared to the LIF data. Intensities of these transitions of Te atoms are compared to analogous ³P ← ³P transitions in S and O atoms.     

Direct measurement of near-threshold rate constants for unimolecular dissociation of CF3I after IR multiphoton excitation

Excited-state populations of CF₃I after IR multiphoton excitation were monitored by time-resolved hot-band UV absorption spectroscopy. Using a calibration of the spectrum by shock-wave experiments, the absorption changes during the laser pulse are analyzed with respect to excited-state populations and dissociation at higher excitation energies. Dissociation of molecules near threshold is detected under collision-free conditions by absorption changes after the laser pulse. At higher pressures, absorption signals after the pulse are markedly influenced by energy transfer between excited and cold molecules. The measured dissociation rate constants near threshold are consistent with statistical calculations of k(E,J), showing pronounced rotational dependence.     

Robust synthesis of trifluoromethionine and its derivatives by reductive trifluoromethylation of amino acid disulfides by CF3I/Na/Liq.NH3 system

We disclose the reductive trifluoromethylation of chemically stable homocystine and cystine to provide corresponding trifluoromethyl ethers by the CF₃I/Na/Liq.NH₃ system. Both non-protected and protected homocystines can be nicely converted into trifluoromethylated methionines under the same condition. The method described offers a robust synthesis of pharmaceutically important trifluoromethionine, suitable for multigram synthesis. Pentafluoroethylation of homocystine was also achieved by the CF₃CF₂I/Na/Liq.NH₃ system.