A R T I C L E S
Kwok et al.
(Spectra-Physics, Spitfire) pumped by the second harmonic from a Nd:
YLF laser (Spectra-Physics, Evolution X) amplified the seed laser beam,
and the output from the regenerative amplifier (800 nm, 1ps, 1 kHz)
was frequency doubled and tripled by KDP crystals to generate the
probe (400 nm) and pump (267 nm) laser sources, respectively. The
time zero delay between the pump and probe laser beams in the TR3
experiments was found by using fluorescence depletion of trans-
stilbene. The time zero was ascertained by varying the optical delay
between the pump and probe beams to a position where the depletion
of the stilbene fluorescence was halfway to the maximum fluorescence
depletion by the probe laser. The accuracy of the time zero measurement
was estimated to be (0.5 ps, and a typical cross-correlation time
between the pump and probe pulses was also measured by the
fluorescence depletion method and determined to be about 1.5 ps
(fwhm). So as to employ the laser beams more effectively in the TR3
experiments and taking into account that the rotational reorientation
dynamics are much faster than the dynamics investigated in this study,
parallel polarization of the pump and probe laser beams was employed
rather than the magic angle polarization. The pump and probe pulses
were loosely focused onto a thin film stream (thickness ∼500 µm) of
the sample solution where typical pulse energies and spot sizes at the
sample for the pump beam were 15 µJ and 250 µm and for the probe
beam were 8 µJ and 150 µm. A backscattering geometry using an
ellipsoidal mirror with f/1.4 was employed to collect the Raman
scattered light and image the light onto the entrance slit of a 0.5 m
spectrograph. The 1200 groove/mm ruled grating blazed at 250 nm of
the spectrograph dispersed the Raman scattered light onto a liquid
nitrogen cooled CCD detector mounted on the exit port of the
spectrograph.
Each spectrum shown here was obtained from subtraction of scaled
probe-before-pump and scaled net solvent measurements from a pump-
probe spectrum to delete CHBr3 ground-state Raman bands and residual
solvent Raman bands, respectively. The known Raman shifts of the
solvent Raman bands were used to calibrate the spectra with an
estimated accuracy of (5 cm-1 in absolute frequency. Commercially
available 99% CHBr3 and spectroscopic grade acetonitrile solvent were
used without further purification to make half-liter volume CHBr3 (8
× 10-2 mol dm-3) samples prepared in acetonitrile and acetonitrile/
water (0.2%, 1%, 2%, 5%) mixed solvents. During the experimental
trials, the samples showed less than a few percent degradation as
determined from the UV absorption spectra obtained before and after
the TR3 measurement.
photon has about 113 kcal/mol of energy and is thus only likely
to break one carbon-halogen bond in the CHBr3, CHBr2Cl,
and CHCl2Br molecules following 253.7 nm excitation. How
does the 253.7 nm photolysis of low concentrations of CHBr3,
CHBr2Cl, and CHCl2Br in water lead to complete conversion
of the halogen atoms into bromide and/or chloride ion products,
and where does the energy come from to break all three carbon-
halogen bonds? Here, we present a combined experimental and
theoretical study of the photochemistry of CHBr3 in pure water
and in acetonitrile/water mixed solvents. This work elucidates
the reactions and mechanisms responsible for the photochemical
conversion of the halogen atoms in CHBr3 into three bromide
ions in water solution.
Experimental and Computational Methods
Photochemistry and Product Analysis Experiments. Ultraviolet/
Visible Absorption and pH Measurements after Photolysis of CHBr3
in Water. Commercially available CHBr3 (99%) and deionized water
were used to prepare 500 mL sample solutions of about 9 × 10-5
M
CHBr3 in water. The sample solution was put in a 10 cm laser path-
length glass holder with quartz windows and was excited by 3 mJ of
240 nm unfocused laser beam from the first anti-Stokes hydrogen
Raman shifted laser line of the fourth harmonic of a nanosecond-Nd:
YAG laser in the photolysis experiments. The absorption spectra for
the photolyzed samples were acquired by employing a 1 cm UV grade
cell and a Perkin-Elmer Lambda 19 UV/vis spectrometer. The pH of
the photolyzed samples was measured by using a ThermoOrion 420A
pH meter equipped with a 8102BN combination pH electrode. The pH
electrode was calibrated with 7.00 pH and 4.01 pH buffer solutions.
13C NMR Measurements after 240 nm Photolysis of CHBr3 in
Water. Commercially available 13CHBr3 (Aldrich) and D2O (99.9%
D) solvent were used to prepare ∼20 mM sample solutions which were
placed in a UV-grade airtight NMR tube for the photolysis experiments.
13C NMR spectra were acquired using a Bruker Advance 400 DPX
spectrometer at room temperature. An initial 13C NMR spectrum was
obtained for the sample before photolysis, and additional spectra were
obtained after varying times following excitation by the 240 nm
unfocused laser beam until all of the 13CHBr3 sample was photolyzed
as determined by the decrease in its 13C NMR band at ∼12 ppm
referenced to the TMS band that was set as 0 ppm.
Ab Initio Calculations. The second-order Møller-Plesset perturba-
tion theory (MP2) was employed to examine the water-assisted O-H
insertion reactions of isobromoform (BrCHBr-Br) + nH2O f CHBr2-
(OH) + HBr + (n - 1)H2O (where n ) 1,2,3), and the decomposition
reactions of CHBr2(OH) + nH2O f HBrCO + nH2O + HBr (n )
0,1,2,3,4) and HBrCO + nH2O f CO + HBr + nH2O (n ) 0,1,2,...,4).
Both the geometry optimization and the frequency calculations were
done with the 6-31G* basis set for C, H, O, and Br atoms. MP2
calculations using a 6-311++G** basis set were also done to find the
optimized geometry, vibrational frequencies, and relative Raman
intensities for the CHBr2OH molecule. All of the calculations made
use of the Gaussian 98W program suite.28 Cartesian coordinates, total
energies, and selected output from the calculations for all of the
calculated structures shown in Figures 4-6 are given in the Supporting
Infrared (IR) Absorption Measurements after 240 nm Photolysis
of CHBr3 in Water. The evolution of gas was observed in both of the
photochemistry experiments described in parts 1 and 2 above. This
gas was collected and introduced into a 10 cm path-length IR gas cell
equipped with KBr windows. IR spectra of the gas obtained after
photolysis of CHBr3 in water were obtained using a Bio-Rad FTS 165
spectrometer.
We attempted to estimate the photoquantum yield for the photolysis
reaction of CHBr3 in water to produce 3Br- (e.g., 3HBr that dissociate
to 3H+ and 3Br- in water). The same setup as for the UV/vis absorption
measurements described above and a laser power meter to measure
the laser beam exciting the sample solution were used to make the
experimental measurements needed to estimate the photoquantum yield.
The equations given in the Supporting Information were used to find
the estimate of the photoquantum yield for production of the 3HBr
leaving groups.
(28) Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Scuseria, G. E.; Robb, M.
A.; Cheeseman, J. R.; Zakrzewski, V. G.; Montgomery, J. A., Jr.; Stratmann,
R. E.; Burant, J. C.; Dapprich, S.; Millam, J. M.; Daniels, A. D.; Kudin,
K. N.; Strain, M. C.; Farkas, O.; Tomasi, J.; Barone, V.; Cossi, M.; Cammi,
R.; Mennucci, B.; Pomelli, C.; Adamo, C.; Clifford, S.; Ochterski, J.;
Petersson, G. A.; Ayala, P. Y.; Cui, Q.; Morokuma, K.; Malick, D. K.;
Rabuck, A. D.; Raghavachari, K.; Foresman, J. B.; Cioslowski, J.; Ortiz,
J. V.; Baboul, A. G.; Stefanov, B. B.; Liu, G.; Liashenko, A.; Piskorz, P.;
Komaromi, I.; Gomperts, R.; Martin, R. L.; Fox, D. J.; Keith, T.; Al-Laham,
M. A.; Peng, C. Y.; Nanayakkara, A.; Gonzalez, C.; Challacombe, M.;
Gill, P. M. W.; Johnson, B.; Chen, W.; Wong, M. W.; Andres, J. L.;
Gonzalez, C.; Head-Gordon, M.; Replogle, E. S.; Pople, J. A. Gaussian
98; Gaussian, Inc.: Pittsburgh, PA, 1998.
Picosecond Time-Resolved Resonance Raman (ps-TR3) Experi-
ments. A femtosecond mode-locked Ti:Sapphire laser (Spectra-Physics,
Tsunami) pumped by the second harmonic from a Nd:YVO4 laser
(Spectra-Physics, Millennia V) was employed as the seed beam for an
amplified laser system. A picosecond mode regenerative amplifier
(27) McGivern, W. S.; Sorkhabi, O.; Suits, A. G.; Derecskei-Kovacs, A.; North,
S. W. J. Phys. Chem. A 2000, 104, 10085-10091.
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3120 J. AM. CHEM. SOC. VOL. 126, NO. 10, 2004