scholarly journals An improved fast-response vacuum-UV resonance fluorescence CO instrument

1999 ◽  
Vol 104 (D1) ◽  
pp. 1699-1704 ◽  
Author(s):  
Christoph Gerbig ◽  
Sandra Schmitgen ◽  
Dieter Kley ◽  
Andreas Volz-Thomas ◽  
Ken Dewey ◽  
...  
2010 ◽  
Vol 10 (4) ◽  
pp. 1911-1922 ◽  
Author(s):  
M. Antiñolo ◽  
E. Jiménez ◽  
A. Notario ◽  
E. Martínez ◽  
J. Albaladejo

Abstract. The absolute rate coefficients for the tropospheric reactions of chlorine (Cl) atoms and hydroxyl (OH) radicals with CF3CH2CHO and CF3(CH2)2CHO were measured as a function of temperature (263–371 K) and pressure (50–215 Torr of He) by pulsed UV laser photolysis techniques. Vacuum UV resonance fluorescence was employed to detect and monitor the time evolution of Cl atoms. Laser induced fluorescence was used in this work for the detection of OH radicals as a function of reaction time. No pressure dependence of the bimolecular rate coefficients, kCl and kOH, was found at all temperatures. At room temperature kCl and kOH were (in 10−11 cm3 molecule−1 s−1): kCl(CF3CH2CHO) = (1.55±0.53); kCl(CF3(CH2)2CHO) = (3.39±1.38); kCl(CF3CH2CHO) = (0.259±0.050); kCl(CF3(CH2)2CHO) = (1.28±0.24). A slightly positive temperature dependence of kCl was observed for CF3CH2CHO and CF3(CH2)2CHO, and kOH(CF3CH2CHO). In contrast, kOH(CF3(CH2)2CHO) did not exhibit a temperature dependence over the range investigated. Arrhenius expressions for these reactions were: kCl(CF3CH2CHO) = (4.4±1.0)×10−11 exp{−(316±68)/T} cm3 molecule−1 s−1 kCl(CF3(CH2)2CHO) = (2.9±0.7)×10−10 exp{−(625±80)/T} cm3 molecule−1 s−1 kOH(CF3CH2CHO) = (7.8±2.2)×10−12 exp{−(314±90)/T} cm3 molecule−1 s−1 The atmospheric impact of the homogeneous removal by OH radicals and Cl atoms of these fluorinated aldehydes is discussed in terms of the global atmospheric lifetimes, taking into account different degradation pathways. The calculated lifetimes show that atmospheric oxidation of CF3(CH2)x CHO are globally dominated by OH radicals, however reactions initiated by Cl atoms can act as a source of free radicals at dawn in the troposphere.


1973 ◽  
Vol 28 (8) ◽  
pp. 1383-1384 ◽  
Author(s):  
F. Stuhl

The kinetic behavior of OH radicals was studied in the presence of a large excess of n-butane. Hydroxyl radicals were produced by pulsed vacuum-uv photolysis of H2O and were monitored directly by a resonance fluorescence method. The rate constant for the reaction OH + n-butane was determined to be 2.35 (±0.35) × 10-12 cm3 molecule-1 sec-1 at 298 °K.


1996 ◽  
Vol 101 (D22) ◽  
pp. 29229-29238 ◽  
Author(s):  
Christoph Gerbig ◽  
Dieter Kley ◽  
Andreas Volz-Thomas ◽  
Joss Kent ◽  
Ken Dewey ◽  
...  

2009 ◽  
Vol 9 (6) ◽  
pp. 24783-24814
Author(s):  
M. Antiñolo ◽  
E. Jiménez ◽  
A. Notario ◽  
E. Martínez ◽  
J. Albaladejo

Abstract. The absolute rate coefficients for the tropospheric reactions of chlorine (Cl) atoms and hydroxyl (OH) radicals with CF3CH2CHO and CF3(CH2)2CHO were measured as a function of temperature (263–371 K) and pressure (50–215 Torr of He) by pulsed UV laser photolysis techniques. Vacuum UV resonance fluorescence was employed to detect and monitor the time evolution of Cl atoms. Laser induced fluorescence was used in this work as a detection of OH radicals as a function of reaction time. No pressure dependence of the bimolecular rate coefficients, kCl and kOH, was found at all temperatures. At room temperature kCl and kOH were (in 10−11 cm3 molecule−1 s−1): kCl(CF3CH2CHO) = (1.55±0.53); kCl(CF3(CH2)2CHO) = (3.39±1.38); kOH(CF3CH2CHO) = (0.259±0.050); kOH(CF3(CH2)2CHO) = (1.28±0.24). A slightly negative temperature dependence of kCl was observed for CF3CH2CHO and CF3(CH2)2CHO, and kOH(CF3CH2CHO). In contrast, kOH(CF3(CH2)2CHO) did not exhibit a temperature dependence in the studied ranged. Arrhenius expressions for these reactions were: kCl(CF3CH2CHO) =(4.4±1.0) × 10−11 exp{−(316±68)/T} cm3 molecule−1 s−1, kCl(CF3(CH2)2CHO) = (2.9±0.7) × 10−10 exp{−625±80)/T} cm3 molecule−1 s−1, kOH(CF3CH2CHO) = (7.8±2.2) × 10−12 exp{−(314±90)/T} cm3 molecule−1 s−1. The atmospheric impact of the homogeneous removal by OH radicals and Cl atoms of these fluorinated aldehydes is discussed in terms of the global atmospheric lifetimes, taking into account different degradation pathways. The calculated lifetimes show that atmospheric oxidation of CF3(CH2)xCHO are globally dominated by OH radicals, however reactions initiated by Cl atoms can act as a source of free radicals at dawn in the troposphere.


1969 ◽  
Vol 24 (12) ◽  
pp. 1953-1958 ◽  
Author(s):  
K.H. Becker ◽  
W Groth ◽  
W Jud

AbstractThe resonance fluorescence of atomic oxygen, nitrogen, krypton, and argon was measured in the vacuum-uv region as a function of the atom concentration. In a model the calculated fluorescence intensity is approximated to the experimental dependences by variation of a single parameter k0 . The best fit to the experimental data defines k0 as effective absorption coefficient in the central part of the resonance lines. The application of the resonance fluorescence as an analytical tool for atom reactions at low pressures is discussed.


Author(s):  
M.J. Kim ◽  
L.C. Liu ◽  
S.H. Risbud ◽  
R.W. Carpenter

When the size of a semiconductor is reduced by an appropriate materials processing technique to a dimension less than about twice the radius of an exciton in the bulk crystal, the band like structure of the semiconductor gives way to discrete molecular orbital electronic states. Clusters of semiconductors in a size regime lower than 2R {where R is the exciton Bohr radius; e.g. 3 nm for CdS and 7.3 nm for CdTe) are called Quantum Dots (QD) because they confine optically excited electron- hole pairs (excitons) in all three spatial dimensions. Structures based on QD are of great interest because of fast response times and non-linearity in optical switching applications.In this paper we report the first HREM analysis of the size and structure of CdTe and CdS QD formed by precipitation from a modified borosilicate glass matrix. The glass melts were quenched by pouring on brass plates, and then annealed to relieve internal stresses. QD precipitate particles were formed during subsequent "striking" heat treatments above the glass crystallization temperature, which was determined by differential thermal analysis.


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