Cavity Ring-down Study of the Visible Absorption Spectrum of the Phenyl Radical and Kinetics of Its Reactions with Cl, Br, Cl2, and O2

Cavity ring-down spectroscopy coupled with pulsed laser photolysis was used to study the visible absorption spectrum (490−535 nm, 2B1 ← 2A1 transition) of the phenyl radical, C6H5, in 10−50 Torr of argon diluent at 298 K. Absorption cross-sections were independent of total pressure over the range st...

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Veröffentlicht in:The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory Molecules, spectroscopy, kinetics, environment, & general theory, 2002-06, Vol.106 (24), p.5908-5917
Hauptverfasser: Tonokura, K, Norikane, Y, Koshi, M, Nakano, Y, Nakamichi, S, Goto, M, Hashimoto, S, Kawasaki, M, Sulbaek Andersen, M. P, Hurley, M. D, Wallington, T. J
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container_issue 24
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container_title The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, & general theory
container_volume 106
creator Tonokura, K
Norikane, Y
Koshi, M
Nakano, Y
Nakamichi, S
Goto, M
Hashimoto, S
Kawasaki, M
Sulbaek Andersen, M. P
Hurley, M. D
Wallington, T. J
description Cavity ring-down spectroscopy coupled with pulsed laser photolysis was used to study the visible absorption spectrum (490−535 nm, 2B1 ← 2A1 transition) of the phenyl radical, C6H5, in 10−50 Torr of argon diluent at 298 K. Absorption cross-sections were independent of total pressure over the range studied. At 504.8 nm, σphenyl = (3.6 ± 1.6) × 10-19 cm2 molecule-1 (base e). Spectral simulation of the rotational structure of an origin band was performed using a model for a type C vibronic band. The vibronic spectrum was analyzed using normal-mode information from quantum chemical calculations employing hybrid density functional theory (B3LYP/aug-cc-pVDZ). The a1 and b1 vibrations were confirmed in the vibronic spectrum. Cavity ring-down spectroscopy was used to follow the loss of phenyl radicals and measure k(C6H5+Cl) = (1.2 ± 0.8) × 10-10, k(C6H5+Br) = (7.0 ± 4.0) × 10-11, and k(C6H5+Cl2) = (2.96 ± 0.53) × 10-11 at 298K, and k(C6H5+Cl2) = ( ) × 10-12 exp[(1000 ± 470)/T] cm3 molecule-1 s-1. Relative rate techniques were used to measure k(C6H5+Cl2)/k(C6H5+O2) = 2.1 ± 0.4 in 10−700 Torr of N2 diluent at 296K. Combining the absolute and relative rate data gives k(C6H5+O2) = (1.4 ± 0.4) × 10-11 cm3 molecule-1 s-1. In 1 atm of air C6H5 radicals have a lifetime of approximately 1.4 × 10-8 s with respect to reaction with O2 to give C6H5O2 radicals. Results are discussed with respect to the spectroscopy and reactivity of C6H5 radicals. Quoted uncertainties are 2 standard deviations from regression analyses.
doi_str_mv 10.1021/jp025585t
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P ; Hurley, M. D ; Wallington, T. J</creator><creatorcontrib>Tonokura, K ; Norikane, Y ; Koshi, M ; Nakano, Y ; Nakamichi, S ; Goto, M ; Hashimoto, S ; Kawasaki, M ; Sulbaek Andersen, M. P ; Hurley, M. D ; Wallington, T. J</creatorcontrib><description>Cavity ring-down spectroscopy coupled with pulsed laser photolysis was used to study the visible absorption spectrum (490−535 nm, 2B1 ← 2A1 transition) of the phenyl radical, C6H5, in 10−50 Torr of argon diluent at 298 K. Absorption cross-sections were independent of total pressure over the range studied. At 504.8 nm, σphenyl = (3.6 ± 1.6) × 10-19 cm2 molecule-1 (base e). Spectral simulation of the rotational structure of an origin band was performed using a model for a type C vibronic band. The vibronic spectrum was analyzed using normal-mode information from quantum chemical calculations employing hybrid density functional theory (B3LYP/aug-cc-pVDZ). The a1 and b1 vibrations were confirmed in the vibronic spectrum. Cavity ring-down spectroscopy was used to follow the loss of phenyl radicals and measure k(C6H5+Cl) = (1.2 ± 0.8) × 10-10, k(C6H5+Br) = (7.0 ± 4.0) × 10-11, and k(C6H5+Cl2) = (2.96 ± 0.53) × 10-11 at 298K, and k(C6H5+Cl2) = ( ) × 10-12 exp[(1000 ± 470)/T] cm3 molecule-1 s-1. Relative rate techniques were used to measure k(C6H5+Cl2)/k(C6H5+O2) = 2.1 ± 0.4 in 10−700 Torr of N2 diluent at 296K. Combining the absolute and relative rate data gives k(C6H5+O2) = (1.4 ± 0.4) × 10-11 cm3 molecule-1 s-1. In 1 atm of air C6H5 radicals have a lifetime of approximately 1.4 × 10-8 s with respect to reaction with O2 to give C6H5O2 radicals. Results are discussed with respect to the spectroscopy and reactivity of C6H5 radicals. 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P</creatorcontrib><creatorcontrib>Hurley, M. D</creatorcontrib><creatorcontrib>Wallington, T. J</creatorcontrib><title>Cavity Ring-down Study of the Visible Absorption Spectrum of the Phenyl Radical and Kinetics of Its Reactions with Cl, Br, Cl2, and O2</title><title>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</title><addtitle>J. Phys. Chem. A</addtitle><description>Cavity ring-down spectroscopy coupled with pulsed laser photolysis was used to study the visible absorption spectrum (490−535 nm, 2B1 ← 2A1 transition) of the phenyl radical, C6H5, in 10−50 Torr of argon diluent at 298 K. Absorption cross-sections were independent of total pressure over the range studied. At 504.8 nm, σphenyl = (3.6 ± 1.6) × 10-19 cm2 molecule-1 (base e). Spectral simulation of the rotational structure of an origin band was performed using a model for a type C vibronic band. The vibronic spectrum was analyzed using normal-mode information from quantum chemical calculations employing hybrid density functional theory (B3LYP/aug-cc-pVDZ). The a1 and b1 vibrations were confirmed in the vibronic spectrum. Cavity ring-down spectroscopy was used to follow the loss of phenyl radicals and measure k(C6H5+Cl) = (1.2 ± 0.8) × 10-10, k(C6H5+Br) = (7.0 ± 4.0) × 10-11, and k(C6H5+Cl2) = (2.96 ± 0.53) × 10-11 at 298K, and k(C6H5+Cl2) = ( ) × 10-12 exp[(1000 ± 470)/T] cm3 molecule-1 s-1. Relative rate techniques were used to measure k(C6H5+Cl2)/k(C6H5+O2) = 2.1 ± 0.4 in 10−700 Torr of N2 diluent at 296K. Combining the absolute and relative rate data gives k(C6H5+O2) = (1.4 ± 0.4) × 10-11 cm3 molecule-1 s-1. In 1 atm of air C6H5 radicals have a lifetime of approximately 1.4 × 10-8 s with respect to reaction with O2 to give C6H5O2 radicals. Results are discussed with respect to the spectroscopy and reactivity of C6H5 radicals. 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A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Tonokura, K</au><au>Norikane, Y</au><au>Koshi, M</au><au>Nakano, Y</au><au>Nakamichi, S</au><au>Goto, M</au><au>Hashimoto, S</au><au>Kawasaki, M</au><au>Sulbaek Andersen, M. P</au><au>Hurley, M. D</au><au>Wallington, T. J</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Cavity Ring-down Study of the Visible Absorption Spectrum of the Phenyl Radical and Kinetics of Its Reactions with Cl, Br, Cl2, and O2</atitle><jtitle>The journal of physical chemistry. A, Molecules, spectroscopy, kinetics, environment, &amp; general theory</jtitle><addtitle>J. Phys. Chem. A</addtitle><date>2002-06-20</date><risdate>2002</risdate><volume>106</volume><issue>24</issue><spage>5908</spage><epage>5917</epage><pages>5908-5917</pages><issn>1089-5639</issn><eissn>1520-5215</eissn><abstract>Cavity ring-down spectroscopy coupled with pulsed laser photolysis was used to study the visible absorption spectrum (490−535 nm, 2B1 ← 2A1 transition) of the phenyl radical, C6H5, in 10−50 Torr of argon diluent at 298 K. Absorption cross-sections were independent of total pressure over the range studied. At 504.8 nm, σphenyl = (3.6 ± 1.6) × 10-19 cm2 molecule-1 (base e). Spectral simulation of the rotational structure of an origin band was performed using a model for a type C vibronic band. The vibronic spectrum was analyzed using normal-mode information from quantum chemical calculations employing hybrid density functional theory (B3LYP/aug-cc-pVDZ). The a1 and b1 vibrations were confirmed in the vibronic spectrum. Cavity ring-down spectroscopy was used to follow the loss of phenyl radicals and measure k(C6H5+Cl) = (1.2 ± 0.8) × 10-10, k(C6H5+Br) = (7.0 ± 4.0) × 10-11, and k(C6H5+Cl2) = (2.96 ± 0.53) × 10-11 at 298K, and k(C6H5+Cl2) = ( ) × 10-12 exp[(1000 ± 470)/T] cm3 molecule-1 s-1. Relative rate techniques were used to measure k(C6H5+Cl2)/k(C6H5+O2) = 2.1 ± 0.4 in 10−700 Torr of N2 diluent at 296K. Combining the absolute and relative rate data gives k(C6H5+O2) = (1.4 ± 0.4) × 10-11 cm3 molecule-1 s-1. In 1 atm of air C6H5 radicals have a lifetime of approximately 1.4 × 10-8 s with respect to reaction with O2 to give C6H5O2 radicals. Results are discussed with respect to the spectroscopy and reactivity of C6H5 radicals. Quoted uncertainties are 2 standard deviations from regression analyses.</abstract><pub>American Chemical Society</pub><doi>10.1021/jp025585t</doi><tpages>10</tpages></addata></record>
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