Library

feed icon rss

Your email was sent successfully. Check your inbox.

An error occurred while sending the email. Please try again.

Proceed reservation?

Export
Filter
  • Articles: DFG German National Licenses  (82)
Source
  • Articles: DFG German National Licenses  (82)
Material
Keywords
  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 98 (1994), S. 11969-11977 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 99 (1995), S. 12188-12194 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 87 (1987), S. 7050-7058 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A tunable pulsed dye laser was used to pump OD to the (A 2∑+,v′=1) level. The fluorescence excitation spectrum of OD in the wavelength region 287.26–290.03 nm in the A→X system was recorded. The rate coefficients for quenching of OD (A 2∑+) from v′=0 and v′=1 levels by O2, N2, air, and SF6 were measured. The rate coefficient for vibrational relaxation of OD (A 2∑+) from v′=1 to v′=0 level was separated from the overall rate coefficient for quenching of OD (A 2∑+) from v′=1 level to the ground (X 2Π) state for the above four gases. The rate coefficients for quenching of OD (A 2∑+) from v′=0 level to the ground (X 2Π) state by 15 common gases were measured by using excess SF6 to rapidly quench the OD (A 2∑+) from v′=1 to v′=0 level. All measurements were carried out in excess helium and are for rotationally thermalized OD (A 2∑+) radicals.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 84 (1986), S. 1349-1354 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Time resolved resonance fluorescence detection of O(3P) and H(2S) has been employed in conjunction with pulsed laser photolysis of O3/HX/He mixtures to determine absolute rate coefficients and product yields for reactions of O(1D) with HCl(1) and HBr(2) at 297 K. Total rate coefficients for O(1D) removal are found to be, in units of 10−10 cm3 molecule−1 s−1, k1=1.50±0.18 and k2=1.48±0.16, where the quoted errors are 2σ and represent precision only. The absolute accuracy of these rate coefficients is estimated to be ±20%. Formation of O(3P)+HX is found to account for 9%±5% of the overall rate of reaction (1) and 20%±7% of the overall rate of reaction (2). Formation of H(2S)+XO is found to account for 24%±5% of the overall rate of reaction (1) but 〈4.5% of the overall rate of reaction (2). By difference, the OH+X(2P) channel accounts for 67%±10% of the overall rate of reaction (1) and 80%±12% of the overall rate of reaction (2).
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 83 (1985), S. 447-448 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Rate coefficients for the reaction OH+HBr → Br+H2O have been measured at 298 K using two different experimental techniques: (1) 266 nm pulsed laser photolysis of O3/H2O/HBr/He mixtures followed by time resolved resonance fluorescence detection of OH (LFP-RF) and (2) 248 nm pulsed laser photolysis of H2O2/HBr/Ar mixtures followed by pulsed laser induced fluorescence detection of OH (LFP-LIF). In both sets of experiments, the HBr concentration was monitored in situ in the slow flow system by UV photometry. Measured rate coefficients in units of 10−12 cm3 molecule−1 s−1 are 11.4±0.3 (LFP-RF) and 10.7±0.3 (LFP-LIF) where the uncertainties are 2σ and represent precision only. The absolute accuracy of the results is estimated to be ±10%. The experimental k1 values are in good agreement with a previous LFP-RF study in our laboratory but significantly faster than values reported by several other groups.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 5878-5886 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The primary quantum yields of OH(X 2Π),H(2S), and oxygen atoms [O(1D)+O(3P)] produced in the photodissociation of H2O2 at 193 and 222 nm have been measured at 298 K. At 193 nm, the primary quantum yields were observed to be 1.51±0.18, 0.16±0.04, and 〈0.02, for Φ(OH), Φ(H), and the sum of Φ(O) and Φ(O 1S), respectively. At 222 nm, the OH yield was Φ(OH)=2.02±0.35, the H atom yield was Φ(H)=0.024±0.012, and Φ(O) was 〈0.002. The errors quoted above are 2σ, precision plus estimated systematic errors. The OH product was directly monitored by pulsed laser-induced fluorescence, and the atomic species were detected via cw resonance fluorescence. The OH quantum yields reported here were measured relative to known product quantum yields in the dissocation of H2O2 at 248 nm. H(2S) yields were measured relative to those in photolysis of HBr and HCl, (at 193 nm) or CH3SH (at 222 nm), whereas O atoms yields were measured relative to O3 photolysis at both wavelengths. The present results indicate unit dissociation of H2O2 at both 222 and 193 nm with only two major products OH (∼80% at 193 nm, 98% at 222 nm) and H(2S) (∼20% at 193 nm, 2% at 222 nm). Up to 15% of the OH produced in the 193 nm photolysis may be vibrationally excited; however, no evidence for vibrationally excited OH was observed at 222 nm.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 92 (1990), S. 996-1003 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The quantum yields of the products, OH(X 2Π), O(3P) [plus O(1D)] and H(2S), in the photolysis of H2O2 and CH3OOH at 248 nm and 298 K have been measured. OH was directly observed by laser-induced fluorescence while the atomic species were detected by cw-resonance fluorescence. All quantum yield measurements were made using relative methods. The quantum yields of OH, O, and H in H2O2 photolysis were measured relative to the well known quantum yields of O(1D) and O(3P) in the photodissociation of O3, and H(2S) in CH3SH. The values we obtain are, 2.09±0.36, 〈0.002 and 〈0.0002 for OH, O, and H, respectively. For CH3OOH photolysis, the quantum yield of OH was measured relative to our value for OH quantum yield in H2O2 photolysis, and the quantum yields of O and H relative to those in O3 and CH3SH photodissociation, respectively. The values we obtain are, 1.00±0.18, 〈0.007 and 0.038±0.007 for OH, O, and H, respectively. In both H2O2 and CH3OOH photolysis, the observed O and H quantum yields showed an apparent dependence on the fluence of the photolysis light, the possible origin of which is discussed. The large quantum yield of OH we measure is consistent with the known continuous and unstructured absorption spectra of these molecules in this wavelength region, where the most important process is the dissociative (A˜ 1A←X˜ 1A) transition to give OH(X 2Π, v‘=0) fragment.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 5887-5895 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The quantum yields for OH, O(3P), O(1D), and H(2S) from the photolysis of HNO3 have been determined at 248, 222, and 193 nm at 298 K. The quantum yield for OH was observed to be near unity at 248 [Φ(OH)=0.95±0.09] and 222 nm [Φ(OH)=0.90±0.11]. However, at 193 nm the quantum yield for OH was found to be 0.33±0.06. The quantum yield for O atoms [O(3P)+O(1D)], Φ(O), was observed to be 0.031±0.010, 0.20±0.03, 0.81±0.13, at 248, 222, and 193 nm, respectively. Both O(3P) and O(1D) were observed at 222 and 193 nm, but only O(3P) was detected at 248 nm. It was observed that 40% of the O atoms formed at both 193 and 222 nm were O(1D) atoms. The upper limits for H(2S) quantum yields: Φ(H)≤0.002 at 248 nm, ≤0.01 at 222 nm, and ≤0.012 at 193 nm were also determined. This present work quantifies the photolysis channel producing HONO+O and show that it accounts for a large fraction at HNO3 photolysis at 193 nm.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 96 (1992), S. 8194-8201 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The primary quantum yields, ΦBr, for the formation of Br atom in the photodissociation of CF2Br2 and CH3Br at 248, 222, and 193 nm, and of CF3Br at 222 and 193 nm were measured at 298 K. The bromine atoms were directly detected via resonance fluorescence following pulsed laser photolysis of the molecules of interest. The Br atom quantum yields in CF2Br2 photolysis increased with decreasing wavelengths: 1.01±0.15, 1.63±0.19, and 1.96±0.27 at 248, 222, and 193 nm, respectively. The ΦBr values in CH3Br and CF3Br were close to unity at all the wavelengths: 0.92±0.15 and 1.12±0.16 at 222 and 193 nm, respectively, for CF3Br; 1.01±0.16, 1.10±0.20, and 1.05±0.11 at 248, 222, and 193 nm, respectively, for CH3Br. Quantum yield of H atom formation in the photolysis of CH3Br at 193 nm was measured to be 0.002±0.001. H atom could not be detected in the photolysis at 248 and 222 nm. In all cases the ΦBr values were found to be independent of buffer gas pressure or the photolysis laser fluence. Our results suggest that the quantum yields for dissociation of all the molecules considered here are unity; therefore, atmospheric lifetime calculations carried out by assuming a unit dissociation quantum yield are correct. The nature of the photodissociation process is discussed in the light of previous and present results.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 95 (1991), S. 3244-3251 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The quantum yields for the formation of O(1D) and O(3P) from the photolysis of ozone have been measured at 222 and 193 nm. The quantum yield for O(3P) was observed to be Φ(3P)=0.13±0.02 at 222 nm, and the primary quantum yield for O(1D) was found to be Φ(1D)=0.87±0.04. This measurement is consistent with other studies of O3 photolysis within the Hartley band which indicate that a significant portion (5–15%) of the products are formed in the ground state. At 193 nm the quantum yield for the production of excited state O(1D) atoms is Φ(1D)=0.46±0.29, which is significantly less than what is observed during photolysis within the lower energy Hartley band. The quantum yield for O(3P) atoms at 193 nm was found to be 0.57±0.14. We have also observed that the quantum yield for O atoms [O(1D)+O(3P)] is greater than unity [Φ(O)=1.20±0.15] at 193 nm indicating the presence of a channel which produces three O(3P) atoms. O2(b 1Σ) has also been detected and quantified, Φ(b 1Σ)=0.50±0.38, from O3 photolysis at 193 nm. These measurements suggest that O(1D) and O2(b1Σ) are co-produced.
    Type of Medium: Electronic Resource
    Library Location Call Number Volume/Issue/Year Availability
    BibTip Others were also interested in ...
Close ⊗
This website uses cookies and the analysis tool Matomo. More information can be found here...