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  • 1
    Electronic Resource
    Electronic Resource
    Springer
    Applied physics 38 (1985), S. 219-224 
    ISSN: 1432-0649
    Keywords: 82.30 ; 82.50
    Source: Springer Online Journal Archives 1860-2000
    Topics: Physics
    Notes: Abstract The reaction of NO2 with isobutane, induced by 488 nm laser radiation, to form 2-nitro-2-methylpropane has been investigated and the results computer-modeled according to two possible reaction mechanisms. The first scheme involves the direct abstraction of H from isobutane by vibronically excited NO2 (NO 2 *Δ ), and the second, abstraction by an intermediate NO3 radial produced by NO 2 *Δ +NO2. The modeling results strongly support the NO 2 *Δ scheme as the dominant reaction mechanism.
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 3395-3400 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photodissociation of nitromethane, CH3NO2, at 266 nm under collision-free conditions results in the single photon production of electronic ground state OH(X 2Πi). A rotational "temperature'' of 1750±50 K describes the rotational distribution of the nascent OH radical. A quantum yield of 0.004±0.001 is determined for the photolytic pathway producing the OH radical. Within experimental uncertainty, no Λ-doublet population preference was observed for OH production from H2O2, HNO3, or CH3NO2 photolysis. If a saturation correction is not utilized apparent Λ-doublet population differences are found. This incorrect saturation compensation may account for previous literature Λ-doublet population ratios, fi/ f′i, that are greater than one.
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 85 (1986), S. 4373-4376 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The reaction CH(X 2Π)+H2(arrow-right-and-left)CH2(X 3B1)+H was studied over the temperature range 372 to 675 K. Laser-induced fluorescence detection of CH radicals allowed direct determination of absolute rate constants for the forward reaction k1. The data are well fit by the Arrhenius expression k1=(2.38±0.31)×10−10 exp[−(1760±60)/T] cm3/s over the temperature range studied. A transition state theory (RRKM) calculation yields the following form for k1, k1=(5.5±1.5)×10−16 T1.79±0.04 exp[−(840±30)/T] cm3/s for the temperature range 300 to 2500 K, thus allowing cautious extrapolation to combustion temperatures. The rate constants for the reverse reaction are evaluated by utilization of the equilibrium and the forward rate constants. The data for k−1 are well fit by k−1=(4.7±0.6) ×10−10 exp[−(370±60)/T] cm3/s over the temperature range 372 to 675 K. A transition state theory calculation yields the following form for k−1, k−1=(6.4±1.1) ×10−15 T1.54±0.02 exp[(430±20)/T] cm3/s for the temperature range 300 to 2500 K. The heat of formation of CH2 at 0 K was determined to be ΔHfo {CH2}=92.6±0.5 kcal/mol, assuming that the CH2+H radical recombination reaction has no activation energy.
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 88 (1988), S. 5983-5984 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Multiphoton laser photolysis of CHBr3 and laser-induced fluorescence detection of CH(X 2Π) radicals is utilized for the direct measurement of rate constants for CH reaction with a series of cycloalkanes. Experiments are performed over the temperature range 295 to 670 K and over the pressure range 30 to 300 Torr. The following Arrhenius equations result: CH+c-C3H6, k=(5.30±0.27)×10−11 exp [(1050±40)/RT] cm3 s−1; CH+c-C5H10, k=(2.66±0.33)×10−10 exp [(400±80)/RT] cm3 s−1; CH+c-C6H12, k=(3.07±0.12)×10−10 exp [(300±30)/RT] cm3 s−1. No change in the measured rates with pressure is observed. A mechanism that involves CH radical insertion into the CH bonds on the cycloalkanes followed by rapid decomposition of the excited adduct is invoked to explain the observed kinetic behavior. A correlation of room temperature rate constant vs number of C–H bonds in the reactant is presented.
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  • 5
    Electronic Resource
    Electronic Resource
    Woodbury, NY : American Institute of Physics (AIP)
    Applied Physics Letters 64 (1994), S. 821-823 
    ISSN: 1077-3118
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Strong permanent gratings (index change Δn∼3×10−3) have been formed in bulk hydrogen treated germano-silicate glass with 242 nm exposure. Diffraction efficiencies of 6% and initial sensitivity (Δn/incident energy density) of 2×10−5 cm2/J have been obtained. The observed sensitivity is comparable to the values achieved in other holographic storage materials such as LiNbO3. It is estimated that by more uniform hydrogen loading of the sample, diffraction efficiencies of 100% can be obtained in 3 mol % GeO2 samples of only 175 μm thickness. These materials are potentially useful as fast access time (sub-μs), high capacity (∼0.8 Tbits), robust, inexpensive write-one-read-many storage media, narrow (subangstrom) linewidth optical filters, and other optical components.
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  • 6
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: We report here a direct measurement of the spatially resolved atomic hydrogen concentration profiles during hot-filament-assisted chemical-vapor deposition (HFCVD) of diamond films. The ground-state hydrogen (1s 2S1/2) atoms generated in this process are monitored by an optical four-wave-mixing technique, third-harmonic generation (THG). For THG, a 364.6 nm dye laser beam is focused into the HFCVD reactor and the third-harmonic radiation near resonant with the Lyman-α (2p 2P0j↔1s 2S1/2) transition in atomic hydrogen at 121.6 nm is observed. The resultant THG intensity and THG peak shift with respect to the Lyman-α transition are both dependent on hydrogen atom concentration. Titration experiments based on the reaction NOCl+H→HCl+NO were conducted to obtain absolute hydrogen atom concentrations from the relative concentrations determined in the THG experiment. Spatially resolved molecular hydrogen temperature and concentration profiles obtained by coherent anti-Stokes Raman scattering in a similar HFCVD reactor are reported. The observed H atom concentrations exceed computed equilibrium concentrations based on the measured gas temperatures. Transport of the atomic hydrogen from the hot filament surfaces is discussed and diffusion is shown to be the principal mechanism controlling the H atom distribution.
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  • 7
    Electronic Resource
    Electronic Resource
    [S.l.] : American Institute of Physics (AIP)
    Journal of Applied Physics 62 (1987), S. 2264-2268 
    ISSN: 1089-7550
    Source: AIP Digital Archive
    Topics: Physics
    Notes: Defect centers induced in GeO2 glass by either 100-KeV x rays at 77 K or γ rays at room temperature were studied by electron-spin resonance. The model of a singly charged oxygen vacancy defect center for the Ge E' center (g(parallel) =2.0012, g⊥ =1.9945) was confirmed by the observation and computer simulation of the 73Ge hyperfine structure associated with this center. The evolutions of the Ge E', peroxy radical, and nonbridging oxygen hole centers were studied by isochronal thermal annealing. Surprisingly, the Ge(2) center, a defect previously known only in Ge-doped silica, and an additional center with a hyperfine coupling constant half that of the Ge E' center were found in pure GeO2 samples irradiated at 77 K; these, too, were studied by isochronal thermal annealing and computer simulation. Structural models for these centers are presented.
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  • 8
    ISSN: 1572-9591
    Source: Springer Online Journal Archives 1860-2000
    Topics: Energy, Environment Protection, Nuclear Power Engineering
    Notes: Abstract The formation of palladium hydride and deuteride by electrolysis has been studied with high precision calorimetry using sealed cells within-situ recombination of gaseous products as well as open cells. Palladium electrodes prepared by different methods were studied. With sealed cells of our design in the heat flow isothermal calorimeter, the uncertainies associated with the gas evolution, evaporation, entrainment, and side reactions were effectively eliminated. No unexpected excess heat was observed within energy balance error of about 2%.
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  • 9
    Electronic Resource
    Electronic Resource
    New York, NY : Wiley-Blackwell
    International Journal of Chemical Kinetics 21 (1989), S. 765-774 
    ISSN: 0538-8066
    Keywords: Chemistry ; Physical Chemistry
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Pulsed laser photolysis/laser-induced fluorescence (LIF) is utilized to measure absolute rate constants of CH radical reactions as a function of temperature and pressure. Multiphoton dissociation of CHBr3 at 266 nm is employed for the generation of CH (X2Π) radicals. The CH radical relative concentration is monitored by exciting fluorescence on the R1(2) line of the (A2Δ - X2Π) transition at 429.8 nm. A resistively heated cell allows temperature studies to be performed from room temperature to ≈670 K. The following Arrhenius equations are derived: \documentclass{article}\pagestyle{empty}\begin{document}$${\rm CH}\,{\rm + }\,{\rm N}_{\rm 2} {\rm O,}\,\,\,\,\,\,\,\,k = (1.59 \pm 0.20)\, \times \,\,10^{ - 11} \,\,\exp [(500 \pm 45)/T]{\rm cm}^{\rm 3} {\rm s}^{{\rm - 1}};$$\end{document} \documentclass{article}\pagestyle{empty}\begin{document}$${\rm CH}\,{\rm + }\,{\rm SO}_{\rm 2} {\rm ,}\,\,\,\,\,\,\,\,k = (1.32 \pm 0.17)\, \times \,\,\,10^{ - 10} \,\,\exp [(250 \pm 45)/T]\,\,{\rm cm}^{\rm 3} {\rm s}^{{\rm - 1}};$$\end{document} \documentclass{article}\pagestyle{empty}\begin{document}$${\rm CH}\,{\rm + }\,{\rm OCS,}\,\,\,\,\,\,\,\,k = (1.99 \pm 0.11)\, \times \,\,\,10^{ - 10} \,\,\exp [(190 \pm 20)/T]\,\,{\rm cm}^{\rm 3} {\rm s}^{{\rm - 1}};$$\end{document} \documentclass{article}\pagestyle{empty}\begin{document}$${\rm CH}\,{\rm + }\,{\rm CS}_{\rm 2} {\rm ,}\,\,\,\,\,\,\,\,k = (3.49 \pm 0.36)\, \times \,\,\,10^{ - 10} \,\,\exp [- (40 \pm 35)/T]\,\,{\rm cm}^{\rm 3} {\rm s}^{{\rm - 1}};$$\end{document} \documentclass{article}\pagestyle{empty}\begin{document}$${\rm CH}\,{\rm + }\,{\rm SF}_{\rm 6} {\rm ,}\,\,\,\,\,\,\,\,k 〈 5\,\,\, \times \,\,\,10^{ - 17} {\rm cm}^{\rm 3} {\rm s}^{{\rm - 1}} .$$\end{document} With the exception of SF6, the reactions of sulfur containing species proceed at rates that are near the theoretical gas kinetic collision frequency. Additionally, these reactions all have activation energies that are near zero or slightly negative. These observations are consistent with an insertion-decomposition mechanism being dominant under these conditions.
    Additional Material: 3 Ill.
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  • 10
    Electronic Resource
    Electronic Resource
    New York, NY : Wiley-Blackwell
    International Journal of Chemical Kinetics 20 (1988), S. 117-129 
    ISSN: 0538-8066
    Keywords: Chemistry ; Physical Chemistry
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Absolute rate constants are measured for the reactions: OH + CH2O, over the temperature range 296-576 K and for OH + 1,3,5-trioxane over the range 292-597 K. The technique employed is laser photolysis of H2O2 or HNO3 to produce OH, and laser-induced fluorescence to directly monitor the relative OH concentration. The results fit the following Arrhenius equations: k (CH2O) = (1.66 ± 0.20) × 10-11 exp[-(170 ± 80)/RT] cm3 s-1 and k(1,3,5-trioxane) = (1.36 ± 0.20) × 10-11 exp[-(460 ± 100)/RT] cm3 s-1. The transition-state theory is employed to model the OH + CH2O reaction and extrapolate into the combustion regime. The calculated result covering 300 to 2500 K can be represented by the equation: k(CH2O) = 1.2 × 10-18 T2.46 exp(970/RT) cm3 s-1. An estimate of 91 ± 2 kcal/mol is obtained for the first C—H bond in 1,3,5-trioxane by using a correlation of C—H bond strength with measured activation energies.
    Additional Material: 4 Ill.
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