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  • 1
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 90 (1989), S. 5930-5935 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The dimeric ClO has been generated in a gaseous discharge–flow system at 220 K and 10–30 Torr by reacting atomic Cl with O3, ClOCl or OClO, and reacting atomic O with ClOCl or OClO, in a stream of Ar. The gas mixture in the flow tube was sampled through a pinhole and condensed on a CsI window maintained at 12 K. The infrared absorption spectrum of the matrix formed after 30–120 min deposition was then recorded. Absorption lines at 752.6, 649.8, and 647.6 cm−1 have been assigned to ClOOCl, and previous assignments for dimeric ClO seem to be in error. The results are in excellent agreement with recent ab initio calculations. Under our experimental conditions, no other isomer of Cl2O2 was observed.
    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 114 (2001), S. 4817-4823 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: A photoionization-efficiency spectrum of CH3SCH2Cl was measured over the wavelength range 108–142 nm by means of a photoionization mass spectrometer coupled to a synchrotron as the source of radiation. Gaseous CH3SCH2Cl was generated in a discharge-flow reactor involving Cl, Cl2, and CH3SCH3 at room temperature via these sequential reactions: Cl+CH3SCH3→CH3SCH2+HCl; CH3SCH2+Cl2→CH3SCH2Cl+Cl. According to the PIE spectrum of CH3SCH2Cl thus obtained, the ionization energy is (9.077±0.007) eV. Based on GAUSSIAN-2 calculations, the observed ionization of CH3SCH2Cl near the threshold region is likely to form from singlet CH3SCH2Cl ionizing to doublet CH3SCH2Cl+; the calculated ionization energy 9.064 eV agrees with the experimental value. The adiabatic ionization energy of CH3SCH2 and appearance energy of CH3SCH2+ from CH3SCH2Cl were determined to be (6.884±0.008) eV and (10.007±0.016) eV, respectively; the dissociation energy of the CH3SCH2–Cl bond is thus derived to be (72.0±0.6) kcal mol−1. © 2001 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 3
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 117 (2002), S. 1633-1640 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Absorption cross sections of CH3OH, CH3OD, CD3OH, and CD3OD are measured in a 107–220 nm spectral region using synchrotron radiation. Spectra of improved quality for four deuterated isotopomers, coupled with extensive calculations on low-lying excited states of methanol using time-dependent density functional theory with a large cc-pV5Z basis set, enable us to improve assignments of observed spectral features and to better understand the nature of these electronic transitions. Energies and oscillator strengths of all transitions predicted with calculations are consistent with experimental results. Observed isotopic shifts clearly indicate that absorption features in the 163–220 nm region (transition 1 1A″–X 1A′) are associated mainly with breaking of the O–H bond, consistent with theoretical predictions. In the 151–163 nm region (transition 2 1A″–X 1A′), observed small vibrational spacings (806 cm−1 for CH3OH) associated with the C–O stretching mode can be rationalized with a broad double-well-like potential-energy curve resulting from avoided crossing of Rydberg states 11A″(2a″→3s) and 2 1A″(2a″→3p); with isotopic data, further vibrational progressions are identified. Absorption lines in the 140–151 nm region with regular vibrational spacing (∼1046 cm−1 for CH3OH), likely associated with the CH2 twisting mode, are assigned to nearly degenerate transitions 3 1A″–X 1A′ and 3 1A′–X 1A′; the 3 1A″ and 3 1A′ states are associated with excitations 2a″→3p′ and 2a″→3p″, respectively. Progressions associated with the torsional mode of the excited state are observed for the first time. For wavelengths smaller than 140 nm, Rydberg transitions with n≥3 are tentatively assigned in accord with their quantum defects that are identical for all isotopomers in each Rydberg series. © 2002 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 103 (1995), S. 6303-6304 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: We determined the threshold for photodissociation of H2O to form OH in matrices by dissociating a matrix sample in situ on scanning the energy of synchrotron radiation and by detecting the increase in intensity of laser-induced fluorescence of OH. The derived threshold, 6.89±0.04 eV for H2O in solid Ar, is almost identical to the previously reported value of 6.9±0.04 eV. The photodissociation threshold in solid Ne, 6.87±0.02 eV, is within experimental uncertainty of that determined in solid Ar. They are identical to recently determined threshold of absorption of H2O in solid Ne and Ar. Hence, photodissociation of H2O in matrices near the threshold is determined by absorption from the ground X˜ state to the repulsive A˜ state. The thresholds of absorption of H2O correspond to ∼1.7 eV excess energies of dissociation; at these energies sudden exit should dominate, consistent with the results from H2S photolysis in matrices. © 1995 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 111 (1999), S. 10093-10098 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photoionization-efficiency (PIE) spectra in the wavelength range of 108–143 nm are measured for C2H5SCl produced from reaction systems Cl/Cl2/C2H5SH and Cl/Cl2/C2H5SSC2H5 in a discharge-flow reactor coupled to a photoionization mass spectrometer employing a synchrotron as the source of radiation. According to PIE spectra of C2H5SCl thus obtained, the ionization energy (IE) is (8.994±0.007) eV. Based on GAUSSIAN-2 calculations, the observed ionization of C2H5SCl near the threshold region is likely to form doublet C2H5SCl+ from singlet C2H5SCl; the calculated IE 8.978 eV agrees well with the experimental value. A vibrational frequency of doublet C2H5SCl+, was found to be (557±60) cm−1, which agrees satisfactorily with a theoretical value of 560.9 cm−1. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 6
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 188-191 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The spectrum of photoionization efficiency (PIE) of S2O2 was measured in the spectral range 105–130 nm by means of a discharge flow and a photoionization mass spectrometer coupled to a synchrotron as a radiation source. S2O2 was generated from self reaction of SO radicals, SO+SO→S2O2, in a gaseous flow system. SO radicals were produced on reacting O atoms with CS2 and OCS. The ionization energy (IE) of S2O2 was determined to be (9.93±0.02) eV. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 7
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 110 (1999), S. 4757-4762 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Photoionization-efficiency (PIE) spectra in the wavelength range 108–144 nm were measured for CH3SCl generated from the reaction system Cl/Cl2/CH3SH(CH3SSCH3) in a discharge-flow reactor coupled to a photoionization mass spectrometer employing a synchrotron as the source of radiation. According to the PIE spectrum of CH3SCl thus obtained, the ionization energy (IE) is (9.147±0.007) eV. Based on GAUSSIAN-2 calculations, the observed ionization of CH3SCl near the threshold region is likely to form from singlet CH3SCl to doublet CH3SCl+; the calculated IE 9.140 eV agrees well with the experimental value. Two vibrational frequencies of singlet CH3SCl and one of doublet CH3SCl+ were found to be (244±60) cm−1, (513±60) cm−1, and (631±60) cm−1, respectively. © 1999 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 8
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 8794-8799 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoionization efficiency (PIE) spectrum of C2H5SO was measured in the spectral range 110–150 nm by means of a photoionization mass spectrometer coupled to a synchrotron radiation source. C2H5SO radicals were generated by reacting O atoms with C2H5SC2H5 or C2H5SSC2H5 in a discharge flow tube. The ionization energy of C2H5SO was determined to be (8.71±0.02) eV, in agreement with theoretical calculations of 8.8 eV for ionization from C2H5SO to singlet C2H5SO+ using the G2 method. PIE spectrum also shows a sharp increase at 10.0 eV, corresponding to the ionization energy from C2H5SO to triplet C2H5SO+ predicted by theory. Theoretical calculations also predict two stable conformers with similar energies for each of C2H5SO, singlet C2H5SO+, and triplet C2H5SO+, respectively; these conformers are indistinguishable in our experiments. © 1997 American Institute of Physics.
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 107 (1997), S. 5273-5274 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoionization efficiency (PIE) spectrum of HSSH was measured in the spectral range (110–140) nm by means of a discharge flow and a photoionization mass spectrometer coupled to a synchrotron radiation source. HSSH was generated from the self-reaction of HS radicals in the flow tube. HS radicals were produced by reacting Cl atoms with H2S. The adiabatic ionization energy of HSSH was determined to be (9.06±0.02) eV. GAUSSIAN-2 ab initio calculations predict 9.086 eV for ionization to the ground state of trans-HSSH+, in satisfactory agreement with the experimental result. The heat of formation of HSSH+, ΔfH°298(HSSH+), was derived to be (212.7±0.5) kcal mol−1. © 1997 American Institute of Physics.
    Type of Medium: Electronic Resource
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  • 10
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 106 (1997), S. 9727-9733 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoionization efficiency (PIE) spectrum of HSO was measured in the spectral range (107–130) nm by means of a discharge flow and a photoionization mass spectrometer coupled to a synchrotron as the radiation source. HSO radicals were generated by reacting O atoms with various organothiol compounds, C2H5SH, 2-C3H7SH, or HSC2H4SH, in the flow tube. The ionization energy of HSO was determined for the first time and found to be (9.918±0.016) eV. GAUSSIAN-2 calculations predict 9.897 eV for ionization to HSO+, the singlet ground state of the molecular ion, in satisfactory agreement with the experimental result. The onset to triplet HSO+ may occur at (11.15±0.04) eV. A vibrational frequency of HSO+ of (1150±160) cm−1 was derived from the separation of steps in the PIE spectrum. The heat of formation of HSO+ was also derived and calculated to be ΔfH298&convolu;(HSO+)=(228±5) kcal mol−1. © 1997 American Institute of Physics.
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