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  • 1
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of organic chemistry 53 (1988), S. 1113-1114 
    ISSN: 1520-6904
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology
    Type of Medium: Electronic Resource
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  • 2
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 89 (1985), S. 3552-3555 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , 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 88 (1988), S. 3086-3091 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The photoexcitation of 2-naphthol as a trace impurity in ice results in the injection of excess protons into the ice network. These protons are immobile at temperatures 〈100 K but warming to ∼120 K generates a near steady-state concentration of mobile protons which decays slowly. This behavior confirms the existence of shallow proton traps in ice which, following Kunst and Warman, are presumed to be intrinsic and, most probably, Bjerrum L defects. The quantity of mobile protons at a given temperature, in a pseudoequilibrium with immobile protons bound to the L defects, is controlled by the temperature coefficients of (a) the pseudoequilibrium constant and (b) the L-defect concentration. Since both the L and D defects are immobile below ∼130 K, the L-defect concentration can be taken to be temperature independent. Consequently, the temperature dependence of the rate at which D2O molecules isolated in H2O cubic ice are converted to (HOD)2 units by mobile protons is a direct measure of the binding energy between the excess protons and the L defects. This binding energy has been estimated at 10.0 kcal/mol. At the completion of each kinetic experiment at T〈126 K, the predominant deuterated species is (HOD)2. Such samples are ideal for observation of the ice L-defect activity which is thermally activated by warming to above 130 K. By following the rate of conversion of (HOD)2 to isolated HOD for the range 134 to 150 K, the activation energy for the L-defect formation and mobility has been determined to be 12.2 kcal for cubic ice. This is close to the value of 12.0 kcal previously determined for cubic ice from isotopic exchange rates, but is less than the accepted value for hexagonal ice of 13.1 kcal/mol. Further, the enthalpy change for ice self-ionization has been estimated as 16.8 kcal from a combination of the activation energies for proton transport (9.5 kcal) and L-defect formation (7.8 kcal) with the L-defect–proton binding energy of 10.0 kcal.
    Type of Medium: Electronic Resource
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  • 4
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 97 (1993), S. 7351-7358 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Physics
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    s.l. : American Chemical Society
    The @journal of physical chemistry 〈Washington, DC〉 97 (1993), S. 8541-8548 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , 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 87 (1987), S. 4126-4131 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: There has recently been a substantial increase in information on low-temperature phase transformations of ice and ice-like substances along with a rapid increse in molecular level information on the defect structure and activity of this subset of hydrogen-bonded solids. These data, some quantitative and some qualitative in nature, are examined from the viewpoint that the phase transformation mechanism depends on the availability of mobile orientational defects (Bjerrum L defects) within the new phase. Some of the data that seem particularly apt for establishing any dependence of the phase transformation on the presence of mobile L defects within the new phase, reflect a strong correlation between transformation rates/temperature and the availability of mobile L defects. One possible inference is that the integrity of a growing phase can be maintained only if defects responsible for orientational mobility at the interface can ultimately achieve equilibrium through recombination. The implications of such a dependence on mobile L defects are examined for a variety of systems. For example, one implication is that, at low temperature (〈160 K), the structure I clathrate hydrate of trimethylene oxide (TMO) should grow more rapidly than the structure II hydrate, since structure I hydrates are known to be relatively rich in mobile defects. New data for the clathrate hydrates of TMO are presented that confirm the preferential growth of the structure I hydrate from amorphous deposits containing water and TMO in ratios ranging from 7:1 to 〉17:1.
    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 84 (1986), S. 6095-6100 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The existing infrared spectroscopic data for the isotopomers of water [H2O, D2O, (HOD)2, and HOD] decoupled in cubic ice at 90 K are reviewed and combined with new results to complete the infrared data for the internal vibrational modes. An assignment of the observed absorption bands, including the perturbed Fermi diads for νs in resonance with 2ν2, that largely follows established views is offered. This assignment is shown to be internally self-consistent by the analysis of the Fermi diads within a single framework based on the simplest representation of the effects of Fermi resonance and using the Burneau–Corset value for the Fermi-interaction parameter appropriate to cubic ice (60 cm−1 for H2O). It is shown that the inclusion of the decoupled-HOD diads significantly lowers the estimated value of νs for H2O and, consequently, allows the downshift of this mode to the observed frequency value (3225 cm−1), through resonance with 2ν2 (where ν2=1735 cm−1), to be closely modeled using the relatively small Fermi-interaction parameter of Burneau and Corset.
    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 83 (1985), S. 4387-4394 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: An ability to prepare clathrate hydrates using low temperature–high vacuum techniques, originally demonstrated for the hydrate of oxirane (Bertie and Devlin), has been extended to include the structure I hydrate of H2S, the mixed structure I hydrate of oxirane and ethane, as well as the structure II simple hydrate of THF and the double hydrates of THF with oxirane and H2S. The crystalline clathrate films (∼6 μ) have been formed either by annealing amorphous host–guest deposits at ∼130 K, epitaxial growth at 110 K (oxirane and mixed ethane–oxirane), or direct deposition at 150 K (THF and its double clathrates). Use of the epitaxial approach at ∼100 K has permitted the formation of the oxirane clathrate hydrate containing intact isolated D2O molecules. This has permitted the FT–IR observation of the ν3–ν1 doublet in the O–D stretching region (2455 and 2380 cm−1 at 100 K) with the values, after correction for Fermi resonance, suggesting a splitting from intramolecular coupling of ∼56 cm−1 (2455 vs 2399 cm−1), which compares closely with the 52 cm−1 deduced for cubic ice. Spectra for the structure I hydrates of oxirane and H2S contain absorption bands produced by guest molecules confined to both small and large clathrate cages. Use of the structure II double hydrates has permitted the firm identification of the structure I infrared bands with oxirane and H2S molecules in cages of one size or the other. Thus, the weaker ν3 and (ν11,ν14) bands of oxirane at 1281 and 1152 cm−1 have been assigned to molecules in the small cages since only these oxirane features remain in the structure II double hydrate with THF. In this case the smaller oxirane molecules occupy the small cages while the THF molecules enter the larger cages, exclusively. In a similar manner, the H–S stretching vibrations of H2S in the structure I small cages have been assigned to a band complex near 2610 cm−1, some 50 cm−1 above the band system for H2S in the large structure I clathrate cages.Such a result suggests that the net H2S perturbation, relative to the gas phase, is greater for the large than for the small cages and may be interpreted as evidence for a "double well'' large cage potential or as further evidence that the cage model of Pimentel and Charles for guest-molecule stretching modes is valid.
    Type of Medium: Electronic Resource
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  • 9
    Electronic Resource
    Electronic Resource
    College Park, Md. : American Institute of Physics (AIP)
    The Journal of Chemical Physics 84 (1986), S. 4111-4112 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Electron beam radiolysis of ice and the ion pair defects it generates in ice are discussed. The FI-IR spectra of thin films of ice are recorded both before and after irradiation. (AIP)
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  • 10
    Publication Date: 1993-08-01
    Print ISSN: 0022-3654
    Electronic ISSN: 1541-5740
    Topics: Chemistry and Pharmacology , Physics
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