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  • 1
    ISSN: 1520-6041
    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
    Industrial and engineering chemistry 19 (1980), S. 551-556 
    Source: ACS Legacy Archives
    Topics: Chemistry and Pharmacology , Process Engineering, Biotechnology, Nutrition Technology
    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 83 (1985), S. 3707-3708 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: The 15N/14N isotope shift on the 15N chemical shielding in a mixture of 15N14N and 15N15N was found to be 0.0601±0.0022 ppm. Using a model developed by Jameson, the nuclear shielding derivative with respect to bond length was calculated from the measured isotope shift, [∂σ(15N)/∂r]e =−910±42 ppm/A(ring). This value is in excellent agreement with a value obtained from the temperature dependence of the shielding constant in the gas phase (at the zero pressure limit) and with a value determined from recent molecular orbital calculations. From relaxation measurements the scalar spin–spin coupling constant, 1J(14N,15N), in 14N15N was calculated to be 1.8±0.6 Hz which gives a reduced coupling constant, 1K(N,N)=2.0±0.7 (1020)m−2kg s−2 A(ring)−2. The magnitude of the reduced coupling constant is compared to that of other isoelectronic species and molecular orbital calculations.
    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 83 (1985), S. 548-551 
    ISSN: 1089-7690
    Source: AIP Digital Archive
    Topics: Physics , Chemistry and Pharmacology
    Notes: Oxygen isotope shifts on the 13C chemical shifts and carbon isotope shifts on the 17O chemical shifts in carbon monoxide and carbon dioxide are reported. Using models developed by Jameson, shielding derivatives with respect to bond lengths can be calculated using the measured isotope shifts. For carbon monoxide, the derivatives were calculated to be [∂σ (13C)/∂r]e =−456±15 ppm/A(ring) and [∂σ (17O)/∂r]e =−1150±130 ppm/A(ring). Although earlier coupled Hartree–Fock calculations give a much lower value for [∂σ (17O)/∂r]e, recent ab initio calculations for carbon monoxide agree very well with our experimental results. Furthermore, the observed 18O/16O iostope shift is similar to values measured previously for a series of metal carbonyls. For carbon dioxide the iostope shift gives [∂σ (13C)/∂r]e =−214±17 ppm/A(ring) which is in excellent agreement with the value obtained from a recent variable temperature gas phase NMR study. In addition, scalar spin–spin coupling constants, 1J(13C,17O) were measured to be 16.4±0.1 Hz in carbon monoxide and 16.1±0.1 Hz in carbon dioxide. To our knowledge, these are the first directly measured carbon–oxygen coupling constants to be reported in the literature. From general trends in the periodic table, it seems likely that the sign of these coupling constants is positive.
    Type of Medium: Electronic Resource
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  • 5
    Electronic Resource
    Electronic Resource
    Chichester : Wiley-Blackwell
    Organic Magnetic Resonance 26 (1988), S. 903-910 
    ISSN: 0749-1581
    Keywords: Multi-dimensional spectroscopy ; Nuclear magnetic resonance ; NMR ; Chemistry ; Analytical Chemistry and Spectroscopy
    Source: Wiley InterScience Backfile Collection 1832-2000
    Topics: Chemistry and Pharmacology
    Notes: Multi-dimensional NMR spectroscopy must satisfy the Nyquist sampling condition in all frequency dimensions. This entails very long experiments and very large data arrays, and may mean that fine structure of cross-peaks cannot be adequately digitized. This sampling restriction can be sidestepped in an alternative approach which explores the new frequency dimensions by scanning selective radiofrequency pulses in small steps over narrow frequency ranges. A pulse envelope shaped according to the first half of a Gaussian curve is particularly well suited to this task. Thus a form of double resonance experiment can be used to generate two-dimensional correlation spectra that have all the features of the well known COSY experiment, with an additional ‘zoom’ capability that reveals the detailed fine structure information. For systems of three coupled spins the corresponding triple resonance experiment generates a three-dimensional correlation specrum, the frequency scans being restricted to the region of interest (the 3D cross-peak) based on information from the conventional NMR spectrum. For correlation spectroscopy of higher dimensionality no frequency search is employed, the selective pulses simply being set at predetermined chemical shift frequencies. A four-dimensional correlation experiment is described which uses population transfer to establish that four non-equivalent protons are coupled in a chain I—S—R—P. It employs an initial ‘ZZ-pulse’ applied at the I-spin frequency to excite longitudinal two-spin order (2IzSz) which is then propagated along the chain by the application of selective ‘ZZZ-pulses’ to the intermediate spins S and R, creating an antiphase intensity perturbation (2RzPz) on the P multiplet. The procedure is recursive and can in principle be extended to N spins coupled pairwise in a ‘linear’ chain. This is a powerful diagnostic tool for structure determination and can be adapted to recognize other topological features such as chain branching and ring closure.
    Additional Material: 12 Ill.
    Type of Medium: Electronic Resource
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