Der Zeeman-Effekt im Rotationsspektrum von Orthodifluorbenzol

The linear and quadratic rotational Zeeman effect in orthodifluorobenzene has been observed in magnetic fields up to 25 kG. The magnetic susceptibility anisotropies are χaa- (χbb -χcc)/2 = (25.4 ± 0.8)* 10 erg/(G * mole) and χbb - (χcc - χaa)/2 = (29.0±0.5)* 10 erg/ (G * mole) ; (the c-axis is perpe...

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Veröffentlicht in:Zeitschrift für Naturforschung. A, A journal of physical sciences A journal of physical sciences, 1974-05, Vol.29 (5), p.786-796
1. Verfasser: Sutter, Dieter H.
Format: Artikel
Sprache:eng
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Zusammenfassung:The linear and quadratic rotational Zeeman effect in orthodifluorobenzene has been observed in magnetic fields up to 25 kG. The magnetic susceptibility anisotropies are χaa- (χbb -χcc)/2 = (25.4 ± 0.8)* 10 erg/(G * mole) and χbb - (χcc - χaa)/2 = (29.0±0.5)* 10 erg/ (G * mole) ; (the c-axis is perpendicular to the molecular plane and the a-axis coincides with the twofold symmetry axis of the molecule); the molecular ^-values are gaa= -0.0412 ± 0.00'I2, gbb=0.0371± 0.0008 and gcc= +0.0163 ±0.0007. A comparison of ⊿χ = χcc- (χaa + χbb)/2 with the corresponding values of related compounds, part of which were determined by the Cotton-Mouton technique, indicates that the effect of the magnetic field on the electric polarizability of benzene - like molecules is in the order of - 1 * 10 cm /G and should be accounted for in the evaluation of Cotton- Mouton data.
ISSN:0932-0784
1865-7109
DOI:10.1515/zna-1974-0521