Phys. Rev. E 73, 051704 (2006) [8 pages]
Stochastic molecular motions in the nematic, smectic-A, and solid phases of p,p -di-n-heptyl-azoxybenzene as seen by quasielastic neutron scattering and 13C cross-polarization magic-angle-spinning NMR
Abstract
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Wojciech Zaj cThe H. Niewodnicza ski Institute of Nuclear Physics, Polish Academy of Sciences, Radzikowskiego 152, 31-342 Kraków, PolandStanis aw UrbanInstitute of Physics, Jagiellonian University, Reymonta 4, 30-059 Kraków, PolandValentina Domenici, Marco Geppi, and Carlo Alberto VeraciniDipartimento di Chimica e Chimica Industriale, Università degli Studi di Pisa, via Risorgimento 35, 56126 Pisa, ItalyMark T. F. TellingISIS Facility, Rutherford Appleton Laboratory, Chilton, Didcot OX11 0QX, United KingdomBarbara J. Gabry Department of Materials Science, University of Oxford, Parks Road, Oxford OX1 3PH, United Kingdom
Received 12 October 2005; published 11 May 2006
Molecular rotational dynamics in p,p -di-n-heptyl-azoxybenzene was studied by means of quasielastic neutron scattering (QENS) and 13C cross-polarization magic-angle-spinning (CPMAS) NMR. Fast reorientation of the hydrogen nuclei was observed by QENS in the two liquid crystalline (LC) phases nematic and smectic A, as well as in the crystalline phase. The latter could not be restricted to the CH3 rotations alone, and a clear indication was found of some other reorientation motions persisting in the crystal. Two Lorentz-type components convoluted with the resolution function gave an excellent fit to the QENS spectra in both LC phases. The narrow (slow) component was attributed to the reorientation of the whole molecule around the long axis. The corresponding characteristic time of ~130 ps agreed well with the values obtained in recent dielectric relaxation and 2H NMR studies. The full width at half maximum of the broader (fast) component shows a quadratic Q dependence (Q is the momentum transfer). Hence the corresponding motions could be described by a stretched exponential correlation function and were interpreted as various "crankshaft-type" motions within the alkyl tails. The 13C CPMAS experiments fully corroborated the QENS results, sometimes considered ambiguous in complex systems.
©2006 The American Physical Society
REFERENCES (32)
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- P. L. Nordio, G. Rigatti, and U. Segre, J. Chem. Phys. 56, 2117 (1972).
- S. Mitra, K. Venu, I. Tsukushi, S. Ikeda, and R. Mukhopadhyay, Phys. Rev. E 69, 061709 (2004).
- A. V. Zakharov and Ronald Y. Dong, Phys. Rev. E 63, 011704 (2000).
- A. V. Zakharov and R. Y. Dong, Phys. Rev. E 64, 031701 (2001).
- U. Buchenau, C. Schönfeld, D. Richter, Phys. Rev. Lett. 73, 2344 (1994).
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