THE ALIGNMENT OF THE SMECTIC A PHASE OF 4-OCTYL-4′-CYANOBIPHENYL INDUCED BY AN ELECTRIC FIELD. A TIME-RESOLVED DEUTERIUM NMR STUDY

Studies of the field-induced alignment of the SmA phase using deuterium NMR spectroscopy have revealed a complex pattern of behaviour when the director is initially orthogonal to the aligning field. Here we report the electric field-induced alignment of the SmA director using time-resolved deuterium...

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Published inMolecular crystals and liquid crystals (Philadelphia, Pa. : 2003) Vol. 402; no. 1; pp. 103 - 116
Main Authors Luckhurst, Geoffrey R., Timimi, Bakir A., Miyamoto, Tetsuo, Sugimura, Akihiko
Format Journal Article Conference Proceeding
LanguageEnglish
Published Philadelphia, PA Taylor & Francis Group 01.01.2003
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Abstract Studies of the field-induced alignment of the SmA phase using deuterium NMR spectroscopy have revealed a complex pattern of behaviour when the director is initially orthogonal to the aligning field. Here we report the electric field-induced alignment of the SmA director using time-resolved deuterium NMR when the aligning electric field E is at an angle with the magnetic field B of the spectrometer which is considerably smaller than 90°; here the director is initially aligned parallel to the magnetic field. The dynamics of the electric field-induced alignment of the director for the smectic phase of 4-α,α-d 2 -octyl-4′-cyanobiphenyl (8CB-d 2 ) was investigated at two angles between B and E of roughly 45° and 54.5° the so-called magic angle, at different electric field strengths and also at two temperatures, 305.1 K and 302.6 K. The dynamics of the SmA director alignment of 8CB-d 2 was monitored by measuring the deuterium NMR spectrum as a function of time. The results for the 45° and 54.5° geometries revealed, in contrast to the complex dynamics of alignment of theSmA director observed for the 90° geometry, a much simpler pattern of relaxation. Here the director appeared to be aligned almost as a monodomain. In general, for either of the two geometries employed here, the ultimate angle of alignment the director achieves relative to E depends on the electric field strength. Lowering the temperature by just 2.5°C from 305.1 K to 302.6 K has a dramatic effect on the rate of director relaxation presumably because of the large increase in the combined rotational viscosity and the elastic energy effectsof the SmA phase with decreasing temperature. Furthermore for the 45° geometry at 302.6 K, the SmA sample separates on relaxation ultimately into two domains with different alignment angles.
AbstractList Studies of the field-induced alignment of the SmA phase using deuterium NMR spectroscopy have revealed a complex pattern of behaviour when the director is initially orthogonal to the aligning field. Here we report the electric field-induced alignment of the SmA director using time-resolved deuterium NMR when the aligning electric field E is at an angle with the magnetic field B of the spectrometer which is considerably smaller than 90°; here the director is initially aligned parallel to the magnetic field. The dynamics of the electric field-induced alignment of the director for the smectic phase of 4-α,α-d 2 -octyl-4′-cyanobiphenyl (8CB-d 2 ) was investigated at two angles between B and E of roughly 45° and 54.5° the so-called magic angle, at different electric field strengths and also at two temperatures, 305.1 K and 302.6 K. The dynamics of the SmA director alignment of 8CB-d 2 was monitored by measuring the deuterium NMR spectrum as a function of time. The results for the 45° and 54.5° geometries revealed, in contrast to the complex dynamics of alignment of theSmA director observed for the 90° geometry, a much simpler pattern of relaxation. Here the director appeared to be aligned almost as a monodomain. In general, for either of the two geometries employed here, the ultimate angle of alignment the director achieves relative to E depends on the electric field strength. Lowering the temperature by just 2.5°C from 305.1 K to 302.6 K has a dramatic effect on the rate of director relaxation presumably because of the large increase in the combined rotational viscosity and the elastic energy effectsof the SmA phase with decreasing temperature. Furthermore for the 45° geometry at 302.6 K, the SmA sample separates on relaxation ultimately into two domains with different alignment angles.
Author Sugimura, Akihiko
Timimi, Bakir A.
Luckhurst, Geoffrey R.
Miyamoto, Tetsuo
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CitedBy_id crossref_primary_10_1080_02678290500124692
crossref_primary_10_1103_PhysRevE_91_062502
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crossref_primary_10_1007_s00723_020_01249_3
crossref_primary_10_1016_j_tsf_2005_07_042
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Issue 1
Keywords Temperature dependence
Smectic crystals
Cyanobiphenyls
Magnetic field effects
Experimental study
Liquid crystals
Time resolved spectra
electric field-induced alignment
Time dependence
Alignment
Electric field effects
Nuclear magnetic resonance
deuterium NMR
Smectic A
Organic compounds
Language English
License CC BY 4.0
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MeetingName Proceedings of the Second Anglo-Japanese Seminar on Liquid Crystals: 5th-7th September 2001, York, United Kingdom. Part III of III
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2003
2003-01-00
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PublicationTitle Molecular crystals and liquid crystals (Philadelphia, Pa. : 2003)
PublicationYear 2003
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Taylor & Francis
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Snippet Studies of the field-induced alignment of the SmA phase using deuterium NMR spectroscopy have revealed a complex pattern of behaviour when the director is...
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SubjectTerms Chemical and knight shifts
Condensed matter: electronic structure, electrical, magnetic, and optical properties
Condensed matter: structure, mechanical and thermal properties
deuterium NMR
electric field-induced alignment
Exact sciences and technology
Liquid crystals
Magnetic resonances and relaxations in condensed matter, mössbauer effect
Nuclear magnetic resonance and relaxation
Orientational order of liquid crystals; electric and magnetic field effects on order
Physics
Smectic A
Structure of solids and liquids; crystallography
Title THE ALIGNMENT OF THE SMECTIC A PHASE OF 4-OCTYL-4′-CYANOBIPHENYL INDUCED BY AN ELECTRIC FIELD. A TIME-RESOLVED DEUTERIUM NMR STUDY
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