Raman scattering studies of order parameters in liquid crystalline dimers exhibiting the nematic and twist-bend nematic phases
Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N TB ) nematic phases of a homologous series of liquid crystalline dimers. The dimers investigated have 7, 8, 9 and 11 methylene groups connecting two cyanobiphenyl mesogens and dat...
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Published in | Journal of materials chemistry. C, Materials for optical and electronic devices Vol. 3; no. 38; pp. 17 - 116 |
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Main Authors | , , , , , , , |
Format | Journal Article |
Language | English |
Published |
01.01.2015
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Subjects | |
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Abstract | Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N
TB
) nematic phases of a homologous series of liquid crystalline dimers. The dimers investigated have 7, 8, 9 and 11 methylene groups connecting two cyanobiphenyl mesogens and data for 4-pentyl-4′-cyanobiphenyl (5CB) and 4-octyl-4′-cyanobiphenyl (8CB) are included for comparison. Simulated and measured Raman spectra for the materials are compared. PRS is used to determine both 〈
P
2
〉 and 〈
P
4
〉 order parameters across the nematic temperature range and immediately below the N
TB
-N phase transition using a model that takes into account the molecular bend of the odd dimers, which is described in detail. In the nematic phase, the odd dimers are found to exhibit rather low order parameters with 〈
P
2
〉 taking values between 0.3 and 0.5 and 〈
P
4
〉 about 0.25. In contrast, the even dimer shows extremely high values of the order parameters with 〈
P
2
〉 taking values between 0.7 and 0.8 and 〈
P
4
〉 between 0.4 and 0.45. For the odd dimers, the values of 〈
P
2
〉 in the N
TB
phase are similar to those of the N phase, whereas 〈
P
4
〉 jumps by approximately 5-10% and then decreases with temperature. On comparing the experimental data with the theoretical predictions, we find reasonable qualitative agreement for all materials with molecular field theory. The odd dimers, however, show higher 〈
P
4
〉 values than obtained from theoretical models, a factor attributed to the neglect of molecular flexibility and biaxiality in the PRS analysis.
The work deduces orientational order parameters in the nematic and twist-bend nematic phases. An homologous series of dimers is studied using Polarized Raman Spectroscopy. |
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AbstractList | Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N sub(TB)) nematic phases of a homologous series of liquid crystalline dimers. The dimers investigated have 7, 8, 9 and 11 methylene groups connecting two cyanobiphenyl mesogens and data for 4-pentyl-4'-cyanobiphenyl (5CB) and 4-octyl-4'-cyanobiphenyl (8CB) are included for comparison. Simulated and measured Raman spectra for the materials are compared. PRS is used to determine both <P sub(2)> and <P sub(4)> order parameters across the nematic temperature range and immediately below the N sub(TB)-N phase transition using a model that takes into account the molecular bend of the odd dimers, which is described in detail. In the nematic phase, the odd dimers are found to exhibit rather low order parameters with <P sub(2)> taking values between 0.3 and 0.5 and <P sub(4)> about 0.25. In contrast, the even dimer shows extremely high values of the order parameters with <P sub(2)> taking values between 0.7 and 0.8 and <P sub(4)> between 0.4 and 0.45. For the odd dimers, the values of <P sub(2)> in the N sub(TB) phase are similar to those of the N phase, whereas <P sub(4)> jumps by approximately 5-10% and then decreases with temperature. On comparing the experimental data with the theoretical predictions, we find reasonable qualitative agreement for all materials with molecular field theory. The odd dimers, however, show higher <P sub(4)> values than obtained from theoretical models, a factor attributed to the neglect of molecular flexibility and biaxiality in the PRS analysis. Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N TB ) nematic phases of a homologous series of liquid crystalline dimers. The dimers investigated have 7, 8, 9 and 11 methylene groups connecting two cyanobiphenyl mesogens and data for 4-pentyl-4′-cyanobiphenyl (5CB) and 4-octyl-4′-cyanobiphenyl (8CB) are included for comparison. Simulated and measured Raman spectra for the materials are compared. PRS is used to determine both 〈 P 2 〉 and 〈 P 4 〉 order parameters across the nematic temperature range and immediately below the N TB -N phase transition using a model that takes into account the molecular bend of the odd dimers, which is described in detail. In the nematic phase, the odd dimers are found to exhibit rather low order parameters with 〈 P 2 〉 taking values between 0.3 and 0.5 and 〈 P 4 〉 about 0.25. In contrast, the even dimer shows extremely high values of the order parameters with 〈 P 2 〉 taking values between 0.7 and 0.8 and 〈 P 4 〉 between 0.4 and 0.45. For the odd dimers, the values of 〈 P 2 〉 in the N TB phase are similar to those of the N phase, whereas 〈 P 4 〉 jumps by approximately 5-10% and then decreases with temperature. On comparing the experimental data with the theoretical predictions, we find reasonable qualitative agreement for all materials with molecular field theory. The odd dimers, however, show higher 〈 P 4 〉 values than obtained from theoretical models, a factor attributed to the neglect of molecular flexibility and biaxiality in the PRS analysis. The work deduces orientational order parameters in the nematic and twist-bend nematic phases. An homologous series of dimers is studied using Polarized Raman Spectroscopy. Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N TB ) nematic phases of a homologous series of liquid crystalline dimers. The dimers investigated have 7, 8, 9 and 11 methylene groups connecting two cyanobiphenyl mesogens and data for 4-pentyl-4′-cyanobiphenyl (5CB) and 4-octyl-4′-cyanobiphenyl (8CB) are included for comparison. Simulated and measured Raman spectra for the materials are compared. PRS is used to determine both 〈 P 2 〉 and 〈 P 4 〉 order parameters across the nematic temperature range and immediately below the N TB –N phase transition using a model that takes into account the molecular bend of the odd dimers, which is described in detail. In the nematic phase, the odd dimers are found to exhibit rather low order parameters with 〈 P 2 〉 taking values between 0.3 and 0.5 and 〈 P 4 〉 about 0.25. In contrast, the even dimer shows extremely high values of the order parameters with 〈 P 2 〉 taking values between 0.7 and 0.8 and 〈 P 4 〉 between 0.4 and 0.45. For the odd dimers, the values of 〈 P 2 〉 in the N TB phase are similar to those of the N phase, whereas 〈 P 4 〉 jumps by approximately 5–10% and then decreases with temperature. On comparing the experimental data with the theoretical predictions, we find reasonable qualitative agreement for all materials with molecular field theory. The odd dimers, however, show higher 〈 P 4 〉 values than obtained from theoretical models, a factor attributed to the neglect of molecular flexibility and biaxiality in the PRS analysis. |
Author | Panov, Vitaly P Jones, J. Cliff Goodby, John W Zhang, Zhaopeng Nagaraj, Mamatha Gleeson, Helen F Luckhurst, Geoffrey R Mandle, Richard J |
AuthorAffiliation | Department of Chemistry University of Leeds University of Southampton School of Physics and Astronomy University of Manchester University of York School of Chemistry |
AuthorAffiliation_xml | – name: University of Southampton – name: Department of Chemistry – name: School of Physics and Astronomy – name: University of Leeds – name: University of Manchester – name: School of Chemistry – name: University of York |
Author_xml | – sequence: 1 givenname: Zhaopeng surname: Zhang fullname: Zhang, Zhaopeng – sequence: 2 givenname: Vitaly P surname: Panov fullname: Panov, Vitaly P – sequence: 3 givenname: Mamatha surname: Nagaraj fullname: Nagaraj, Mamatha – sequence: 4 givenname: Richard J surname: Mandle fullname: Mandle, Richard J – sequence: 5 givenname: John W surname: Goodby fullname: Goodby, John W – sequence: 6 givenname: Geoffrey R surname: Luckhurst fullname: Luckhurst, Geoffrey R – sequence: 7 givenname: J. Cliff surname: Jones fullname: Jones, J. Cliff – sequence: 8 givenname: Helen F surname: Gleeson fullname: Gleeson, Helen F |
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Snippet | Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N
TB
) nematic phases of a homologous... Polarized Raman Spectroscopy (PRS) is used to quantify the orientational order in the conventional (N) and twist-bend (N sub(TB)) nematic phases of a... |
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SubjectTerms | Dimers Field theory Liquid crystals Mathematical models Methylene Nematic Order parameters Phases |
Title | Raman scattering studies of order parameters in liquid crystalline dimers exhibiting the nematic and twist-bend nematic phases |
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