Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold
In this paper, we demonstrate electric field-induced wavelength tuning of the entire photonic band-gap of an achiral nematic liquid crystal (LC) filled into a chiral polymer scaffold. This chiral polymer scaffold has been formed by creating a template of a chiral nematic LC phase, which remarka...
| Glavni autori: | , , , |
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| Format: | Journal article |
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American Chemical Society
2016
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| _version_ | 1826289782774300672 |
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| author | Morris, S Elston, S Fells, J Wood, S |
| author_facet | Morris, S Elston, S Fells, J Wood, S |
| author_sort | Morris, S |
| collection | OXFORD |
| description | In this paper, we demonstrate electric field-induced wavelength tuning of the entire photonic band-gap of an achiral nematic liquid crystal (LC) filled into a chiral polymer scaffold. This chiral polymer scaffold has been formed by creating a template of a chiral nematic LC phase, which remarkably does not compromise the optical finesse of the band-gap when compared to that of a conventional, polymer-stabilized chiral nematic LC. We present results on the spectral shift and temporal evolution of the photonic band-gap in the presence of an external a.c. electric field. It is shown that, initially, there is a rapid (τ ≈ 1 ms) blue-shift of the longwavelength band-edge followed by a considerably slower blue-shift (τ ≈ 6.5 s) of the entire band-gap. We compare the results with those obtained for a polymer-stabilized chiral nematic LC where only a blue-shift of the long-wavelength band-edge is observed. Consequently, we find that, for the templated sample, the tuning range is more than a factor of two greater than that observed for the polymer-stabilized chiral nematic LC for the same range of electric field amplitudes. It is also found that there is little in the way of hysteresis upon increasing and decreasing the applied electric field magnitude. Finally, we present experimental evidence that suggests that the blue-shift of the entire band-gap is due to an additional tuning mechanism present only for the case of the templated samples. This is believed to be caused by a contraction of the pitch that results from a translational motion of the polymer network. The greater tuning range observed in these templated samples are potentially important for the development of tunable 1-dimensional photonic band-gaps and LC lasers. Furthermore, it avoids the use of d.c. electric fields that can lead to long-term issues regarding stability. |
| first_indexed | 2024-03-07T02:34:09Z |
| format | Journal article |
| id | oxford-uuid:a83b2fe8-06e1-4a5d-b25e-e712c9938d6e |
| institution | University of Oxford |
| last_indexed | 2024-03-07T02:34:09Z |
| publishDate | 2016 |
| publisher | American Chemical Society |
| record_format | dspace |
| spelling | oxford-uuid:a83b2fe8-06e1-4a5d-b25e-e712c9938d6e2022-03-27T02:59:57ZWavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffoldJournal articlehttp://purl.org/coar/resource_type/c_dcae04bcuuid:a83b2fe8-06e1-4a5d-b25e-e712c9938d6eSymplectic Elements at OxfordAmerican Chemical Society2016Morris, SElston, SFells, JWood, SIn this paper, we demonstrate electric field-induced wavelength tuning of the entire photonic band-gap of an achiral nematic liquid crystal (LC) filled into a chiral polymer scaffold. This chiral polymer scaffold has been formed by creating a template of a chiral nematic LC phase, which remarkably does not compromise the optical finesse of the band-gap when compared to that of a conventional, polymer-stabilized chiral nematic LC. We present results on the spectral shift and temporal evolution of the photonic band-gap in the presence of an external a.c. electric field. It is shown that, initially, there is a rapid (τ ≈ 1 ms) blue-shift of the longwavelength band-edge followed by a considerably slower blue-shift (τ ≈ 6.5 s) of the entire band-gap. We compare the results with those obtained for a polymer-stabilized chiral nematic LC where only a blue-shift of the long-wavelength band-edge is observed. Consequently, we find that, for the templated sample, the tuning range is more than a factor of two greater than that observed for the polymer-stabilized chiral nematic LC for the same range of electric field amplitudes. It is also found that there is little in the way of hysteresis upon increasing and decreasing the applied electric field magnitude. Finally, we present experimental evidence that suggests that the blue-shift of the entire band-gap is due to an additional tuning mechanism present only for the case of the templated samples. This is believed to be caused by a contraction of the pitch that results from a translational motion of the polymer network. The greater tuning range observed in these templated samples are potentially important for the development of tunable 1-dimensional photonic band-gaps and LC lasers. Furthermore, it avoids the use of d.c. electric fields that can lead to long-term issues regarding stability. |
| spellingShingle | Morris, S Elston, S Fells, J Wood, S Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
| title | Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
| title_full | Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
| title_fullStr | Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
| title_full_unstemmed | Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
| title_short | Wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
| title_sort | wavelength tuning of the photonic band gap of an achiral nematic liquid crystal filled into a chiral polymer scaffold |
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