Field-induced second-harmonic generation induced by distorted soft chiral crystal
The nonlinear optical response of soft chiral crystal system-blue-phase (BP) liquid crystals was studied experimentally using a second-harmonic-generation (SHG) microscope. With the aid of the SHG microscope (SHM), the internal coupling between the polarization and structural deformation was visuali...
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Veröffentlicht in: | Journal of physics. D, Applied physics Applied physics, 2023-03, Vol.56 (12), p.125303 |
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creator | Chen, Hui-Yu Araoka, Fumito Lee, Fang-Yu Lee, Chi Chen, Jui Jiun |
description | The nonlinear optical response of soft chiral crystal system-blue-phase (BP) liquid crystals was studied experimentally using a second-harmonic-generation (SHG) microscope. With the aid of the SHG microscope (SHM), the internal coupling between the polarization and structural deformation was visualized in a short time. In this study, a fringing field, formed at the electrode edges, causes lattice deformation of the cubic BPs, which contributes to the flexoelectric-optic response and field-induced SHG at low frequencies. Using the SHM, we can observe the spatial distribution of the induced polarization in the BPs, and the mean SHG intensity of the cubic BP depends quadratically on the strength of the electric field at a lower value. As the applied electric field increases, the structure of the BPs transfers to the chiral nematic phase (N*), and then the SHG intensity remains constant. Compared to the mean intensities of the SHG signal in N* and the different BPs in the low electric field, the SHG signal caused by the lattice deformation in BPs is weaker in N* and depends on the cubic structure of the BPs. The experimental results demonstrate that through the SHM, the influence of the inhomogeneous electric field on the BPs can be exhibited clearly because the response of the SHG signal in BPs is sensitive to field-induced lattice deformation and phase transitions between the BPs and chiral nematic. This will help us elucidate the mechanism of the secondary electro-optical response in BPs and for further improvement and development of high-performance photonic devices using BPs. |
doi_str_mv | 10.1088/1361-6463/acbe09 |
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With the aid of the SHG microscope (SHM), the internal coupling between the polarization and structural deformation was visualized in a short time. In this study, a fringing field, formed at the electrode edges, causes lattice deformation of the cubic BPs, which contributes to the flexoelectric-optic response and field-induced SHG at low frequencies. Using the SHM, we can observe the spatial distribution of the induced polarization in the BPs, and the mean SHG intensity of the cubic BP depends quadratically on the strength of the electric field at a lower value. As the applied electric field increases, the structure of the BPs transfers to the chiral nematic phase (N*), and then the SHG intensity remains constant. Compared to the mean intensities of the SHG signal in N* and the different BPs in the low electric field, the SHG signal caused by the lattice deformation in BPs is weaker in N* and depends on the cubic structure of the BPs. The experimental results demonstrate that through the SHM, the influence of the inhomogeneous electric field on the BPs can be exhibited clearly because the response of the SHG signal in BPs is sensitive to field-induced lattice deformation and phase transitions between the BPs and chiral nematic. This will help us elucidate the mechanism of the secondary electro-optical response in BPs and for further improvement and development of high-performance photonic devices using BPs.</description><identifier>ISSN: 0022-3727</identifier><identifier>EISSN: 1361-6463</identifier><identifier>DOI: 10.1088/1361-6463/acbe09</identifier><identifier>CODEN: JPAPBE</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>blue phase ; electro-optical response ; lattice deformation ; liquid crystals ; second-harmonic generation</subject><ispartof>Journal of physics. D, Applied physics, 2023-03, Vol.56 (12), p.125303</ispartof><rights>2023 IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><cites>FETCH-LOGICAL-c330t-70a2f76166ffe285e17529b0bf61e08aaad518791da5d4305c001a38979a6d5e3</cites><orcidid>0000-0002-9662-2976</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/1361-6463/acbe09/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,776,780,27901,27902,53821,53868</link.rule.ids></links><search><creatorcontrib>Chen, Hui-Yu</creatorcontrib><creatorcontrib>Araoka, Fumito</creatorcontrib><creatorcontrib>Lee, Fang-Yu</creatorcontrib><creatorcontrib>Lee, Chi</creatorcontrib><creatorcontrib>Chen, Jui Jiun</creatorcontrib><title>Field-induced second-harmonic generation induced by distorted soft chiral crystal</title><title>Journal of physics. D, Applied physics</title><addtitle>JPhysD</addtitle><addtitle>J. Phys. D: Appl. Phys</addtitle><description>The nonlinear optical response of soft chiral crystal system-blue-phase (BP) liquid crystals was studied experimentally using a second-harmonic-generation (SHG) microscope. With the aid of the SHG microscope (SHM), the internal coupling between the polarization and structural deformation was visualized in a short time. In this study, a fringing field, formed at the electrode edges, causes lattice deformation of the cubic BPs, which contributes to the flexoelectric-optic response and field-induced SHG at low frequencies. Using the SHM, we can observe the spatial distribution of the induced polarization in the BPs, and the mean SHG intensity of the cubic BP depends quadratically on the strength of the electric field at a lower value. As the applied electric field increases, the structure of the BPs transfers to the chiral nematic phase (N*), and then the SHG intensity remains constant. Compared to the mean intensities of the SHG signal in N* and the different BPs in the low electric field, the SHG signal caused by the lattice deformation in BPs is weaker in N* and depends on the cubic structure of the BPs. The experimental results demonstrate that through the SHM, the influence of the inhomogeneous electric field on the BPs can be exhibited clearly because the response of the SHG signal in BPs is sensitive to field-induced lattice deformation and phase transitions between the BPs and chiral nematic. This will help us elucidate the mechanism of the secondary electro-optical response in BPs and for further improvement and development of high-performance photonic devices using BPs.</description><subject>blue phase</subject><subject>electro-optical response</subject><subject>lattice deformation</subject><subject>liquid crystals</subject><subject>second-harmonic generation</subject><issn>0022-3727</issn><issn>1361-6463</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2023</creationdate><recordtype>article</recordtype><recordid>eNp9kM1LAzEQxYMoWKt3j3vyZHSSNNnsUYpVoSCCnsNsPmzKdlOS7aH_vV2qnkQYeDD83jDvEXLN4I6B1vdMKEbVTIl7tK2H5oRMflenZALAORU1r8_JRSlrAJBKswl5W0TfORp7t7PeVcXb1Du6wrxJfbTVp-99xiGmvvpB2n3lYhlSHkY-haGyq5ixq2zelwG7S3IWsCv-6lun5GPx-D5_psvXp5f5w5JaIWCgNSAPtWJKheC5lp7VkjcttEExDxoRnWS6bphD6WYCpAVgKHRTN6ic9GJK4HjX5lRK9sFsc9xg3hsGZqzEjPnNmN8cKzlYbo-WmLZmnXa5Pzz4H37zB-6MVIbxw0gBwmxdEF8iKHAa</recordid><startdate>20230323</startdate><enddate>20230323</enddate><creator>Chen, Hui-Yu</creator><creator>Araoka, Fumito</creator><creator>Lee, Fang-Yu</creator><creator>Lee, Chi</creator><creator>Chen, Jui Jiun</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><orcidid>https://orcid.org/0000-0002-9662-2976</orcidid></search><sort><creationdate>20230323</creationdate><title>Field-induced second-harmonic generation induced by distorted soft chiral crystal</title><author>Chen, Hui-Yu ; Araoka, Fumito ; Lee, Fang-Yu ; Lee, Chi ; Chen, Jui Jiun</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c330t-70a2f76166ffe285e17529b0bf61e08aaad518791da5d4305c001a38979a6d5e3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2023</creationdate><topic>blue phase</topic><topic>electro-optical response</topic><topic>lattice deformation</topic><topic>liquid crystals</topic><topic>second-harmonic generation</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chen, Hui-Yu</creatorcontrib><creatorcontrib>Araoka, Fumito</creatorcontrib><creatorcontrib>Lee, Fang-Yu</creatorcontrib><creatorcontrib>Lee, Chi</creatorcontrib><creatorcontrib>Chen, Jui Jiun</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of physics. D, Applied physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chen, Hui-Yu</au><au>Araoka, Fumito</au><au>Lee, Fang-Yu</au><au>Lee, Chi</au><au>Chen, Jui Jiun</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Field-induced second-harmonic generation induced by distorted soft chiral crystal</atitle><jtitle>Journal of physics. D, Applied physics</jtitle><stitle>JPhysD</stitle><addtitle>J. Phys. D: Appl. Phys</addtitle><date>2023-03-23</date><risdate>2023</risdate><volume>56</volume><issue>12</issue><spage>125303</spage><pages>125303-</pages><issn>0022-3727</issn><eissn>1361-6463</eissn><coden>JPAPBE</coden><abstract>The nonlinear optical response of soft chiral crystal system-blue-phase (BP) liquid crystals was studied experimentally using a second-harmonic-generation (SHG) microscope. With the aid of the SHG microscope (SHM), the internal coupling between the polarization and structural deformation was visualized in a short time. In this study, a fringing field, formed at the electrode edges, causes lattice deformation of the cubic BPs, which contributes to the flexoelectric-optic response and field-induced SHG at low frequencies. Using the SHM, we can observe the spatial distribution of the induced polarization in the BPs, and the mean SHG intensity of the cubic BP depends quadratically on the strength of the electric field at a lower value. As the applied electric field increases, the structure of the BPs transfers to the chiral nematic phase (N*), and then the SHG intensity remains constant. Compared to the mean intensities of the SHG signal in N* and the different BPs in the low electric field, the SHG signal caused by the lattice deformation in BPs is weaker in N* and depends on the cubic structure of the BPs. The experimental results demonstrate that through the SHM, the influence of the inhomogeneous electric field on the BPs can be exhibited clearly because the response of the SHG signal in BPs is sensitive to field-induced lattice deformation and phase transitions between the BPs and chiral nematic. This will help us elucidate the mechanism of the secondary electro-optical response in BPs and for further improvement and development of high-performance photonic devices using BPs.</abstract><pub>IOP Publishing</pub><doi>10.1088/1361-6463/acbe09</doi><tpages>8</tpages><orcidid>https://orcid.org/0000-0002-9662-2976</orcidid></addata></record> |
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subjects | blue phase electro-optical response lattice deformation liquid crystals second-harmonic generation |
title | Field-induced second-harmonic generation induced by distorted soft chiral crystal |
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