3D Imaging and Simulation of the Polarisation Distribution in Molecular Crystals
The spatial polarisation distribution in inhomogeneously polar molecular crystals has been imaged by scanning pyroelectric tomography and simulated by a Markov process. The experimental technique combines scanning pyroelectric microscopy (SPEM) with layerwise thinning of crystals. The SPEM probes th...
Gespeichert in:
Veröffentlicht in: | Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals Molecular crystals and liquid crystals, 2000-01, Vol.338 (1), p.243-256 |
---|---|
Hauptverfasser: | , , , |
Format: | Artikel |
Sprache: | eng |
Schlagworte: | |
Online-Zugang: | Volltext |
Tags: |
Tag hinzufügen
Keine Tags, Fügen Sie den ersten Tag hinzu!
|
container_end_page | 256 |
---|---|
container_issue | 1 |
container_start_page | 243 |
container_title | Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals |
container_volume | 338 |
creator | Quintel, Andrea Roth, Stephan W. Hulliger, Jürg Wübbenhorst, Michael |
description | The spatial polarisation distribution in inhomogeneously polar molecular crystals has been imaged by scanning pyroelectric tomography and simulated by a Markov process. The experimental technique combines scanning pyroelectric microscopy (SPEM) with layerwise thinning of crystals. The SPEM probes the local spontaneous polarisation by its temperature dependence (pyroelectric effect). A focused and intensity modulated laser beam scans the surface of a polar sample and induces temperature changes in a volume depending on the laser spot size and the thermal diffusion length λ
th
. Since high lateral resolution of the SPEM is only available for small values of λ
th
. depth information to a resolution of ∼ 10 μ is achieved by repeated scanning and stepwise thinning of crystals. A layer by layer technique can provide 3D imaging of the polar ordering with a lateral resolution of ∼ 20 μ at a probed layer thickness of ∼ 10 μ. Applied to perhydrotriphenylene (PHTP) co-crystallised with 1-(4-nitrophenyl)piperazine (NPP) two conical macro-domains of opposite and nearly constant polarisation were found. The SPEM results are in good agreement with a homogeneous Markov chain model driving dipolar molecules into a parallel state within channels of PHTP. The new tomographic view reveals that the opposing cones are partially overlapping at the tips. Lateral growth processes are assumed to be responsible for this. A theoretical section covers aspects of the convergency into the polar state and the length of polar chains discussed in terms of intermolecular interaction energies. |
doi_str_mv | 10.1080/10587250008024433 |
format | Article |
fullrecord | <record><control><sourceid>pascalfrancis_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1080_10587250008024433</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>794408</sourcerecordid><originalsourceid>FETCH-LOGICAL-c372t-7651d7bd7c62a0bf0e2186f4608221ad2c6e8c78042df6a00679ddde131276323</originalsourceid><addsrcrecordid>eNqFkE9LAzEUxHNQsFY_gLeA59WXP5tswYu0WgsVCyp4W9JkUyO7m5KkaL-9W1e9FPQ0zDC_92AQOiNwQaCASwJ5IWkO0BnKOWMHaLDLsi58OULHMb4BUJJzPkALNsGzRq1cu8KqNfjRNZtaJedb7C1OrxVe-FoFF_ts4mIKbrn5Mq7F976udAcEPA7bmFQdT9Ch7aQ6_dYher69eRrfZfOH6Wx8Pc80kzRlUuTEyKWRWlAFSwsVJYWwXEBBKVGGalEVWhbAqbFCAQg5MsZUhBEqBaNsiEh_VwcfY6hsuQ6uUWFbEih3M5R7M3TMec-sVdSqtkG12sVfUI44h6JrXfUt11ofGvXuQ23KpLa1Dz8I--uJ_Bffo8r0kdgn88eDCw</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>3D Imaging and Simulation of the Polarisation Distribution in Molecular Crystals</title><source>Taylor & Francis</source><creator>Quintel, Andrea ; Roth, Stephan W. ; Hulliger, Jürg ; Wübbenhorst, Michael</creator><creatorcontrib>Quintel, Andrea ; Roth, Stephan W. ; Hulliger, Jürg ; Wübbenhorst, Michael</creatorcontrib><description>The spatial polarisation distribution in inhomogeneously polar molecular crystals has been imaged by scanning pyroelectric tomography and simulated by a Markov process. The experimental technique combines scanning pyroelectric microscopy (SPEM) with layerwise thinning of crystals. The SPEM probes the local spontaneous polarisation by its temperature dependence (pyroelectric effect). A focused and intensity modulated laser beam scans the surface of a polar sample and induces temperature changes in a volume depending on the laser spot size and the thermal diffusion length λ
th
. Since high lateral resolution of the SPEM is only available for small values of λ
th
. depth information to a resolution of ∼ 10 μ is achieved by repeated scanning and stepwise thinning of crystals. A layer by layer technique can provide 3D imaging of the polar ordering with a lateral resolution of ∼ 20 μ at a probed layer thickness of ∼ 10 μ. Applied to perhydrotriphenylene (PHTP) co-crystallised with 1-(4-nitrophenyl)piperazine (NPP) two conical macro-domains of opposite and nearly constant polarisation were found. The SPEM results are in good agreement with a homogeneous Markov chain model driving dipolar molecules into a parallel state within channels of PHTP. The new tomographic view reveals that the opposing cones are partially overlapping at the tips. Lateral growth processes are assumed to be responsible for this. A theoretical section covers aspects of the convergency into the polar state and the length of polar chains discussed in terms of intermolecular interaction energies.</description><identifier>ISSN: 1058-725X</identifier><identifier>DOI: 10.1080/10587250008024433</identifier><language>eng</language><publisher>Philadelphia, PA: Taylor & Francis Group</publisher><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties ; Dielectric properties of solids and liquids ; Dielectrics, piezoelectrics, and ferroelectrics and their properties ; Exact sciences and technology ; inclusion compound ; Markov process ; Physics ; Polarization and depolarization ; Pyroelectric and electrocaloric effects ; pyroelectricity ; scanning probe microscopy ; tomography</subject><ispartof>Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals, 2000-01, Vol.338 (1), p.243-256</ispartof><rights>Copyright Taylor & Francis Group, LLC 2000</rights><rights>2001 INIST-CNRS</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c372t-7651d7bd7c62a0bf0e2186f4608221ad2c6e8c78042df6a00679ddde131276323</citedby><cites>FETCH-LOGICAL-c372t-7651d7bd7c62a0bf0e2186f4608221ad2c6e8c78042df6a00679ddde131276323</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://www.tandfonline.com/doi/pdf/10.1080/10587250008024433$$EPDF$$P50$$Ginformaworld$$H</linktopdf><linktohtml>$$Uhttps://www.tandfonline.com/doi/full/10.1080/10587250008024433$$EHTML$$P50$$Ginformaworld$$H</linktohtml><link.rule.ids>314,776,780,4010,27900,27901,27902,59620,60409</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&idt=794408$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Quintel, Andrea</creatorcontrib><creatorcontrib>Roth, Stephan W.</creatorcontrib><creatorcontrib>Hulliger, Jürg</creatorcontrib><creatorcontrib>Wübbenhorst, Michael</creatorcontrib><title>3D Imaging and Simulation of the Polarisation Distribution in Molecular Crystals</title><title>Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals</title><description>The spatial polarisation distribution in inhomogeneously polar molecular crystals has been imaged by scanning pyroelectric tomography and simulated by a Markov process. The experimental technique combines scanning pyroelectric microscopy (SPEM) with layerwise thinning of crystals. The SPEM probes the local spontaneous polarisation by its temperature dependence (pyroelectric effect). A focused and intensity modulated laser beam scans the surface of a polar sample and induces temperature changes in a volume depending on the laser spot size and the thermal diffusion length λ
th
. Since high lateral resolution of the SPEM is only available for small values of λ
th
. depth information to a resolution of ∼ 10 μ is achieved by repeated scanning and stepwise thinning of crystals. A layer by layer technique can provide 3D imaging of the polar ordering with a lateral resolution of ∼ 20 μ at a probed layer thickness of ∼ 10 μ. Applied to perhydrotriphenylene (PHTP) co-crystallised with 1-(4-nitrophenyl)piperazine (NPP) two conical macro-domains of opposite and nearly constant polarisation were found. The SPEM results are in good agreement with a homogeneous Markov chain model driving dipolar molecules into a parallel state within channels of PHTP. The new tomographic view reveals that the opposing cones are partially overlapping at the tips. Lateral growth processes are assumed to be responsible for this. A theoretical section covers aspects of the convergency into the polar state and the length of polar chains discussed in terms of intermolecular interaction energies.</description><subject>Condensed matter: electronic structure, electrical, magnetic, and optical properties</subject><subject>Dielectric properties of solids and liquids</subject><subject>Dielectrics, piezoelectrics, and ferroelectrics and their properties</subject><subject>Exact sciences and technology</subject><subject>inclusion compound</subject><subject>Markov process</subject><subject>Physics</subject><subject>Polarization and depolarization</subject><subject>Pyroelectric and electrocaloric effects</subject><subject>pyroelectricity</subject><subject>scanning probe microscopy</subject><subject>tomography</subject><issn>1058-725X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2000</creationdate><recordtype>article</recordtype><recordid>eNqFkE9LAzEUxHNQsFY_gLeA59WXP5tswYu0WgsVCyp4W9JkUyO7m5KkaL-9W1e9FPQ0zDC_92AQOiNwQaCASwJ5IWkO0BnKOWMHaLDLsi58OULHMb4BUJJzPkALNsGzRq1cu8KqNfjRNZtaJedb7C1OrxVe-FoFF_ts4mIKbrn5Mq7F976udAcEPA7bmFQdT9Ch7aQ6_dYher69eRrfZfOH6Wx8Pc80kzRlUuTEyKWRWlAFSwsVJYWwXEBBKVGGalEVWhbAqbFCAQg5MsZUhBEqBaNsiEh_VwcfY6hsuQ6uUWFbEih3M5R7M3TMec-sVdSqtkG12sVfUI44h6JrXfUt11ofGvXuQ23KpLa1Dz8I--uJ_Bffo8r0kdgn88eDCw</recordid><startdate>20000101</startdate><enddate>20000101</enddate><creator>Quintel, Andrea</creator><creator>Roth, Stephan W.</creator><creator>Hulliger, Jürg</creator><creator>Wübbenhorst, Michael</creator><general>Taylor & Francis Group</general><general>Gordon and Breach</general><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20000101</creationdate><title>3D Imaging and Simulation of the Polarisation Distribution in Molecular Crystals</title><author>Quintel, Andrea ; Roth, Stephan W. ; Hulliger, Jürg ; Wübbenhorst, Michael</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c372t-7651d7bd7c62a0bf0e2186f4608221ad2c6e8c78042df6a00679ddde131276323</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2000</creationdate><topic>Condensed matter: electronic structure, electrical, magnetic, and optical properties</topic><topic>Dielectric properties of solids and liquids</topic><topic>Dielectrics, piezoelectrics, and ferroelectrics and their properties</topic><topic>Exact sciences and technology</topic><topic>inclusion compound</topic><topic>Markov process</topic><topic>Physics</topic><topic>Polarization and depolarization</topic><topic>Pyroelectric and electrocaloric effects</topic><topic>pyroelectricity</topic><topic>scanning probe microscopy</topic><topic>tomography</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Quintel, Andrea</creatorcontrib><creatorcontrib>Roth, Stephan W.</creatorcontrib><creatorcontrib>Hulliger, Jürg</creatorcontrib><creatorcontrib>Wübbenhorst, Michael</creatorcontrib><collection>Pascal-Francis</collection><collection>CrossRef</collection><jtitle>Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Quintel, Andrea</au><au>Roth, Stephan W.</au><au>Hulliger, Jürg</au><au>Wübbenhorst, Michael</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>3D Imaging and Simulation of the Polarisation Distribution in Molecular Crystals</atitle><jtitle>Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals</jtitle><date>2000-01-01</date><risdate>2000</risdate><volume>338</volume><issue>1</issue><spage>243</spage><epage>256</epage><pages>243-256</pages><issn>1058-725X</issn><abstract>The spatial polarisation distribution in inhomogeneously polar molecular crystals has been imaged by scanning pyroelectric tomography and simulated by a Markov process. The experimental technique combines scanning pyroelectric microscopy (SPEM) with layerwise thinning of crystals. The SPEM probes the local spontaneous polarisation by its temperature dependence (pyroelectric effect). A focused and intensity modulated laser beam scans the surface of a polar sample and induces temperature changes in a volume depending on the laser spot size and the thermal diffusion length λ
th
. Since high lateral resolution of the SPEM is only available for small values of λ
th
. depth information to a resolution of ∼ 10 μ is achieved by repeated scanning and stepwise thinning of crystals. A layer by layer technique can provide 3D imaging of the polar ordering with a lateral resolution of ∼ 20 μ at a probed layer thickness of ∼ 10 μ. Applied to perhydrotriphenylene (PHTP) co-crystallised with 1-(4-nitrophenyl)piperazine (NPP) two conical macro-domains of opposite and nearly constant polarisation were found. The SPEM results are in good agreement with a homogeneous Markov chain model driving dipolar molecules into a parallel state within channels of PHTP. The new tomographic view reveals that the opposing cones are partially overlapping at the tips. Lateral growth processes are assumed to be responsible for this. A theoretical section covers aspects of the convergency into the polar state and the length of polar chains discussed in terms of intermolecular interaction energies.</abstract><cop>Philadelphia, PA</cop><pub>Taylor & Francis Group</pub><doi>10.1080/10587250008024433</doi><tpages>14</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1058-725X |
ispartof | Molecular crystals and liquid crystals science and technology. Section A, Molecular crystals and liquid crystals, 2000-01, Vol.338 (1), p.243-256 |
issn | 1058-725X |
language | eng |
recordid | cdi_crossref_primary_10_1080_10587250008024433 |
source | Taylor & Francis |
subjects | Condensed matter: electronic structure, electrical, magnetic, and optical properties Dielectric properties of solids and liquids Dielectrics, piezoelectrics, and ferroelectrics and their properties Exact sciences and technology inclusion compound Markov process Physics Polarization and depolarization Pyroelectric and electrocaloric effects pyroelectricity scanning probe microscopy tomography |
title | 3D Imaging and Simulation of the Polarisation Distribution in Molecular Crystals |
url | https://sfx.bib-bvb.de/sfx_tum?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-31T02%3A14%3A40IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-pascalfrancis_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=3D%20Imaging%20and%20Simulation%20of%20the%20Polarisation%20Distribution%20in%20Molecular%20Crystals&rft.jtitle=Molecular%20crystals%20and%20liquid%20crystals%20science%20and%20technology.%20Section%20A,%20Molecular%20crystals%20and%20liquid%20crystals&rft.au=Quintel,%20Andrea&rft.date=2000-01-01&rft.volume=338&rft.issue=1&rft.spage=243&rft.epage=256&rft.pages=243-256&rft.issn=1058-725X&rft_id=info:doi/10.1080/10587250008024433&rft_dat=%3Cpascalfrancis_cross%3E794408%3C/pascalfrancis_cross%3E%3Curl%3E%3C/url%3E&disable_directlink=true&sfx.directlink=off&sfx.report_link=0&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |