Properties of α-monoclinic selenium

<p>The growth of bulky and platelet shaped α-monoclinic crystals is discussed. A simple method is devised for identifying and orienting them.</p> <p>The density, previously in disagreement with the value calculated from x-ray studies, is carefully redetermined, and found to be in...

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Main Author: Taynai, Joseph Dean
Format: Others
Published: 1970
Online Access:https://thesis.library.caltech.edu/8671/1/Taynai_JD_1970.pdf
Taynai, Joseph Dean (1970) Properties of α-monoclinic selenium. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/2T9A-6F21. https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539 <https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539>
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spelling ndltd-CALTECH-oai-thesis.library.caltech.edu-86712019-12-22T03:09:45Z Properties of α-monoclinic selenium Taynai, Joseph Dean <p>The growth of bulky and platelet shaped α-monoclinic crystals is discussed. A simple method is devised for identifying and orienting them.</p> <p>The density, previously in disagreement with the value calculated from x-ray studies, is carefully redetermined, and found to be in good agreement with the latter.</p> <p>The relative dielectric constant is determined, an effort being made to eliminate errors inherent in previous measurements, which have not been in agreement. A two parameter model is derived which explains the anisotropy in the relative dielectric constant of orthorhombic sulfur, which is also composed of 8-atom puckered ring molecules. The model works less well for α-monoclinic selenium. The relative dielectric constant anisotropy is quite noticeable, being 6.06 along the crystal b axis, and 8.52-8.93 normal to the axis.</p> <p>Thin crystal platelets of α-monoclinic selenium (less than 1µ thick) are used to extend optical transmission measurements up to 4.5eV. Previously the measurements extended up to 2.1 eV, limited by the thickness of the available crystals. The absorption edge is at 2.20 eV, with changes in slope of the absorption coefficient occurring at 2.85 eV and 3.8 eV. Measurement of transmission through solutions of selenium in CS_2 and trichlorethylene yield an absorption edge of 2.75 eV. There is evidence the selenium exists in solution partly as Se_8 rings, the building block of monoclinic selenium. Transmission is measured at low temperatures (80°K and 10°K) using the platelets. The absorption edge is at 2.38 eV and 2.39 eV, respectively, for the two temperatures. Measurements at low temperatures with polarized and unpolarized light reveal interesting absorption anisotropy near 2.65 eV.</p> 1970 Thesis NonPeerReviewed application/pdf https://thesis.library.caltech.edu/8671/1/Taynai_JD_1970.pdf https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539 Taynai, Joseph Dean (1970) Properties of α-monoclinic selenium. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/2T9A-6F21. https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539 <https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539> https://thesis.library.caltech.edu/8671/
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description <p>The growth of bulky and platelet shaped α-monoclinic crystals is discussed. A simple method is devised for identifying and orienting them.</p> <p>The density, previously in disagreement with the value calculated from x-ray studies, is carefully redetermined, and found to be in good agreement with the latter.</p> <p>The relative dielectric constant is determined, an effort being made to eliminate errors inherent in previous measurements, which have not been in agreement. A two parameter model is derived which explains the anisotropy in the relative dielectric constant of orthorhombic sulfur, which is also composed of 8-atom puckered ring molecules. The model works less well for α-monoclinic selenium. The relative dielectric constant anisotropy is quite noticeable, being 6.06 along the crystal b axis, and 8.52-8.93 normal to the axis.</p> <p>Thin crystal platelets of α-monoclinic selenium (less than 1µ thick) are used to extend optical transmission measurements up to 4.5eV. Previously the measurements extended up to 2.1 eV, limited by the thickness of the available crystals. The absorption edge is at 2.20 eV, with changes in slope of the absorption coefficient occurring at 2.85 eV and 3.8 eV. Measurement of transmission through solutions of selenium in CS_2 and trichlorethylene yield an absorption edge of 2.75 eV. There is evidence the selenium exists in solution partly as Se_8 rings, the building block of monoclinic selenium. Transmission is measured at low temperatures (80°K and 10°K) using the platelets. The absorption edge is at 2.38 eV and 2.39 eV, respectively, for the two temperatures. Measurements at low temperatures with polarized and unpolarized light reveal interesting absorption anisotropy near 2.65 eV.</p>
author Taynai, Joseph Dean
spellingShingle Taynai, Joseph Dean
Properties of α-monoclinic selenium
author_facet Taynai, Joseph Dean
author_sort Taynai, Joseph Dean
title Properties of α-monoclinic selenium
title_short Properties of α-monoclinic selenium
title_full Properties of α-monoclinic selenium
title_fullStr Properties of α-monoclinic selenium
title_full_unstemmed Properties of α-monoclinic selenium
title_sort properties of α-monoclinic selenium
publishDate 1970
url https://thesis.library.caltech.edu/8671/1/Taynai_JD_1970.pdf
Taynai, Joseph Dean (1970) Properties of α-monoclinic selenium. Dissertation (Ph.D.), California Institute of Technology. doi:10.7907/2T9A-6F21. https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539 <https://resolver.caltech.edu/CaltechTHESIS:10072014-094710539>
work_keys_str_mv AT taynaijosephdean propertiesofamonoclinicselenium
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