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High energy-resolution electron energy-loss spectroscopy and soft-x-ray emission spectroscopy studies of amorphous diamond transformed from neutron-irradiated graphite
High energy-resolution electron energy-loss spectroscopy measurements were performed for amorphous diamond (am-DIA), which was synthesized from neutron-irradiated graphite by shock compression, by using a monochromator transmission electron microscope (TEM). Soft-X-ray emission spectroscopy (SXES) m...
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Published in: | Journal of physics. Conference series 2014-05, Vol.500 (19), p.192013-5 |
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container_start_page | 192013 |
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creator | Sato, Y Terauchi, M Niwase, K Nakamura, K G Atou, T Iwata, T |
description | High energy-resolution electron energy-loss spectroscopy measurements were performed for amorphous diamond (am-DIA), which was synthesized from neutron-irradiated graphite by shock compression, by using a monochromator transmission electron microscope (TEM). Soft-X-ray emission spectroscopy (SXES) measurements were performed by a wavelength-dispersive type spectrometer attached to the monochromator TEM. A volume plasmon peak of am-DIA is observed at 32.5 eV, which is a little smaller than that of crystalline diamond (c-DIA). The smaller plasmon energy of am-DIA indicates a smaller valence electron density of am-DIA than that of c-DIA. From the onset energies of the K-shell excitation and the SXES spectra, the band gap energy of am-DIA is estimated to be 4 eV, which is similar to the value, 3.9 eV, from the valence electron excitation spectrum and reported values, 3.5-4.5 eV, for the am-DIA synthesized from C60 fullerene by shock compression. |
doi_str_mv | 10.1088/1742-6596/500/19/192013 |
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Soft-X-ray emission spectroscopy (SXES) measurements were performed by a wavelength-dispersive type spectrometer attached to the monochromator TEM. A volume plasmon peak of am-DIA is observed at 32.5 eV, which is a little smaller than that of crystalline diamond (c-DIA). The smaller plasmon energy of am-DIA indicates a smaller valence electron density of am-DIA than that of c-DIA. From the onset energies of the K-shell excitation and the SXES spectra, the band gap energy of am-DIA is estimated to be 4 eV, which is similar to the value, 3.9 eV, from the valence electron excitation spectrum and reported values, 3.5-4.5 eV, for the am-DIA synthesized from C60 fullerene by shock compression.</description><identifier>ISSN: 1742-6596</identifier><identifier>ISSN: 1742-6588</identifier><identifier>EISSN: 1742-6596</identifier><identifier>DOI: 10.1088/1742-6596/500/19/192013</identifier><language>eng</language><publisher>Bristol: IOP Publishing</publisher><subject>Buckminsterfullerene ; Compressing ; Diamonds ; Electron density ; Electron energy ; Electron energy loss spectroscopy ; Electrons ; Emission analysis ; Emission spectroscopy ; Energy ; Energy gap ; Excitation ; Excitation spectra ; Fullerenes ; Graphite ; Monochromators ; Physics ; Spectroscopic analysis ; Spectroscopy ; Spectrum analysis ; Synthesis ; Transmission electron microscopy</subject><ispartof>Journal of physics. 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Conference series</title><description>High energy-resolution electron energy-loss spectroscopy measurements were performed for amorphous diamond (am-DIA), which was synthesized from neutron-irradiated graphite by shock compression, by using a monochromator transmission electron microscope (TEM). Soft-X-ray emission spectroscopy (SXES) measurements were performed by a wavelength-dispersive type spectrometer attached to the monochromator TEM. A volume plasmon peak of am-DIA is observed at 32.5 eV, which is a little smaller than that of crystalline diamond (c-DIA). The smaller plasmon energy of am-DIA indicates a smaller valence electron density of am-DIA than that of c-DIA. From the onset energies of the K-shell excitation and the SXES spectra, the band gap energy of am-DIA is estimated to be 4 eV, which is similar to the value, 3.9 eV, from the valence electron excitation spectrum and reported values, 3.5-4.5 eV, for the am-DIA synthesized from C60 fullerene by shock compression.</description><subject>Buckminsterfullerene</subject><subject>Compressing</subject><subject>Diamonds</subject><subject>Electron density</subject><subject>Electron energy</subject><subject>Electron energy loss spectroscopy</subject><subject>Electrons</subject><subject>Emission analysis</subject><subject>Emission spectroscopy</subject><subject>Energy</subject><subject>Energy gap</subject><subject>Excitation</subject><subject>Excitation spectra</subject><subject>Fullerenes</subject><subject>Graphite</subject><subject>Monochromators</subject><subject>Physics</subject><subject>Spectroscopic analysis</subject><subject>Spectroscopy</subject><subject>Spectrum analysis</subject><subject>Synthesis</subject><subject>Transmission electron microscopy</subject><issn>1742-6596</issn><issn>1742-6588</issn><issn>1742-6596</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>PIMPY</sourceid><recordid>eNpdkc9KxDAQxosouK4-gwEvXuomTZu0R1n8Bwte9Byy6WS3S9vUTAruE_mapq6IGgIZZn7fZJIvSS4ZvWG0LBdM5lkqikosCkoXrIo7o4wfJbOfyvGv-DQ5Q9xRyuOSs-TjsdlsCfTgN_vUA7p2DI3rCbRggp-CQ6l1iASHryQaN-yJ7muCzob0PfV6T6BrECflHwjDWDeAxFmiO-eHrRuR1E2Mozp43aN1voOaWO860sM43Zk23usIhZjfeD1smwDnyYnVLcLF9zlPXu_vXpaP6er54Wl5u0pNLmVIS8Mqmq1Lm9UllIIKLmqmBecl03QNtoBCZIxRURhpcs0hqzgVdW2ZYaakFZ8n14e-g3dvI2BQ8V0G2lb3EGdXTEY9FbnMI3r1D9250fdxOpUVUoisygsZKXmgTPwT9GDV4JtO-71iVE0GqskaNVmjooGKVepgIP8EOSWTOg</recordid><startdate>20140507</startdate><enddate>20140507</enddate><creator>Sato, Y</creator><creator>Terauchi, M</creator><creator>Niwase, K</creator><creator>Nakamura, K G</creator><creator>Atou, T</creator><creator>Iwata, T</creator><general>IOP Publishing</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>8FE</scope><scope>8FG</scope><scope>ABUWG</scope><scope>AFKRA</scope><scope>ARAPS</scope><scope>AZQEC</scope><scope>BENPR</scope><scope>BGLVJ</scope><scope>CCPQU</scope><scope>DWQXO</scope><scope>H8D</scope><scope>HCIFZ</scope><scope>L7M</scope><scope>P5Z</scope><scope>P62</scope><scope>PIMPY</scope><scope>PQEST</scope><scope>PQQKQ</scope><scope>PQUKI</scope><scope>PRINS</scope><scope>7U5</scope><scope>8BQ</scope><scope>JG9</scope></search><sort><creationdate>20140507</creationdate><title>High energy-resolution electron energy-loss spectroscopy and soft-x-ray emission spectroscopy studies of amorphous diamond transformed from neutron-irradiated graphite</title><author>Sato, Y ; 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Conference series</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Sato, Y</au><au>Terauchi, M</au><au>Niwase, K</au><au>Nakamura, K G</au><au>Atou, T</au><au>Iwata, T</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>High energy-resolution electron energy-loss spectroscopy and soft-x-ray emission spectroscopy studies of amorphous diamond transformed from neutron-irradiated graphite</atitle><jtitle>Journal of physics. Conference series</jtitle><date>2014-05-07</date><risdate>2014</risdate><volume>500</volume><issue>19</issue><spage>192013</spage><epage>5</epage><pages>192013-5</pages><issn>1742-6596</issn><issn>1742-6588</issn><eissn>1742-6596</eissn><abstract>High energy-resolution electron energy-loss spectroscopy measurements were performed for amorphous diamond (am-DIA), which was synthesized from neutron-irradiated graphite by shock compression, by using a monochromator transmission electron microscope (TEM). Soft-X-ray emission spectroscopy (SXES) measurements were performed by a wavelength-dispersive type spectrometer attached to the monochromator TEM. A volume plasmon peak of am-DIA is observed at 32.5 eV, which is a little smaller than that of crystalline diamond (c-DIA). The smaller plasmon energy of am-DIA indicates a smaller valence electron density of am-DIA than that of c-DIA. From the onset energies of the K-shell excitation and the SXES spectra, the band gap energy of am-DIA is estimated to be 4 eV, which is similar to the value, 3.9 eV, from the valence electron excitation spectrum and reported values, 3.5-4.5 eV, for the am-DIA synthesized from C60 fullerene by shock compression.</abstract><cop>Bristol</cop><pub>IOP Publishing</pub><doi>10.1088/1742-6596/500/19/192013</doi><tpages>5</tpages><oa>free_for_read</oa></addata></record> |
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subjects | Buckminsterfullerene Compressing Diamonds Electron density Electron energy Electron energy loss spectroscopy Electrons Emission analysis Emission spectroscopy Energy Energy gap Excitation Excitation spectra Fullerenes Graphite Monochromators Physics Spectroscopic analysis Spectroscopy Spectrum analysis Synthesis Transmission electron microscopy |
title | High energy-resolution electron energy-loss spectroscopy and soft-x-ray emission spectroscopy studies of amorphous diamond transformed from neutron-irradiated graphite |
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