On the crystal structure of Cr2N precipitates in high-nitrogen austenitic stainless steel. III. Neutron diffraction study on the ordered Cr2N superstructure

The ordered structure of Cr2N precipitates in high‐nitrogen austenitic steel was investigated utilizing high‐resolution neutron powder diffractometry (HRPD). On the basis of the Rietveld refinement of neutron diffraction patterns, the ordered Cr2N superstructure was confirmed to be trigonal (space g...

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Veröffentlicht in:Acta crystallographica. Section B, Structural science Structural science, 2006-12, Vol.62 (6), p.979-986
Hauptverfasser: Kim, Sung-Joon, Shin, Eunjoo, Takaki, Setsuo, Lee, Tae-Ho
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Shin, Eunjoo
Takaki, Setsuo
Lee, Tae-Ho
description The ordered structure of Cr2N precipitates in high‐nitrogen austenitic steel was investigated utilizing high‐resolution neutron powder diffractometry (HRPD). On the basis of the Rietveld refinement of neutron diffraction patterns, the ordered Cr2N superstructure was confirmed to be trigonal (space group ), with lattice parameters a = 4.800 (4) and c = 4.472 (5) Å, as suggested in previous transmission electron microscopy studies [Lee, Oh, Han, Lee, Kim & Takaki (2005). Acta Cryst. B61, 137–144; Lee, Kim & Takaki (2006). Acta Cryst. B62, 190–196]. The occupancies of the N atoms in four crystallographic sites [1(a), 1(b), 2(d) and 2(c) Wyckoff sites] were determined to be 1.00 (5), 0.0, 0.74 (9) and 0.12 (3), respectively, reflecting a partial disordering of N atoms along the c axis. The position of the metal atom was specified to be x = 0.346 (8) and z = 0.244 (6), corresponding to a deviation from the ideal position (x = 0.333 and z = 0.250). This deviation caused the ‐type superlattice reflection to appear. A comparison between the ideal and measured crystal structures of Cr2N was performed using a computer simulation of selected‐area diffraction patterns.
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III. Neutron diffraction study on the ordered Cr2N superstructure</title><source>Wiley Online Library Journals Frontfile Complete</source><source>Free Full-Text Journals in Chemistry</source><creator>Kim, Sung-Joon ; Shin, Eunjoo ; Takaki, Setsuo ; Lee, Tae-Ho</creator><creatorcontrib>Kim, Sung-Joon ; Shin, Eunjoo ; Takaki, Setsuo ; Lee, Tae-Ho</creatorcontrib><description>The ordered structure of Cr2N precipitates in high‐nitrogen austenitic steel was investigated utilizing high‐resolution neutron powder diffractometry (HRPD). On the basis of the Rietveld refinement of neutron diffraction patterns, the ordered Cr2N superstructure was confirmed to be trigonal (space group ), with lattice parameters a = 4.800 (4) and c = 4.472 (5) Å, as suggested in previous transmission electron microscopy studies [Lee, Oh, Han, Lee, Kim &amp; Takaki (2005). Acta Cryst. B61, 137–144; Lee, Kim &amp; Takaki (2006). Acta Cryst. B62, 190–196]. The occupancies of the N atoms in four crystallographic sites [1(a), 1(b), 2(d) and 2(c) Wyckoff sites] were determined to be 1.00 (5), 0.0, 0.74 (9) and 0.12 (3), respectively, reflecting a partial disordering of N atoms along the c axis. The position of the metal atom was specified to be x = 0.346 (8) and z = 0.244 (6), corresponding to a deviation from the ideal position (x = 0.333 and z = 0.250). This deviation caused the ‐type superlattice reflection to appear. 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III. Neutron diffraction study on the ordered Cr2N superstructure</title><title>Acta crystallographica. Section B, Structural science</title><addtitle>Acta Cryst. B</addtitle><description>The ordered structure of Cr2N precipitates in high‐nitrogen austenitic steel was investigated utilizing high‐resolution neutron powder diffractometry (HRPD). On the basis of the Rietveld refinement of neutron diffraction patterns, the ordered Cr2N superstructure was confirmed to be trigonal (space group ), with lattice parameters a = 4.800 (4) and c = 4.472 (5) Å, as suggested in previous transmission electron microscopy studies [Lee, Oh, Han, Lee, Kim &amp; Takaki (2005). Acta Cryst. B61, 137–144; Lee, Kim &amp; Takaki (2006). Acta Cryst. B62, 190–196]. The occupancies of the N atoms in four crystallographic sites [1(a), 1(b), 2(d) and 2(c) Wyckoff sites] were determined to be 1.00 (5), 0.0, 0.74 (9) and 0.12 (3), respectively, reflecting a partial disordering of N atoms along the c axis. The position of the metal atom was specified to be x = 0.346 (8) and z = 0.244 (6), corresponding to a deviation from the ideal position (x = 0.333 and z = 0.250). This deviation caused the ‐type superlattice reflection to appear. A comparison between the ideal and measured crystal structures of Cr2N was performed using a computer simulation of selected‐area diffraction patterns.</description><subject>Chemical compounds</subject><subject>Comparative studies</subject><subject>Condensed matter: structure, mechanical and thermal properties</subject><subject>Cr2N</subject><subject>Crystal lattices</subject><subject>Crystal structure</subject><subject>Crystallography</subject><subject>Diffraction</subject><subject>Equations of state, phase equilibria, and phase transitions</subject><subject>Exact sciences and technology</subject><subject>General studies of phase transitions</subject><subject>Inorganic compounds</subject><subject>neutron diffraction</subject><subject>Neutrons</subject><subject>Nitrogen</subject><subject>Order-disorder and statistical mechanics of model systems</subject><subject>ordered structures</subject><subject>partial disorder</subject><subject>Physics</subject><subject>Stainless steel</subject><subject>Structure of solids and liquids; crystallography</subject><subject>Structure of specific crystalline solids</subject><issn>0108-7681</issn><issn>2052-5192</issn><issn>1600-5740</issn><issn>2052-5206</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2006</creationdate><recordtype>article</recordtype><recordid>eNplkVGL1DAQx4Mo3nr6AXyRIOhb10nTtN3Hs3h3C2UPURGfQppMb3N2216S4u138cOava53oBDIDP_fzH-YIeQ1gyVjUHz4AgzKIi8Z5MAzVvAnZMFygEQUGTwli4OcHPQT8sL7GwDIWAnPyQkropILWJDfVz0NW6Ta7X1QHfXBTTpMDunQ0sqlGzo61Ha0QQX01PZ0a6-3SW-DG66xp2ryAWNmdSxVtu_Q-xghdku6Xq-XdINTRHtqbNs6pYONsQ-T2dNhdh6cQYdmNvPTiO5hhpfkWas6j6-O_yn5dv7pa3WZ1FcX6-qsTmzGVpCYPC3aZpVDy3hh7l-rWpXiqi0xZmWDwjRC5RpMumqajHHelpwZzTJheMpPyfu57-iG2wl9kDvrNXad6nGYvIwbFGnGIYJv_wFvhsn1cTaZAmcHrojQmyM0NTs0cnR2p9xe_l16BN4dAeW16uJaem39IxdHSxkTkStn7pftcP-ogzxcX_53fXn242NdCbi3SOZSG29x91Cq3E-ZF7wQ8vvmQpZ1ldafN0Je8j8T_7Il</recordid><startdate>200612</startdate><enddate>200612</enddate><creator>Kim, Sung-Joon</creator><creator>Shin, Eunjoo</creator><creator>Takaki, Setsuo</creator><creator>Lee, Tae-Ho</creator><general>Blackwell Publishing Ltd</general><general>Blackwell</general><scope>BSCLL</scope><scope>IQODW</scope><scope>NPM</scope><scope>7SR</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>7X8</scope></search><sort><creationdate>200612</creationdate><title>On the crystal structure of Cr2N precipitates in high-nitrogen austenitic stainless steel. 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B</addtitle><date>2006-12</date><risdate>2006</risdate><volume>62</volume><issue>6</issue><spage>979</spage><epage>986</epage><pages>979-986</pages><issn>0108-7681</issn><issn>2052-5192</issn><eissn>1600-5740</eissn><eissn>2052-5206</eissn><coden>ASBSDK</coden><abstract>The ordered structure of Cr2N precipitates in high‐nitrogen austenitic steel was investigated utilizing high‐resolution neutron powder diffractometry (HRPD). On the basis of the Rietveld refinement of neutron diffraction patterns, the ordered Cr2N superstructure was confirmed to be trigonal (space group ), with lattice parameters a = 4.800 (4) and c = 4.472 (5) Å, as suggested in previous transmission electron microscopy studies [Lee, Oh, Han, Lee, Kim &amp; Takaki (2005). Acta Cryst. B61, 137–144; Lee, Kim &amp; Takaki (2006). Acta Cryst. B62, 190–196]. The occupancies of the N atoms in four crystallographic sites [1(a), 1(b), 2(d) and 2(c) Wyckoff sites] were determined to be 1.00 (5), 0.0, 0.74 (9) and 0.12 (3), respectively, reflecting a partial disordering of N atoms along the c axis. The position of the metal atom was specified to be x = 0.346 (8) and z = 0.244 (6), corresponding to a deviation from the ideal position (x = 0.333 and z = 0.250). This deviation caused the ‐type superlattice reflection to appear. A comparison between the ideal and measured crystal structures of Cr2N was performed using a computer simulation of selected‐area diffraction patterns.</abstract><cop>5 Abbey Square, Chester, Cheshire CH1 2HU, England</cop><pub>Blackwell Publishing Ltd</pub><pmid>17108650</pmid><doi>10.1107/S0108768106034173</doi><tpages>8</tpages></addata></record>
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source Wiley Online Library Journals Frontfile Complete; Free Full-Text Journals in Chemistry
subjects Chemical compounds
Comparative studies
Condensed matter: structure, mechanical and thermal properties
Cr2N
Crystal lattices
Crystal structure
Crystallography
Diffraction
Equations of state, phase equilibria, and phase transitions
Exact sciences and technology
General studies of phase transitions
Inorganic compounds
neutron diffraction
Neutrons
Nitrogen
Order-disorder and statistical mechanics of model systems
ordered structures
partial disorder
Physics
Stainless steel
Structure of solids and liquids
crystallography
Structure of specific crystalline solids
title On the crystal structure of Cr2N precipitates in high-nitrogen austenitic stainless steel. III. Neutron diffraction study on the ordered Cr2N superstructure
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