The nature of the structural phase transition from the hexagonal (4H) phase to the cubic (3C) phase of silver
The phase transition from the hexagonal 4H polytype of silver to the commonly known 3C (fcc) phase was studied in detail using x-ray diffraction, electron microscopy, differential scanning calorimetry and Raman spectroscopy. The phase transition is irreversible and accompanied by extensive microstru...
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Veröffentlicht in: | Journal of physics. Condensed matter 2014-03, Vol.26 (11), p.115405-115405 |
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description | The phase transition from the hexagonal 4H polytype of silver to the commonly known 3C (fcc) phase was studied in detail using x-ray diffraction, electron microscopy, differential scanning calorimetry and Raman spectroscopy. The phase transition is irreversible and accompanied by extensive microstructural changes and grain growth. Detailed scanning and isothermal calorimetric analysis suggests that it is an autocatalytic transformation. Though the calorimetric data suggest an exothermic first-order phase transition with an onset at 155.6 °C (for a heating rate of 2 K min−1) and a latent heat of 312.9 J g−1, the microstructure and the electrical resistance appear to change gradually from much lower temperatures. The 4H phase shows a Raman active mode at 64.3 cm−1 (at 4 K) that undergoes mode softening as the 4H → 3C transformation temperature is approached. A first-principles density functional theory calculation shows that the stacking fault energy of 4H-Ag increases monotonically with temperature. That 4H-Ag has a higher density of stacking faults than 3C-Ag, implies the metastability of the former at higher temperatures. Energetically, the 4H phase is intermediate between the hexagonal 2H phase and the 3C ground state, as indicated by the spontaneous transformation of the 2H to the 4H phase at −4 °C. Our data appear to indicate that the 4H-Ag phase is stabilized at reduced dimensions and thermally induced grain growth is probably responsible for triggering the irreversible transformation to cubic Ag. |
doi_str_mv | 10.1088/0953-8984/26/11/115405 |
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The phase transition is irreversible and accompanied by extensive microstructural changes and grain growth. Detailed scanning and isothermal calorimetric analysis suggests that it is an autocatalytic transformation. Though the calorimetric data suggest an exothermic first-order phase transition with an onset at 155.6 °C (for a heating rate of 2 K min−1) and a latent heat of 312.9 J g−1, the microstructure and the electrical resistance appear to change gradually from much lower temperatures. The 4H phase shows a Raman active mode at 64.3 cm−1 (at 4 K) that undergoes mode softening as the 4H → 3C transformation temperature is approached. A first-principles density functional theory calculation shows that the stacking fault energy of 4H-Ag increases monotonically with temperature. That 4H-Ag has a higher density of stacking faults than 3C-Ag, implies the metastability of the former at higher temperatures. Energetically, the 4H phase is intermediate between the hexagonal 2H phase and the 3C ground state, as indicated by the spontaneous transformation of the 2H to the 4H phase at −4 °C. Our data appear to indicate that the 4H-Ag phase is stabilized at reduced dimensions and thermally induced grain growth is probably responsible for triggering the irreversible transformation to cubic Ag.</description><identifier>ISSN: 0953-8984</identifier><identifier>EISSN: 1361-648X</identifier><identifier>DOI: 10.1088/0953-8984/26/11/115405</identifier><identifier>PMID: 24589655</identifier><identifier>CODEN: JCOMEL</identifier><language>eng</language><publisher>England: IOP Publishing</publisher><subject>Calorimetry ; Calorimetry, Differential Scanning ; Condensed matter ; Density ; density functional theory ; Grain growth ; Microstructure ; Models, Molecular ; Molecular Dynamics Simulation ; Phase transformations ; Phase Transition ; polytypes of silver ; Silver ; Silver - chemistry ; size-driven transition ; stacking fault energy ; structural phase transition ; Thermodynamics ; transformation kinetics ; Transformations ; Transition Temperature ; X-Ray Diffraction</subject><ispartof>Journal of physics. Condensed matter, 2014-03, Vol.26 (11), p.115405-115405</ispartof><rights>2014 IOP Publishing Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c419t-e865138fb1d717257a11b0c17055ab240aab64abfc6150d2ace81caee199b14f3</citedby><cites>FETCH-LOGICAL-c419t-e865138fb1d717257a11b0c17055ab240aab64abfc6150d2ace81caee199b14f3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1088/0953-8984/26/11/115405/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,777,781,27905,27906,53827,53874</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/24589655$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Chakraborty, Indrani</creatorcontrib><creatorcontrib>Shirodkar, Sharmila N</creatorcontrib><creatorcontrib>Gohil, Smita</creatorcontrib><creatorcontrib>Waghmare, Umesh V</creatorcontrib><creatorcontrib>Ayyub, Pushan</creatorcontrib><title>The nature of the structural phase transition from the hexagonal (4H) phase to the cubic (3C) phase of silver</title><title>Journal of physics. Condensed matter</title><addtitle>JPhysCM</addtitle><addtitle>J. Phys.: Condens. Matter</addtitle><description>The phase transition from the hexagonal 4H polytype of silver to the commonly known 3C (fcc) phase was studied in detail using x-ray diffraction, electron microscopy, differential scanning calorimetry and Raman spectroscopy. The phase transition is irreversible and accompanied by extensive microstructural changes and grain growth. Detailed scanning and isothermal calorimetric analysis suggests that it is an autocatalytic transformation. Though the calorimetric data suggest an exothermic first-order phase transition with an onset at 155.6 °C (for a heating rate of 2 K min−1) and a latent heat of 312.9 J g−1, the microstructure and the electrical resistance appear to change gradually from much lower temperatures. The 4H phase shows a Raman active mode at 64.3 cm−1 (at 4 K) that undergoes mode softening as the 4H → 3C transformation temperature is approached. A first-principles density functional theory calculation shows that the stacking fault energy of 4H-Ag increases monotonically with temperature. That 4H-Ag has a higher density of stacking faults than 3C-Ag, implies the metastability of the former at higher temperatures. Energetically, the 4H phase is intermediate between the hexagonal 2H phase and the 3C ground state, as indicated by the spontaneous transformation of the 2H to the 4H phase at −4 °C. Our data appear to indicate that the 4H-Ag phase is stabilized at reduced dimensions and thermally induced grain growth is probably responsible for triggering the irreversible transformation to cubic Ag.</description><subject>Calorimetry</subject><subject>Calorimetry, Differential Scanning</subject><subject>Condensed matter</subject><subject>Density</subject><subject>density functional theory</subject><subject>Grain growth</subject><subject>Microstructure</subject><subject>Models, Molecular</subject><subject>Molecular Dynamics Simulation</subject><subject>Phase transformations</subject><subject>Phase Transition</subject><subject>polytypes of silver</subject><subject>Silver</subject><subject>Silver - chemistry</subject><subject>size-driven transition</subject><subject>stacking fault energy</subject><subject>structural phase transition</subject><subject>Thermodynamics</subject><subject>transformation kinetics</subject><subject>Transformations</subject><subject>Transition Temperature</subject><subject>X-Ray Diffraction</subject><issn>0953-8984</issn><issn>1361-648X</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2014</creationdate><recordtype>article</recordtype><sourceid>EIF</sourceid><recordid>eNqFkUtLxDAUhYMoOo7-BenOcVEnt03SZCmDLxDcjOAupGnqVNqmJq3ovzedFwiCEAi5-c65cA5CF4CvAXM-x4KmMReczBM2BwiHEkwP0ARSBjEj_PUQTfbQCTr1_h1jTHhKjtFJQigXjNIJapYrE7WqH5yJbBn14eV7N-gwUHXUrZQ3Ue9U66u-sm1UOtusoZX5Um-2DcyMPFztQLv-00Ne6WiWLnbzYOyr-tO4M3RUqtqb8-09RS93t8vFQ_z0fP-4uHmKNQHRx4YzCikvcygyyBKaKYAca8gwpSpPCFYqZ0TlpWZAcZEobThoZQwIkQMp0ymabXw7Zz8G43vZVF6bulatsYOXEPwJYULA_yjFhFBBshFlG1Q7670zpexc1Sj3LQHLsRU5Bi7HwGXCJIDctBKEF9sdQ96YYi_b1RCAZANUtpPvdnAhWP-_6-UfIt38omRXlOkP_OWipQ</recordid><startdate>20140319</startdate><enddate>20140319</enddate><creator>Chakraborty, Indrani</creator><creator>Shirodkar, Sharmila N</creator><creator>Gohil, Smita</creator><creator>Waghmare, Umesh V</creator><creator>Ayyub, Pushan</creator><general>IOP Publishing</general><scope>CGR</scope><scope>CUY</scope><scope>CVF</scope><scope>ECM</scope><scope>EIF</scope><scope>NPM</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><scope>7U5</scope><scope>8BQ</scope><scope>8FD</scope><scope>JG9</scope><scope>L7M</scope></search><sort><creationdate>20140319</creationdate><title>The nature of the structural phase transition from the hexagonal (4H) phase to the cubic (3C) phase of silver</title><author>Chakraborty, Indrani ; Shirodkar, Sharmila N ; Gohil, Smita ; Waghmare, Umesh V ; Ayyub, Pushan</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c419t-e865138fb1d717257a11b0c17055ab240aab64abfc6150d2ace81caee199b14f3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2014</creationdate><topic>Calorimetry</topic><topic>Calorimetry, Differential Scanning</topic><topic>Condensed matter</topic><topic>Density</topic><topic>density functional theory</topic><topic>Grain growth</topic><topic>Microstructure</topic><topic>Models, Molecular</topic><topic>Molecular Dynamics Simulation</topic><topic>Phase transformations</topic><topic>Phase Transition</topic><topic>polytypes of silver</topic><topic>Silver</topic><topic>Silver - chemistry</topic><topic>size-driven transition</topic><topic>stacking fault energy</topic><topic>structural phase transition</topic><topic>Thermodynamics</topic><topic>transformation kinetics</topic><topic>Transformations</topic><topic>Transition Temperature</topic><topic>X-Ray Diffraction</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Chakraborty, Indrani</creatorcontrib><creatorcontrib>Shirodkar, Sharmila N</creatorcontrib><creatorcontrib>Gohil, Smita</creatorcontrib><creatorcontrib>Waghmare, Umesh V</creatorcontrib><creatorcontrib>Ayyub, Pushan</creatorcontrib><collection>Medline</collection><collection>MEDLINE</collection><collection>MEDLINE (Ovid)</collection><collection>MEDLINE</collection><collection>MEDLINE</collection><collection>PubMed</collection><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><collection>Solid State and Superconductivity Abstracts</collection><collection>METADEX</collection><collection>Technology Research Database</collection><collection>Materials Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Journal of physics. Condensed matter</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Chakraborty, Indrani</au><au>Shirodkar, Sharmila N</au><au>Gohil, Smita</au><au>Waghmare, Umesh V</au><au>Ayyub, Pushan</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The nature of the structural phase transition from the hexagonal (4H) phase to the cubic (3C) phase of silver</atitle><jtitle>Journal of physics. Condensed matter</jtitle><stitle>JPhysCM</stitle><addtitle>J. Phys.: Condens. Matter</addtitle><date>2014-03-19</date><risdate>2014</risdate><volume>26</volume><issue>11</issue><spage>115405</spage><epage>115405</epage><pages>115405-115405</pages><issn>0953-8984</issn><eissn>1361-648X</eissn><coden>JCOMEL</coden><abstract>The phase transition from the hexagonal 4H polytype of silver to the commonly known 3C (fcc) phase was studied in detail using x-ray diffraction, electron microscopy, differential scanning calorimetry and Raman spectroscopy. The phase transition is irreversible and accompanied by extensive microstructural changes and grain growth. Detailed scanning and isothermal calorimetric analysis suggests that it is an autocatalytic transformation. Though the calorimetric data suggest an exothermic first-order phase transition with an onset at 155.6 °C (for a heating rate of 2 K min−1) and a latent heat of 312.9 J g−1, the microstructure and the electrical resistance appear to change gradually from much lower temperatures. The 4H phase shows a Raman active mode at 64.3 cm−1 (at 4 K) that undergoes mode softening as the 4H → 3C transformation temperature is approached. A first-principles density functional theory calculation shows that the stacking fault energy of 4H-Ag increases monotonically with temperature. That 4H-Ag has a higher density of stacking faults than 3C-Ag, implies the metastability of the former at higher temperatures. Energetically, the 4H phase is intermediate between the hexagonal 2H phase and the 3C ground state, as indicated by the spontaneous transformation of the 2H to the 4H phase at −4 °C. Our data appear to indicate that the 4H-Ag phase is stabilized at reduced dimensions and thermally induced grain growth is probably responsible for triggering the irreversible transformation to cubic Ag.</abstract><cop>England</cop><pub>IOP Publishing</pub><pmid>24589655</pmid><doi>10.1088/0953-8984/26/11/115405</doi><tpages>8</tpages></addata></record> |
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subjects | Calorimetry Calorimetry, Differential Scanning Condensed matter Density density functional theory Grain growth Microstructure Models, Molecular Molecular Dynamics Simulation Phase transformations Phase Transition polytypes of silver Silver Silver - chemistry size-driven transition stacking fault energy structural phase transition Thermodynamics transformation kinetics Transformations Transition Temperature X-Ray Diffraction |
title | The nature of the structural phase transition from the hexagonal (4H) phase to the cubic (3C) phase of silver |
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