An unexplored antipolar phase in HfO2 from first principles and implication for wake-up mechanism
Perturbing tetragonal HfO2 supercells in simulation with dopants or interstitial oxygen in the context of the ferroelectric Pca 2 1 No. 29 (oIII-phase) formation frequently leads to an unexplored, lower energetic orthorhombic crystal phase with space group Pnma No. 62 (oV-phase). The crystal structu...
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creator | Azevedo Antunes, Luis Ganser, Richard Alcala, Ruben Mikolajick, Thomas Schroeder, Uwe Kersch, Alfred |
description | Perturbing tetragonal HfO2 supercells in simulation with dopants or interstitial oxygen in the context of the ferroelectric
Pca
2
1 No. 29 (oIII-phase) formation frequently leads to an unexplored, lower energetic orthorhombic crystal phase with space group Pnma No. 62 (oV-phase). The crystal structure is inequivalent to cottunite oII-phase with the same space group but is closely related to the second ferroelectric
Pmn
2
1 No. 31 (oIV-phase) space group, as antipolar alignment. To explore the possibility of oIV- or oV-phase formation, we calculate the free energy in harmonic approximation and the energy landscape. Starting from the tetragonal
P
4
2/nmc No. 137 phase (t-phase), according to energy and activation barrier, the formation of the oV-phase is more favorable than that of the oIV-phase. Furthermore, exploring the energy landscape of the oIV–oV system, we find possible antiferroelectric-like behavior in HfO2 and Hf0.5Zr0.5O2, but not in ZrO2. We propose the formation of an oV-phase fraction as a possible structural explanation for a contribution to the wake-up phenomenon in HfO2. X-ray diffraction results on 10 nm Hf1−xZrxO2 thin films with varying Zr content are consistent with the claim. |
doi_str_mv | 10.1063/5.0063808 |
format | Article |
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Pca
2
1 No. 29 (oIII-phase) formation frequently leads to an unexplored, lower energetic orthorhombic crystal phase with space group Pnma No. 62 (oV-phase). The crystal structure is inequivalent to cottunite oII-phase with the same space group but is closely related to the second ferroelectric
Pmn
2
1 No. 31 (oIV-phase) space group, as antipolar alignment. To explore the possibility of oIV- or oV-phase formation, we calculate the free energy in harmonic approximation and the energy landscape. Starting from the tetragonal
P
4
2/nmc No. 137 phase (t-phase), according to energy and activation barrier, the formation of the oV-phase is more favorable than that of the oIV-phase. Furthermore, exploring the energy landscape of the oIV–oV system, we find possible antiferroelectric-like behavior in HfO2 and Hf0.5Zr0.5O2, but not in ZrO2. We propose the formation of an oV-phase fraction as a possible structural explanation for a contribution to the wake-up phenomenon in HfO2. X-ray diffraction results on 10 nm Hf1−xZrxO2 thin films with varying Zr content are consistent with the claim.</description><identifier>ISSN: 0003-6951</identifier><identifier>EISSN: 1077-3118</identifier><identifier>DOI: 10.1063/5.0063808</identifier><identifier>CODEN: APPLAB</identifier><language>eng</language><publisher>Melville: American Institute of Physics</publisher><subject>Antiferroelectricity ; Applied physics ; Crystal structure ; Ferroelectric materials ; First principles ; Free energy ; Hafnium oxide ; Thin films ; Zirconium dioxide</subject><ispartof>Applied physics letters, 2021-08, Vol.119 (8)</ispartof><rights>Author(s)</rights><rights>2021 Author(s). Published under an exclusive license by AIP Publishing.</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c257t-cf2354de66f36341dfbcf50a16e78881045b20d15b81dbe2454cde91b07511293</citedby><cites>FETCH-LOGICAL-c257t-cf2354de66f36341dfbcf50a16e78881045b20d15b81dbe2454cde91b07511293</cites><orcidid>0000-0003-4407-555X ; 0000-0002-7163-8859 ; 0000-0003-2799-9793 ; 0000-0002-6824-2386 ; 0000-0002-0052-3528 ; 0000-0003-3814-0378</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://pubs.aip.org/apl/article-lookup/doi/10.1063/5.0063808$$EHTML$$P50$$Gscitation$$H</linktohtml><link.rule.ids>314,776,780,790,4498,27901,27902,76126</link.rule.ids></links><search><creatorcontrib>Azevedo Antunes, Luis</creatorcontrib><creatorcontrib>Ganser, Richard</creatorcontrib><creatorcontrib>Alcala, Ruben</creatorcontrib><creatorcontrib>Mikolajick, Thomas</creatorcontrib><creatorcontrib>Schroeder, Uwe</creatorcontrib><creatorcontrib>Kersch, Alfred</creatorcontrib><title>An unexplored antipolar phase in HfO2 from first principles and implication for wake-up mechanism</title><title>Applied physics letters</title><description>Perturbing tetragonal HfO2 supercells in simulation with dopants or interstitial oxygen in the context of the ferroelectric
Pca
2
1 No. 29 (oIII-phase) formation frequently leads to an unexplored, lower energetic orthorhombic crystal phase with space group Pnma No. 62 (oV-phase). The crystal structure is inequivalent to cottunite oII-phase with the same space group but is closely related to the second ferroelectric
Pmn
2
1 No. 31 (oIV-phase) space group, as antipolar alignment. To explore the possibility of oIV- or oV-phase formation, we calculate the free energy in harmonic approximation and the energy landscape. Starting from the tetragonal
P
4
2/nmc No. 137 phase (t-phase), according to energy and activation barrier, the formation of the oV-phase is more favorable than that of the oIV-phase. Furthermore, exploring the energy landscape of the oIV–oV system, we find possible antiferroelectric-like behavior in HfO2 and Hf0.5Zr0.5O2, but not in ZrO2. We propose the formation of an oV-phase fraction as a possible structural explanation for a contribution to the wake-up phenomenon in HfO2. X-ray diffraction results on 10 nm Hf1−xZrxO2 thin films with varying Zr content are consistent with the claim.</description><subject>Antiferroelectricity</subject><subject>Applied physics</subject><subject>Crystal structure</subject><subject>Ferroelectric materials</subject><subject>First principles</subject><subject>Free energy</subject><subject>Hafnium oxide</subject><subject>Thin films</subject><subject>Zirconium dioxide</subject><issn>0003-6951</issn><issn>1077-3118</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2021</creationdate><recordtype>article</recordtype><recordid>eNqd0MtKAzEUBuAgCtbqwjcIuFKYmsskM12WolYodKPrkMmFps4kMZnx8vZObcG9q58DH-dwfgCuMZphxOk9m6ExalSfgAlGVVVQjOtTMEEI0YLPGT4HFznvxpERSidALjwcvPmKbUhGQ-l7F0MrE4xbmQ10Hq7shkCbQgetS7mHMTmvXGxNHrWGroutU7J3wUMbEvyUb6YYIuyM2krvcncJzqxss7k65hS8Pj68LFfFevP0vFysC0VY1RfKEspKbTi3lNMSa9soy5DE3FR1XWNUsoYgjVlTY90YUrJSaTPHDaoYxmROp-DmsDem8D6Y3ItdGJIfTwrCeEn3vfBR3R6USiHnZKwY_-lk-hYYiX2Dgoljg6O9O9isXP_74f_wR0h_UERt6Q9cGX6N</recordid><startdate>20210823</startdate><enddate>20210823</enddate><creator>Azevedo Antunes, Luis</creator><creator>Ganser, Richard</creator><creator>Alcala, Ruben</creator><creator>Mikolajick, Thomas</creator><creator>Schroeder, Uwe</creator><creator>Kersch, Alfred</creator><general>American Institute of Physics</general><scope>AAYXX</scope><scope>CITATION</scope><scope>8FD</scope><scope>H8D</scope><scope>L7M</scope><orcidid>https://orcid.org/0000-0003-4407-555X</orcidid><orcidid>https://orcid.org/0000-0002-7163-8859</orcidid><orcidid>https://orcid.org/0000-0003-2799-9793</orcidid><orcidid>https://orcid.org/0000-0002-6824-2386</orcidid><orcidid>https://orcid.org/0000-0002-0052-3528</orcidid><orcidid>https://orcid.org/0000-0003-3814-0378</orcidid></search><sort><creationdate>20210823</creationdate><title>An unexplored antipolar phase in HfO2 from first principles and implication for wake-up mechanism</title><author>Azevedo Antunes, Luis ; Ganser, Richard ; Alcala, Ruben ; Mikolajick, Thomas ; Schroeder, Uwe ; Kersch, Alfred</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c257t-cf2354de66f36341dfbcf50a16e78881045b20d15b81dbe2454cde91b07511293</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2021</creationdate><topic>Antiferroelectricity</topic><topic>Applied physics</topic><topic>Crystal structure</topic><topic>Ferroelectric materials</topic><topic>First principles</topic><topic>Free energy</topic><topic>Hafnium oxide</topic><topic>Thin films</topic><topic>Zirconium dioxide</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Azevedo Antunes, Luis</creatorcontrib><creatorcontrib>Ganser, Richard</creatorcontrib><creatorcontrib>Alcala, Ruben</creatorcontrib><creatorcontrib>Mikolajick, Thomas</creatorcontrib><creatorcontrib>Schroeder, Uwe</creatorcontrib><creatorcontrib>Kersch, Alfred</creatorcontrib><collection>CrossRef</collection><collection>Technology Research Database</collection><collection>Aerospace Database</collection><collection>Advanced Technologies Database with Aerospace</collection><jtitle>Applied physics letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Azevedo Antunes, Luis</au><au>Ganser, Richard</au><au>Alcala, Ruben</au><au>Mikolajick, Thomas</au><au>Schroeder, Uwe</au><au>Kersch, Alfred</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>An unexplored antipolar phase in HfO2 from first principles and implication for wake-up mechanism</atitle><jtitle>Applied physics letters</jtitle><date>2021-08-23</date><risdate>2021</risdate><volume>119</volume><issue>8</issue><issn>0003-6951</issn><eissn>1077-3118</eissn><coden>APPLAB</coden><abstract>Perturbing tetragonal HfO2 supercells in simulation with dopants or interstitial oxygen in the context of the ferroelectric
Pca
2
1 No. 29 (oIII-phase) formation frequently leads to an unexplored, lower energetic orthorhombic crystal phase with space group Pnma No. 62 (oV-phase). The crystal structure is inequivalent to cottunite oII-phase with the same space group but is closely related to the second ferroelectric
Pmn
2
1 No. 31 (oIV-phase) space group, as antipolar alignment. To explore the possibility of oIV- or oV-phase formation, we calculate the free energy in harmonic approximation and the energy landscape. Starting from the tetragonal
P
4
2/nmc No. 137 phase (t-phase), according to energy and activation barrier, the formation of the oV-phase is more favorable than that of the oIV-phase. Furthermore, exploring the energy landscape of the oIV–oV system, we find possible antiferroelectric-like behavior in HfO2 and Hf0.5Zr0.5O2, but not in ZrO2. We propose the formation of an oV-phase fraction as a possible structural explanation for a contribution to the wake-up phenomenon in HfO2. X-ray diffraction results on 10 nm Hf1−xZrxO2 thin films with varying Zr content are consistent with the claim.</abstract><cop>Melville</cop><pub>American Institute of Physics</pub><doi>10.1063/5.0063808</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0003-4407-555X</orcidid><orcidid>https://orcid.org/0000-0002-7163-8859</orcidid><orcidid>https://orcid.org/0000-0003-2799-9793</orcidid><orcidid>https://orcid.org/0000-0002-6824-2386</orcidid><orcidid>https://orcid.org/0000-0002-0052-3528</orcidid><orcidid>https://orcid.org/0000-0003-3814-0378</orcidid></addata></record> |
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source | AIP Journals Complete; Alma/SFX Local Collection |
subjects | Antiferroelectricity Applied physics Crystal structure Ferroelectric materials First principles Free energy Hafnium oxide Thin films Zirconium dioxide |
title | An unexplored antipolar phase in HfO2 from first principles and implication for wake-up mechanism |
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