Optimization of MIS type Non-Volatile Memory Device with Al-Doped HfO2 as Charge Trapping Layer
The reduction in physical size of the Non-volatile memory (NVM) demands the use of high-k dielectrics due to loss in charge trapping behavior. The large bandgap of Al2O3 (∼7.0 eV) proves it suitable for blocking and tunneling layer, while the high dielectric constant of HfO2 proves it suitable for c...
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creator | Yoon, Geonju Kim, Taeyong Agrawal, Khushabu Kim, Jaemin Park, Jinsu Kim, Hyun-Hoo Cho, Eun-Chel Yi, Junsin |
description | The reduction in physical size of the Non-volatile memory (NVM) demands the use of high-k dielectrics due to loss in charge trapping behavior. The large bandgap of Al2O3 (∼7.0 eV) proves it suitable for blocking and tunneling layer, while the high dielectric constant of HfO2 proves it suitable for charge trapping layer (CTL). In this paper, we propose the application of Al doped HfO2 used as CTL. The doping concentration has been varied by varying the number of sub-cycles (sequential cycles of HfO2, Al2O3) by ALD system. The optical energy bandgap of Al doped HfO2 observed to be increases from 4.91−5.20 eV as the Al incorporation content increases with 1:9−1:4 ALD sub-cycles. Oxygen vacancy defect in the thin film decreased to 17.87% for 1:4-Al doped HfO2 sample as verified from the XPS. The increase in Al incorporation leads to charge loss towards silicon substrate due to high bandgap energy. In addition, charge traps are not well performed due to reduction of internal defects in the film. After 10 years, the NVM device with Al doped HfO2 (1:9) CTL has improved charge retention characteristics by 14% as compared to a normal HfO2 charge trap layer NVM device. |
doi_str_mv | 10.1149/2162-8777/abaf10 |
format | Article |
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The large bandgap of Al2O3 (∼7.0 eV) proves it suitable for blocking and tunneling layer, while the high dielectric constant of HfO2 proves it suitable for charge trapping layer (CTL). In this paper, we propose the application of Al doped HfO2 used as CTL. The doping concentration has been varied by varying the number of sub-cycles (sequential cycles of HfO2, Al2O3) by ALD system. The optical energy bandgap of Al doped HfO2 observed to be increases from 4.91−5.20 eV as the Al incorporation content increases with 1:9−1:4 ALD sub-cycles. Oxygen vacancy defect in the thin film decreased to 17.87% for 1:4-Al doped HfO2 sample as verified from the XPS. The increase in Al incorporation leads to charge loss towards silicon substrate due to high bandgap energy. In addition, charge traps are not well performed due to reduction of internal defects in the film. After 10 years, the NVM device with Al doped HfO2 (1:9) CTL has improved charge retention characteristics by 14% as compared to a normal HfO2 charge trap layer NVM device.</description><identifier>ISSN: 2162-8769</identifier><identifier>EISSN: 2162-8777</identifier><identifier>DOI: 10.1149/2162-8777/abaf10</identifier><identifier>CODEN: EJSSBG</identifier><language>eng</language><publisher>IOP Publishing</publisher><subject>Al-doped HfO2 ; Atomic layer deposition ; Dielectrics - High-k ; Non-volatile memory</subject><ispartof>ECS journal of solid state science and technology, 2020-08, Vol.9 (7)</ispartof><rights>2020 The Electrochemical Society ("ECS"). Published on behalf of ECS by IOP Publishing Limited</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0002-6579-6682 ; 0000-0001-8464-2104</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://iopscience.iop.org/article/10.1149/2162-8777/abaf10/pdf$$EPDF$$P50$$Giop$$H</linktopdf><link.rule.ids>314,780,784,27924,27925,53846,53893</link.rule.ids></links><search><creatorcontrib>Yoon, Geonju</creatorcontrib><creatorcontrib>Kim, Taeyong</creatorcontrib><creatorcontrib>Agrawal, Khushabu</creatorcontrib><creatorcontrib>Kim, Jaemin</creatorcontrib><creatorcontrib>Park, Jinsu</creatorcontrib><creatorcontrib>Kim, Hyun-Hoo</creatorcontrib><creatorcontrib>Cho, Eun-Chel</creatorcontrib><creatorcontrib>Yi, Junsin</creatorcontrib><title>Optimization of MIS type Non-Volatile Memory Device with Al-Doped HfO2 as Charge Trapping Layer</title><title>ECS journal of solid state science and technology</title><addtitle>JSS</addtitle><addtitle>ECS J. Solid State Sci. Technol</addtitle><description>The reduction in physical size of the Non-volatile memory (NVM) demands the use of high-k dielectrics due to loss in charge trapping behavior. The large bandgap of Al2O3 (∼7.0 eV) proves it suitable for blocking and tunneling layer, while the high dielectric constant of HfO2 proves it suitable for charge trapping layer (CTL). In this paper, we propose the application of Al doped HfO2 used as CTL. The doping concentration has been varied by varying the number of sub-cycles (sequential cycles of HfO2, Al2O3) by ALD system. The optical energy bandgap of Al doped HfO2 observed to be increases from 4.91−5.20 eV as the Al incorporation content increases with 1:9−1:4 ALD sub-cycles. Oxygen vacancy defect in the thin film decreased to 17.87% for 1:4-Al doped HfO2 sample as verified from the XPS. The increase in Al incorporation leads to charge loss towards silicon substrate due to high bandgap energy. In addition, charge traps are not well performed due to reduction of internal defects in the film. After 10 years, the NVM device with Al doped HfO2 (1:9) CTL has improved charge retention characteristics by 14% as compared to a normal HfO2 charge trap layer NVM device.</description><subject>Al-doped HfO2</subject><subject>Atomic layer deposition</subject><subject>Dielectrics - High-k</subject><subject>Non-volatile memory</subject><issn>2162-8769</issn><issn>2162-8777</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><sourceid/><recordid>eNqVT7FuwjAUtCoqFQF7xzd1asBO0piMFRSBVMpQ1PXJLc_gKMSWnbZKv55ErZi6cMud7m64Y-xW8LEQaT6JRRZHUynlRL0rLfgV65-t3lln-Q0bhVDwFtk0lUncZ7hxtTmaH1UbW4HVsF69Qt04ghdbRW-2bIOSYE1H6xuY05f5IPg29QEey2huHe1gqTcxqACzg_J7gq1XzplqD8-qIT9k11qVgUZ_PGD3i6ftbBkZ67Cwn75qXRQcux_YDcVuNP7-SC6u3_1TL0LAHCVy-cB5im6nkxN8KFty</recordid><startdate>20200824</startdate><enddate>20200824</enddate><creator>Yoon, Geonju</creator><creator>Kim, Taeyong</creator><creator>Agrawal, Khushabu</creator><creator>Kim, Jaemin</creator><creator>Park, Jinsu</creator><creator>Kim, Hyun-Hoo</creator><creator>Cho, Eun-Chel</creator><creator>Yi, Junsin</creator><general>IOP Publishing</general><scope/><orcidid>https://orcid.org/0000-0002-6579-6682</orcidid><orcidid>https://orcid.org/0000-0001-8464-2104</orcidid></search><sort><creationdate>20200824</creationdate><title>Optimization of MIS type Non-Volatile Memory Device with Al-Doped HfO2 as Charge Trapping Layer</title><author>Yoon, Geonju ; Kim, Taeyong ; Agrawal, Khushabu ; Kim, Jaemin ; Park, Jinsu ; Kim, Hyun-Hoo ; Cho, Eun-Chel ; Yi, Junsin</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-iop_journals_10_1149_2162_8777_abaf103</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Al-doped HfO2</topic><topic>Atomic layer deposition</topic><topic>Dielectrics - High-k</topic><topic>Non-volatile memory</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Yoon, Geonju</creatorcontrib><creatorcontrib>Kim, Taeyong</creatorcontrib><creatorcontrib>Agrawal, Khushabu</creatorcontrib><creatorcontrib>Kim, Jaemin</creatorcontrib><creatorcontrib>Park, Jinsu</creatorcontrib><creatorcontrib>Kim, Hyun-Hoo</creatorcontrib><creatorcontrib>Cho, Eun-Chel</creatorcontrib><creatorcontrib>Yi, Junsin</creatorcontrib><jtitle>ECS journal of solid state science and technology</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Yoon, Geonju</au><au>Kim, Taeyong</au><au>Agrawal, Khushabu</au><au>Kim, Jaemin</au><au>Park, Jinsu</au><au>Kim, Hyun-Hoo</au><au>Cho, Eun-Chel</au><au>Yi, Junsin</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Optimization of MIS type Non-Volatile Memory Device with Al-Doped HfO2 as Charge Trapping Layer</atitle><jtitle>ECS journal of solid state science and technology</jtitle><stitle>JSS</stitle><addtitle>ECS J. Solid State Sci. Technol</addtitle><date>2020-08-24</date><risdate>2020</risdate><volume>9</volume><issue>7</issue><issn>2162-8769</issn><eissn>2162-8777</eissn><coden>EJSSBG</coden><abstract>The reduction in physical size of the Non-volatile memory (NVM) demands the use of high-k dielectrics due to loss in charge trapping behavior. The large bandgap of Al2O3 (∼7.0 eV) proves it suitable for blocking and tunneling layer, while the high dielectric constant of HfO2 proves it suitable for charge trapping layer (CTL). In this paper, we propose the application of Al doped HfO2 used as CTL. The doping concentration has been varied by varying the number of sub-cycles (sequential cycles of HfO2, Al2O3) by ALD system. The optical energy bandgap of Al doped HfO2 observed to be increases from 4.91−5.20 eV as the Al incorporation content increases with 1:9−1:4 ALD sub-cycles. Oxygen vacancy defect in the thin film decreased to 17.87% for 1:4-Al doped HfO2 sample as verified from the XPS. The increase in Al incorporation leads to charge loss towards silicon substrate due to high bandgap energy. In addition, charge traps are not well performed due to reduction of internal defects in the film. After 10 years, the NVM device with Al doped HfO2 (1:9) CTL has improved charge retention characteristics by 14% as compared to a normal HfO2 charge trap layer NVM device.</abstract><pub>IOP Publishing</pub><doi>10.1149/2162-8777/abaf10</doi><tpages>6</tpages><orcidid>https://orcid.org/0000-0002-6579-6682</orcidid><orcidid>https://orcid.org/0000-0001-8464-2104</orcidid></addata></record> |
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subjects | Al-doped HfO2 Atomic layer deposition Dielectrics - High-k Non-volatile memory |
title | Optimization of MIS type Non-Volatile Memory Device with Al-Doped HfO2 as Charge Trapping Layer |
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