Loading…

The Effect of Active-Layer Thickness and Back-Channel Conductivity on the Subthreshold Transfer Characteristics of Hf-In-Zn-O TFTs

The effect of active-layer thickness and back-channel conductivity on the subthreshold transfer characteristics of hafnium-indium-zinc-oxide (HIZO) thin-film transistors was studied. Experiments show that subthreshold humps in the transfer curves become more pronounced as the active-layer thickness...

Full description

Saved in:
Bibliographic Details
Published in:IEEE electron device letters 2011-08, Vol.32 (8), p.1077-1079
Main Authors: Maeng, W. J., Joon Seok Park, Hyun-Suk Kim, Eok Soo Kim, Kyoung Seok Son, Tae Sang Kim, Myungkwan Ryu, Sangyoon Lee
Format: Article
Language:English
Subjects:
Citations: Items that this one cites
Items that cite this one
Online Access:Get full text
Tags: Add Tag
No Tags, Be the first to tag this record!
cited_by cdi_FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3
cites cdi_FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3
container_end_page 1079
container_issue 8
container_start_page 1077
container_title IEEE electron device letters
container_volume 32
creator Maeng, W. J.
Joon Seok Park
Hyun-Suk Kim
Eok Soo Kim
Kyoung Seok Son
Tae Sang Kim
Myungkwan Ryu
Sangyoon Lee
description The effect of active-layer thickness and back-channel conductivity on the subthreshold transfer characteristics of hafnium-indium-zinc-oxide (HIZO) thin-film transistors was studied. Experiments show that subthreshold humps in the transfer curves become more pronounced as the active-layer thickness increases, in the presence of a highly conductive back channel. With a highly conductive thin back channel, subthreshold humps were observed as the total active-layer thickness exceeded 80 nm. The above results can be interpreted as a consequence of a reduction in the effective gate field as the active thickness exceeds the "screening length". The screening length of the HIZO layer is calculated to be approximately 78 nm, and accordingly, as the active thickness exceeds this value, subthreshold humps that are anticipated to originate from the back-channel conduction appear.
doi_str_mv 10.1109/LED.2011.2156756
format article
fullrecord <record><control><sourceid>proquest_pasca</sourceid><recordid>TN_cdi_pascalfrancis_primary_24415937</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><ieee_id>5873119</ieee_id><sourcerecordid>2559703521</sourcerecordid><originalsourceid>FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3</originalsourceid><addsrcrecordid>eNpdkUFrHCEYhqW00G3ae6EXKZSe3OioM84x3W6awEIOnV56EVc_GZOJk6pT2Gt_eV12ySEnQZ_38eN7EfrI6Jox2l_utt_XDWVs3TDZdrJ9hVZMSkWobPlrtKKdYIQz2r5F73K-p5QJ0YkV-jeMgLfegy149vjKlvAXyM4cIOFhDPYhQs7YRIe_GftANqOJESa8maNbjmwoBzxHXKrl57IvY4I8zpPDQzIx-yqpiWRsgRRyCTYfP7nx5DaS35Hc4eF6yO_RG2-mDB_O5wX6db0dNjdkd_fjdnO1I5bLphBFW2r2jHnrJHNKUGmdqHdKCacsgJOee8Otoorz3jS-cVYx530jKHTtnl-gryfvU5r_LJCLfgzZwjSZCPOSdU-7nqteyEp-fkHez0uKdTjd1-22HZV9hegJsmnOOYHXTyk8mnTQjOpjJbpWoo-V6HMlNfLl7DXZmsnXHdmQn3ONEKyKu8p9OnEBAJ6fpeo4Yz3_DyTblAo</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>915667059</pqid></control><display><type>article</type><title>The Effect of Active-Layer Thickness and Back-Channel Conductivity on the Subthreshold Transfer Characteristics of Hf-In-Zn-O TFTs</title><source>IEEE Electronic Library (IEL) Journals</source><creator>Maeng, W. J. ; Joon Seok Park ; Hyun-Suk Kim ; Eok Soo Kim ; Kyoung Seok Son ; Tae Sang Kim ; Myungkwan Ryu ; Sangyoon Lee</creator><creatorcontrib>Maeng, W. J. ; Joon Seok Park ; Hyun-Suk Kim ; Eok Soo Kim ; Kyoung Seok Son ; Tae Sang Kim ; Myungkwan Ryu ; Sangyoon Lee</creatorcontrib><description>The effect of active-layer thickness and back-channel conductivity on the subthreshold transfer characteristics of hafnium-indium-zinc-oxide (HIZO) thin-film transistors was studied. Experiments show that subthreshold humps in the transfer curves become more pronounced as the active-layer thickness increases, in the presence of a highly conductive back channel. With a highly conductive thin back channel, subthreshold humps were observed as the total active-layer thickness exceeded 80 nm. The above results can be interpreted as a consequence of a reduction in the effective gate field as the active thickness exceeds the "screening length". The screening length of the HIZO layer is calculated to be approximately 78 nm, and accordingly, as the active thickness exceeds this value, subthreshold humps that are anticipated to originate from the back-channel conduction appear.</description><identifier>ISSN: 0741-3106</identifier><identifier>EISSN: 1558-0563</identifier><identifier>DOI: 10.1109/LED.2011.2156756</identifier><identifier>CODEN: EDLEDZ</identifier><language>eng</language><publisher>New York, NY: IEEE</publisher><subject>Active-layer thickness ; Applied sciences ; back channel ; Channels ; Conductivity ; Devices ; Electronics ; Exact sciences and technology ; Gates ; Hafnium ; hump ; Logic gates ; Mathematical analysis ; Pixel ; Plasmas ; Screening ; Semiconductor devices ; Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices ; Thin film transistors ; thin-film transistors (TFTs) ; Threshold voltage ; Transistors</subject><ispartof>IEEE electron device letters, 2011-08, Vol.32 (8), p.1077-1079</ispartof><rights>2015 INIST-CNRS</rights><rights>Copyright The Institute of Electrical and Electronics Engineers, Inc. (IEEE) Aug 2011</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3</citedby><cites>FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://ieeexplore.ieee.org/document/5873119$$EHTML$$P50$$Gieee$$H</linktohtml><link.rule.ids>314,780,784,27924,27925,54796</link.rule.ids><backlink>$$Uhttp://pascal-francis.inist.fr/vibad/index.php?action=getRecordDetail&amp;idt=24415937$$DView record in Pascal Francis$$Hfree_for_read</backlink></links><search><creatorcontrib>Maeng, W. J.</creatorcontrib><creatorcontrib>Joon Seok Park</creatorcontrib><creatorcontrib>Hyun-Suk Kim</creatorcontrib><creatorcontrib>Eok Soo Kim</creatorcontrib><creatorcontrib>Kyoung Seok Son</creatorcontrib><creatorcontrib>Tae Sang Kim</creatorcontrib><creatorcontrib>Myungkwan Ryu</creatorcontrib><creatorcontrib>Sangyoon Lee</creatorcontrib><title>The Effect of Active-Layer Thickness and Back-Channel Conductivity on the Subthreshold Transfer Characteristics of Hf-In-Zn-O TFTs</title><title>IEEE electron device letters</title><addtitle>LED</addtitle><description>The effect of active-layer thickness and back-channel conductivity on the subthreshold transfer characteristics of hafnium-indium-zinc-oxide (HIZO) thin-film transistors was studied. Experiments show that subthreshold humps in the transfer curves become more pronounced as the active-layer thickness increases, in the presence of a highly conductive back channel. With a highly conductive thin back channel, subthreshold humps were observed as the total active-layer thickness exceeded 80 nm. The above results can be interpreted as a consequence of a reduction in the effective gate field as the active thickness exceeds the "screening length". The screening length of the HIZO layer is calculated to be approximately 78 nm, and accordingly, as the active thickness exceeds this value, subthreshold humps that are anticipated to originate from the back-channel conduction appear.</description><subject>Active-layer thickness</subject><subject>Applied sciences</subject><subject>back channel</subject><subject>Channels</subject><subject>Conductivity</subject><subject>Devices</subject><subject>Electronics</subject><subject>Exact sciences and technology</subject><subject>Gates</subject><subject>Hafnium</subject><subject>hump</subject><subject>Logic gates</subject><subject>Mathematical analysis</subject><subject>Pixel</subject><subject>Plasmas</subject><subject>Screening</subject><subject>Semiconductor devices</subject><subject>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</subject><subject>Thin film transistors</subject><subject>thin-film transistors (TFTs)</subject><subject>Threshold voltage</subject><subject>Transistors</subject><issn>0741-3106</issn><issn>1558-0563</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNpdkUFrHCEYhqW00G3ae6EXKZSe3OioM84x3W6awEIOnV56EVc_GZOJk6pT2Gt_eV12ySEnQZ_38eN7EfrI6Jox2l_utt_XDWVs3TDZdrJ9hVZMSkWobPlrtKKdYIQz2r5F73K-p5QJ0YkV-jeMgLfegy149vjKlvAXyM4cIOFhDPYhQs7YRIe_GftANqOJESa8maNbjmwoBzxHXKrl57IvY4I8zpPDQzIx-yqpiWRsgRRyCTYfP7nx5DaS35Hc4eF6yO_RG2-mDB_O5wX6db0dNjdkd_fjdnO1I5bLphBFW2r2jHnrJHNKUGmdqHdKCacsgJOee8Otoorz3jS-cVYx530jKHTtnl-gryfvU5r_LJCLfgzZwjSZCPOSdU-7nqteyEp-fkHez0uKdTjd1-22HZV9hegJsmnOOYHXTyk8mnTQjOpjJbpWoo-V6HMlNfLl7DXZmsnXHdmQn3ONEKyKu8p9OnEBAJ6fpeo4Yz3_DyTblAo</recordid><startdate>20110801</startdate><enddate>20110801</enddate><creator>Maeng, W. J.</creator><creator>Joon Seok Park</creator><creator>Hyun-Suk Kim</creator><creator>Eok Soo Kim</creator><creator>Kyoung Seok Son</creator><creator>Tae Sang Kim</creator><creator>Myungkwan Ryu</creator><creator>Sangyoon Lee</creator><general>IEEE</general><general>Institute of Electrical and Electronics Engineers</general><general>The Institute of Electrical and Electronics Engineers, Inc. (IEEE)</general><scope>97E</scope><scope>RIA</scope><scope>RIE</scope><scope>IQODW</scope><scope>AAYXX</scope><scope>CITATION</scope><scope>7SP</scope><scope>8FD</scope><scope>L7M</scope><scope>F28</scope><scope>FR3</scope></search><sort><creationdate>20110801</creationdate><title>The Effect of Active-Layer Thickness and Back-Channel Conductivity on the Subthreshold Transfer Characteristics of Hf-In-Zn-O TFTs</title><author>Maeng, W. J. ; Joon Seok Park ; Hyun-Suk Kim ; Eok Soo Kim ; Kyoung Seok Son ; Tae Sang Kim ; Myungkwan Ryu ; Sangyoon Lee</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><topic>Active-layer thickness</topic><topic>Applied sciences</topic><topic>back channel</topic><topic>Channels</topic><topic>Conductivity</topic><topic>Devices</topic><topic>Electronics</topic><topic>Exact sciences and technology</topic><topic>Gates</topic><topic>Hafnium</topic><topic>hump</topic><topic>Logic gates</topic><topic>Mathematical analysis</topic><topic>Pixel</topic><topic>Plasmas</topic><topic>Screening</topic><topic>Semiconductor devices</topic><topic>Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices</topic><topic>Thin film transistors</topic><topic>thin-film transistors (TFTs)</topic><topic>Threshold voltage</topic><topic>Transistors</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Maeng, W. J.</creatorcontrib><creatorcontrib>Joon Seok Park</creatorcontrib><creatorcontrib>Hyun-Suk Kim</creatorcontrib><creatorcontrib>Eok Soo Kim</creatorcontrib><creatorcontrib>Kyoung Seok Son</creatorcontrib><creatorcontrib>Tae Sang Kim</creatorcontrib><creatorcontrib>Myungkwan Ryu</creatorcontrib><creatorcontrib>Sangyoon Lee</creatorcontrib><collection>IEEE All-Society Periodicals Package (ASPP) 2005-present</collection><collection>IEEE All-Society Periodicals Package (ASPP) 1998-Present</collection><collection>IEEE/IET Electronic Library</collection><collection>Pascal-Francis</collection><collection>CrossRef</collection><collection>Electronics &amp; Communications Abstracts</collection><collection>Technology Research Database</collection><collection>Advanced Technologies Database with Aerospace</collection><collection>ANTE: Abstracts in New Technology &amp; Engineering</collection><collection>Engineering Research Database</collection><jtitle>IEEE electron device letters</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Maeng, W. J.</au><au>Joon Seok Park</au><au>Hyun-Suk Kim</au><au>Eok Soo Kim</au><au>Kyoung Seok Son</au><au>Tae Sang Kim</au><au>Myungkwan Ryu</au><au>Sangyoon Lee</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>The Effect of Active-Layer Thickness and Back-Channel Conductivity on the Subthreshold Transfer Characteristics of Hf-In-Zn-O TFTs</atitle><jtitle>IEEE electron device letters</jtitle><stitle>LED</stitle><date>2011-08-01</date><risdate>2011</risdate><volume>32</volume><issue>8</issue><spage>1077</spage><epage>1079</epage><pages>1077-1079</pages><issn>0741-3106</issn><eissn>1558-0563</eissn><coden>EDLEDZ</coden><abstract>The effect of active-layer thickness and back-channel conductivity on the subthreshold transfer characteristics of hafnium-indium-zinc-oxide (HIZO) thin-film transistors was studied. Experiments show that subthreshold humps in the transfer curves become more pronounced as the active-layer thickness increases, in the presence of a highly conductive back channel. With a highly conductive thin back channel, subthreshold humps were observed as the total active-layer thickness exceeded 80 nm. The above results can be interpreted as a consequence of a reduction in the effective gate field as the active thickness exceeds the "screening length". The screening length of the HIZO layer is calculated to be approximately 78 nm, and accordingly, as the active thickness exceeds this value, subthreshold humps that are anticipated to originate from the back-channel conduction appear.</abstract><cop>New York, NY</cop><pub>IEEE</pub><doi>10.1109/LED.2011.2156756</doi><tpages>3</tpages></addata></record>
fulltext fulltext
identifier ISSN: 0741-3106
ispartof IEEE electron device letters, 2011-08, Vol.32 (8), p.1077-1079
issn 0741-3106
1558-0563
language eng
recordid cdi_pascalfrancis_primary_24415937
source IEEE Electronic Library (IEL) Journals
subjects Active-layer thickness
Applied sciences
back channel
Channels
Conductivity
Devices
Electronics
Exact sciences and technology
Gates
Hafnium
hump
Logic gates
Mathematical analysis
Pixel
Plasmas
Screening
Semiconductor devices
Semiconductor electronics. Microelectronics. Optoelectronics. Solid state devices
Thin film transistors
thin-film transistors (TFTs)
Threshold voltage
Transistors
title The Effect of Active-Layer Thickness and Back-Channel Conductivity on the Subthreshold Transfer Characteristics of Hf-In-Zn-O TFTs
url http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-07T17%3A35%3A40IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_pasca&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=The%20Effect%20of%20Active-Layer%20Thickness%20and%20Back-Channel%20Conductivity%20on%20the%20Subthreshold%20Transfer%20Characteristics%20of%20Hf-In-Zn-O%20TFTs&rft.jtitle=IEEE%20electron%20device%20letters&rft.au=Maeng,%20W.%20J.&rft.date=2011-08-01&rft.volume=32&rft.issue=8&rft.spage=1077&rft.epage=1079&rft.pages=1077-1079&rft.issn=0741-3106&rft.eissn=1558-0563&rft.coden=EDLEDZ&rft_id=info:doi/10.1109/LED.2011.2156756&rft_dat=%3Cproquest_pasca%3E2559703521%3C/proquest_pasca%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-c352t-8060ab11fcd51d8405cd4060884d8ceed5f3fa3c808339a2f2dc81dff240e76b3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=915667059&rft_id=info:pmid/&rft_ieee_id=5873119&rfr_iscdi=true