Loading…
Contact Architecture Controls Conductance in Monolayer Devices
The architecture of electrically contacting the self-assembled monolayer (SAM) of an organophosphonate has a profound effect on a device where the SAM serves as an intermolecular conductive channel in the plane of the substrate. Nanotransfer printing (nTP) enabled the construction of top-contact and...
Saved in:
Published in: | ACS applied materials & interfaces 2020-06, Vol.12 (25), p.28446-28450 |
---|---|
Main Authors: | , , , , , , |
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-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3 |
---|---|
cites | cdi_FETCH-LOGICAL-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3 |
container_end_page | 28450 |
container_issue | 25 |
container_start_page | 28446 |
container_title | ACS applied materials & interfaces |
container_volume | 12 |
creator | Saller, Kai B Liao, Kung-Ching Riedl, Hubert Lugli, Paolo Koblmüller, Gregor Schwartz, Jeffrey Tornow, Marc |
description | The architecture of electrically contacting the self-assembled monolayer (SAM) of an organophosphonate has a profound effect on a device where the SAM serves as an intermolecular conductive channel in the plane of the substrate. Nanotransfer printing (nTP) enabled the construction of top-contact and bottom-contact architectures; contacts were composed of 13 nm thin metal films that were separated by a ca. 20 nm gap. Top-contact devices were fabricated by assembling the SAM across the entire surface of an insulating substrate and then applying the patterned metallic electrodes by nTP; bottom-contact ones were fabricated by nTP of the electrode pattern onto the substrate before the SAM was grown in the patterned nanogaps. SAMs were prepared from (9,10-di(naphthalen-2-yl)anthracen-2-yl)phosphonate; here, the naphthyl groups extend laterally from the anthracenylphosphonate backbone. Significantly, top-contact devices supported current that was about 3 orders of magnitude greater than that for comparable bottom-contact devices and that was at least 100,000 times greater than for a control device devoid of a SAM (at 0.5 V bias). These large differences in conductance between top- and bottom-contact architectures are discussed in consideration of differential contact-to-SAM geometries and, hence, resistances. |
doi_str_mv | 10.1021/acsami.0c08902 |
format | article |
fullrecord | <record><control><sourceid>proquest_cross</sourceid><recordid>TN_cdi_proquest_miscellaneous_2411530565</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>2411530565</sourcerecordid><originalsourceid>FETCH-LOGICAL-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3</originalsourceid><addsrcrecordid>eNp1kM1LAzEUxIMoWKtXz3sUYWu-N70IpX5CxYuew2vyilu2m5pkhf737rLFm6c3DL8ZeEPINaMzRjm7A5dgV8-oo2ZO-QmZsLmUpeGKn_5pKc_JRUpbSrXgVE3I_TK0GVwuFtF91Rld7iIWgxlDkwbhO5ehdVjUbfEW2tDAAWPxgD-1w3RJzjbQJLw63in5fHr8WL6Uq_fn1-ViVYKgVS6NZsjXzEgvBJpKr32lnVCDBKg8eFNx6aXXoAAcGCbXuifnrNJ-gxzElNyMvfsYvjtM2e7q5LBpoMXQJcslY0pQpVWPzkbUxZBSxI3dx3oH8WAZtcNQdhzKHofqA7djoPftNnSx7T_5D_4FzMpq6Q</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype><pqid>2411530565</pqid></control><display><type>article</type><title>Contact Architecture Controls Conductance in Monolayer Devices</title><source>American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list)</source><creator>Saller, Kai B ; Liao, Kung-Ching ; Riedl, Hubert ; Lugli, Paolo ; Koblmüller, Gregor ; Schwartz, Jeffrey ; Tornow, Marc</creator><creatorcontrib>Saller, Kai B ; Liao, Kung-Ching ; Riedl, Hubert ; Lugli, Paolo ; Koblmüller, Gregor ; Schwartz, Jeffrey ; Tornow, Marc</creatorcontrib><description>The architecture of electrically contacting the self-assembled monolayer (SAM) of an organophosphonate has a profound effect on a device where the SAM serves as an intermolecular conductive channel in the plane of the substrate. Nanotransfer printing (nTP) enabled the construction of top-contact and bottom-contact architectures; contacts were composed of 13 nm thin metal films that were separated by a ca. 20 nm gap. Top-contact devices were fabricated by assembling the SAM across the entire surface of an insulating substrate and then applying the patterned metallic electrodes by nTP; bottom-contact ones were fabricated by nTP of the electrode pattern onto the substrate before the SAM was grown in the patterned nanogaps. SAMs were prepared from (9,10-di(naphthalen-2-yl)anthracen-2-yl)phosphonate; here, the naphthyl groups extend laterally from the anthracenylphosphonate backbone. Significantly, top-contact devices supported current that was about 3 orders of magnitude greater than that for comparable bottom-contact devices and that was at least 100,000 times greater than for a control device devoid of a SAM (at 0.5 V bias). These large differences in conductance between top- and bottom-contact architectures are discussed in consideration of differential contact-to-SAM geometries and, hence, resistances.</description><identifier>ISSN: 1944-8244</identifier><identifier>EISSN: 1944-8252</identifier><identifier>DOI: 10.1021/acsami.0c08902</identifier><language>eng</language><publisher>American Chemical Society</publisher><subject>Organic Electronic Devices</subject><ispartof>ACS applied materials & interfaces, 2020-06, Vol.12 (25), p.28446-28450</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3</citedby><cites>FETCH-LOGICAL-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3</cites><orcidid>0000-0001-9873-4499 ; 0000-0002-1860-2769 ; 0000-0002-7228-0158 ; 0000-0002-6659-2390</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,778,782,27907,27908</link.rule.ids></links><search><creatorcontrib>Saller, Kai B</creatorcontrib><creatorcontrib>Liao, Kung-Ching</creatorcontrib><creatorcontrib>Riedl, Hubert</creatorcontrib><creatorcontrib>Lugli, Paolo</creatorcontrib><creatorcontrib>Koblmüller, Gregor</creatorcontrib><creatorcontrib>Schwartz, Jeffrey</creatorcontrib><creatorcontrib>Tornow, Marc</creatorcontrib><title>Contact Architecture Controls Conductance in Monolayer Devices</title><title>ACS applied materials & interfaces</title><addtitle>ACS Appl. Mater. Interfaces</addtitle><description>The architecture of electrically contacting the self-assembled monolayer (SAM) of an organophosphonate has a profound effect on a device where the SAM serves as an intermolecular conductive channel in the plane of the substrate. Nanotransfer printing (nTP) enabled the construction of top-contact and bottom-contact architectures; contacts were composed of 13 nm thin metal films that were separated by a ca. 20 nm gap. Top-contact devices were fabricated by assembling the SAM across the entire surface of an insulating substrate and then applying the patterned metallic electrodes by nTP; bottom-contact ones were fabricated by nTP of the electrode pattern onto the substrate before the SAM was grown in the patterned nanogaps. SAMs were prepared from (9,10-di(naphthalen-2-yl)anthracen-2-yl)phosphonate; here, the naphthyl groups extend laterally from the anthracenylphosphonate backbone. Significantly, top-contact devices supported current that was about 3 orders of magnitude greater than that for comparable bottom-contact devices and that was at least 100,000 times greater than for a control device devoid of a SAM (at 0.5 V bias). These large differences in conductance between top- and bottom-contact architectures are discussed in consideration of differential contact-to-SAM geometries and, hence, resistances.</description><subject>Organic Electronic Devices</subject><issn>1944-8244</issn><issn>1944-8252</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2020</creationdate><recordtype>article</recordtype><recordid>eNp1kM1LAzEUxIMoWKtXz3sUYWu-N70IpX5CxYuew2vyilu2m5pkhf737rLFm6c3DL8ZeEPINaMzRjm7A5dgV8-oo2ZO-QmZsLmUpeGKn_5pKc_JRUpbSrXgVE3I_TK0GVwuFtF91Rld7iIWgxlDkwbhO5ehdVjUbfEW2tDAAWPxgD-1w3RJzjbQJLw63in5fHr8WL6Uq_fn1-ViVYKgVS6NZsjXzEgvBJpKr32lnVCDBKg8eFNx6aXXoAAcGCbXuifnrNJ-gxzElNyMvfsYvjtM2e7q5LBpoMXQJcslY0pQpVWPzkbUxZBSxI3dx3oH8WAZtcNQdhzKHofqA7djoPftNnSx7T_5D_4FzMpq6Q</recordid><startdate>20200624</startdate><enddate>20200624</enddate><creator>Saller, Kai B</creator><creator>Liao, Kung-Ching</creator><creator>Riedl, Hubert</creator><creator>Lugli, Paolo</creator><creator>Koblmüller, Gregor</creator><creator>Schwartz, Jeffrey</creator><creator>Tornow, Marc</creator><general>American Chemical Society</general><scope>AAYXX</scope><scope>CITATION</scope><scope>7X8</scope><orcidid>https://orcid.org/0000-0001-9873-4499</orcidid><orcidid>https://orcid.org/0000-0002-1860-2769</orcidid><orcidid>https://orcid.org/0000-0002-7228-0158</orcidid><orcidid>https://orcid.org/0000-0002-6659-2390</orcidid></search><sort><creationdate>20200624</creationdate><title>Contact Architecture Controls Conductance in Monolayer Devices</title><author>Saller, Kai B ; Liao, Kung-Ching ; Riedl, Hubert ; Lugli, Paolo ; Koblmüller, Gregor ; Schwartz, Jeffrey ; Tornow, Marc</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2020</creationdate><topic>Organic Electronic Devices</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Saller, Kai B</creatorcontrib><creatorcontrib>Liao, Kung-Ching</creatorcontrib><creatorcontrib>Riedl, Hubert</creatorcontrib><creatorcontrib>Lugli, Paolo</creatorcontrib><creatorcontrib>Koblmüller, Gregor</creatorcontrib><creatorcontrib>Schwartz, Jeffrey</creatorcontrib><creatorcontrib>Tornow, Marc</creatorcontrib><collection>CrossRef</collection><collection>MEDLINE - Academic</collection><jtitle>ACS applied materials & interfaces</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Saller, Kai B</au><au>Liao, Kung-Ching</au><au>Riedl, Hubert</au><au>Lugli, Paolo</au><au>Koblmüller, Gregor</au><au>Schwartz, Jeffrey</au><au>Tornow, Marc</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Contact Architecture Controls Conductance in Monolayer Devices</atitle><jtitle>ACS applied materials & interfaces</jtitle><addtitle>ACS Appl. Mater. Interfaces</addtitle><date>2020-06-24</date><risdate>2020</risdate><volume>12</volume><issue>25</issue><spage>28446</spage><epage>28450</epage><pages>28446-28450</pages><issn>1944-8244</issn><eissn>1944-8252</eissn><abstract>The architecture of electrically contacting the self-assembled monolayer (SAM) of an organophosphonate has a profound effect on a device where the SAM serves as an intermolecular conductive channel in the plane of the substrate. Nanotransfer printing (nTP) enabled the construction of top-contact and bottom-contact architectures; contacts were composed of 13 nm thin metal films that were separated by a ca. 20 nm gap. Top-contact devices were fabricated by assembling the SAM across the entire surface of an insulating substrate and then applying the patterned metallic electrodes by nTP; bottom-contact ones were fabricated by nTP of the electrode pattern onto the substrate before the SAM was grown in the patterned nanogaps. SAMs were prepared from (9,10-di(naphthalen-2-yl)anthracen-2-yl)phosphonate; here, the naphthyl groups extend laterally from the anthracenylphosphonate backbone. Significantly, top-contact devices supported current that was about 3 orders of magnitude greater than that for comparable bottom-contact devices and that was at least 100,000 times greater than for a control device devoid of a SAM (at 0.5 V bias). These large differences in conductance between top- and bottom-contact architectures are discussed in consideration of differential contact-to-SAM geometries and, hence, resistances.</abstract><pub>American Chemical Society</pub><doi>10.1021/acsami.0c08902</doi><tpages>5</tpages><orcidid>https://orcid.org/0000-0001-9873-4499</orcidid><orcidid>https://orcid.org/0000-0002-1860-2769</orcidid><orcidid>https://orcid.org/0000-0002-7228-0158</orcidid><orcidid>https://orcid.org/0000-0002-6659-2390</orcidid></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1944-8244 |
ispartof | ACS applied materials & interfaces, 2020-06, Vol.12 (25), p.28446-28450 |
issn | 1944-8244 1944-8252 |
language | eng |
recordid | cdi_proquest_miscellaneous_2411530565 |
source | American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list) |
subjects | Organic Electronic Devices |
title | Contact Architecture Controls Conductance in Monolayer Devices |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2025-01-16T21%3A49%3A10IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-proquest_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Contact%20Architecture%20Controls%20Conductance%20in%20Monolayer%20Devices&rft.jtitle=ACS%20applied%20materials%20&%20interfaces&rft.au=Saller,%20Kai%20B&rft.date=2020-06-24&rft.volume=12&rft.issue=25&rft.spage=28446&rft.epage=28450&rft.pages=28446-28450&rft.issn=1944-8244&rft.eissn=1944-8252&rft_id=info:doi/10.1021/acsami.0c08902&rft_dat=%3Cproquest_cross%3E2411530565%3C/proquest_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a307t-861e2b184d33e876bd76c35e876aa7dad8724d4d6a5aaca814b633e9176dfe2a3%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_pqid=2411530565&rft_id=info:pmid/&rfr_iscdi=true |