Loading…
Strain-Induced Tunable Band Gap and Morphology-Dependent Photocurrent in RGO–CdS Nanostructures
In situ CdS nanostructures (nanorods, nanoparticles, nanoclusters) are grown on a reduced graphene oxide (RGO) surface to tune the photocurrent generated due to transfer of excited charge from CdS to RGO. The highest change in photocurrent is achieved in the case of nanoclusters, while nanorods show...
Saved in:
Published in: | Journal of physical chemistry. C 2015-12, Vol.119 (49), p.27749-27758 |
---|---|
Main Authors: | , , , |
Format: | Article |
Language: | English |
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-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03 |
---|---|
cites | cdi_FETCH-LOGICAL-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03 |
container_end_page | 27758 |
container_issue | 49 |
container_start_page | 27749 |
container_title | Journal of physical chemistry. C |
container_volume | 119 |
creator | Mondal, Supriya Sudhu, Suparna Bhattacharya, Shatabda Saha, Shyamal K |
description | In situ CdS nanostructures (nanorods, nanoparticles, nanoclusters) are grown on a reduced graphene oxide (RGO) surface to tune the photocurrent generated due to transfer of excited charge from CdS to RGO. The highest change in photocurrent is achieved in the case of nanoclusters, while nanorods show the lowest. Rietveld analysis has been done to find the microstrain present in three nanocomposites. UV–vis spectroscopy reveals the modulation in band gap due to different growth morphology. From the band structure, it is seen that in nanorod structure strain-induced localized states lower the conduction band which essentially decreases the charge transfer from CdS to RGO, resulting in a smaller change in the photocurrent, while in the case of a nanocluster the photocurrent is maximum due to the lowest strain. This is also consistent with the photoluminescence (PL) quenching as obtained from PL spectra. |
doi_str_mv | 10.1021/acs.jpcc.5b08116 |
format | article |
fullrecord | <record><control><sourceid>acs_cross</sourceid><recordid>TN_cdi_crossref_primary_10_1021_acs_jpcc_5b08116</recordid><sourceformat>XML</sourceformat><sourcesystem>PC</sourcesystem><sourcerecordid>i82244801</sourcerecordid><originalsourceid>FETCH-LOGICAL-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03</originalsourceid><addsrcrecordid>eNp1kE1OwzAQRi0EEqWwZ-kDkGLH-XGWUGipVCii3UcTe0xbFTuyk0V33IEbchISWrFj9c1o5o1Gj5BrzkacxfwWVBhta6VGacUk59kJGfBCxFGepOnpX53k5-QihC1jqWBcDAgsGw8bG82sbhVqumotVDuk92A1nUJN-3x2vl67nXvfRw9Yo9VoG_q6do1Trfd9s7H0bbr4_vwa6yV9AetC41vVtB7DJTkzsAt4dcwhWU0eV-OnaL6YzsZ38whEkjWRkhUzBY-FSdLMZJJJ1GhiJRQDzUEKIwpTxDwX3Mi4kAIThSigA1LQTAwJO5xV3oXg0ZS133yA35eclb2hsjNU9obKo6EOuTkgvxPXetv99__6D-8ibEs</addsrcrecordid><sourcetype>Aggregation Database</sourcetype><iscdi>true</iscdi><recordtype>article</recordtype></control><display><type>article</type><title>Strain-Induced Tunable Band Gap and Morphology-Dependent Photocurrent in RGO–CdS Nanostructures</title><source>American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list)</source><creator>Mondal, Supriya ; Sudhu, Suparna ; Bhattacharya, Shatabda ; Saha, Shyamal K</creator><creatorcontrib>Mondal, Supriya ; Sudhu, Suparna ; Bhattacharya, Shatabda ; Saha, Shyamal K</creatorcontrib><description>In situ CdS nanostructures (nanorods, nanoparticles, nanoclusters) are grown on a reduced graphene oxide (RGO) surface to tune the photocurrent generated due to transfer of excited charge from CdS to RGO. The highest change in photocurrent is achieved in the case of nanoclusters, while nanorods show the lowest. Rietveld analysis has been done to find the microstrain present in three nanocomposites. UV–vis spectroscopy reveals the modulation in band gap due to different growth morphology. From the band structure, it is seen that in nanorod structure strain-induced localized states lower the conduction band which essentially decreases the charge transfer from CdS to RGO, resulting in a smaller change in the photocurrent, while in the case of a nanocluster the photocurrent is maximum due to the lowest strain. This is also consistent with the photoluminescence (PL) quenching as obtained from PL spectra.</description><identifier>ISSN: 1932-7447</identifier><identifier>EISSN: 1932-7455</identifier><identifier>DOI: 10.1021/acs.jpcc.5b08116</identifier><language>eng</language><publisher>American Chemical Society</publisher><ispartof>Journal of physical chemistry. C, 2015-12, Vol.119 (49), p.27749-27758</ispartof><rights>Copyright © 2015 American Chemical Society</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03</citedby><cites>FETCH-LOGICAL-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,780,784,27924,27925</link.rule.ids></links><search><creatorcontrib>Mondal, Supriya</creatorcontrib><creatorcontrib>Sudhu, Suparna</creatorcontrib><creatorcontrib>Bhattacharya, Shatabda</creatorcontrib><creatorcontrib>Saha, Shyamal K</creatorcontrib><title>Strain-Induced Tunable Band Gap and Morphology-Dependent Photocurrent in RGO–CdS Nanostructures</title><title>Journal of physical chemistry. C</title><addtitle>J. Phys. Chem. C</addtitle><description>In situ CdS nanostructures (nanorods, nanoparticles, nanoclusters) are grown on a reduced graphene oxide (RGO) surface to tune the photocurrent generated due to transfer of excited charge from CdS to RGO. The highest change in photocurrent is achieved in the case of nanoclusters, while nanorods show the lowest. Rietveld analysis has been done to find the microstrain present in three nanocomposites. UV–vis spectroscopy reveals the modulation in band gap due to different growth morphology. From the band structure, it is seen that in nanorod structure strain-induced localized states lower the conduction band which essentially decreases the charge transfer from CdS to RGO, resulting in a smaller change in the photocurrent, while in the case of a nanocluster the photocurrent is maximum due to the lowest strain. This is also consistent with the photoluminescence (PL) quenching as obtained from PL spectra.</description><issn>1932-7447</issn><issn>1932-7455</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2015</creationdate><recordtype>article</recordtype><recordid>eNp1kE1OwzAQRi0EEqWwZ-kDkGLH-XGWUGipVCii3UcTe0xbFTuyk0V33IEbchISWrFj9c1o5o1Gj5BrzkacxfwWVBhta6VGacUk59kJGfBCxFGepOnpX53k5-QihC1jqWBcDAgsGw8bG82sbhVqumotVDuk92A1nUJN-3x2vl67nXvfRw9Yo9VoG_q6do1Trfd9s7H0bbr4_vwa6yV9AetC41vVtB7DJTkzsAt4dcwhWU0eV-OnaL6YzsZ38whEkjWRkhUzBY-FSdLMZJJJ1GhiJRQDzUEKIwpTxDwX3Mi4kAIThSigA1LQTAwJO5xV3oXg0ZS133yA35eclb2hsjNU9obKo6EOuTkgvxPXetv99__6D-8ibEs</recordid><startdate>20151210</startdate><enddate>20151210</enddate><creator>Mondal, Supriya</creator><creator>Sudhu, Suparna</creator><creator>Bhattacharya, Shatabda</creator><creator>Saha, Shyamal K</creator><general>American Chemical Society</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20151210</creationdate><title>Strain-Induced Tunable Band Gap and Morphology-Dependent Photocurrent in RGO–CdS Nanostructures</title><author>Mondal, Supriya ; Sudhu, Suparna ; Bhattacharya, Shatabda ; Saha, Shyamal K</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2015</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Mondal, Supriya</creatorcontrib><creatorcontrib>Sudhu, Suparna</creatorcontrib><creatorcontrib>Bhattacharya, Shatabda</creatorcontrib><creatorcontrib>Saha, Shyamal K</creatorcontrib><collection>CrossRef</collection><jtitle>Journal of physical chemistry. C</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Mondal, Supriya</au><au>Sudhu, Suparna</au><au>Bhattacharya, Shatabda</au><au>Saha, Shyamal K</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Strain-Induced Tunable Band Gap and Morphology-Dependent Photocurrent in RGO–CdS Nanostructures</atitle><jtitle>Journal of physical chemistry. C</jtitle><addtitle>J. Phys. Chem. C</addtitle><date>2015-12-10</date><risdate>2015</risdate><volume>119</volume><issue>49</issue><spage>27749</spage><epage>27758</epage><pages>27749-27758</pages><issn>1932-7447</issn><eissn>1932-7455</eissn><abstract>In situ CdS nanostructures (nanorods, nanoparticles, nanoclusters) are grown on a reduced graphene oxide (RGO) surface to tune the photocurrent generated due to transfer of excited charge from CdS to RGO. The highest change in photocurrent is achieved in the case of nanoclusters, while nanorods show the lowest. Rietveld analysis has been done to find the microstrain present in three nanocomposites. UV–vis spectroscopy reveals the modulation in band gap due to different growth morphology. From the band structure, it is seen that in nanorod structure strain-induced localized states lower the conduction band which essentially decreases the charge transfer from CdS to RGO, resulting in a smaller change in the photocurrent, while in the case of a nanocluster the photocurrent is maximum due to the lowest strain. This is also consistent with the photoluminescence (PL) quenching as obtained from PL spectra.</abstract><pub>American Chemical Society</pub><doi>10.1021/acs.jpcc.5b08116</doi><tpages>10</tpages></addata></record> |
fulltext | fulltext |
identifier | ISSN: 1932-7447 |
ispartof | Journal of physical chemistry. C, 2015-12, Vol.119 (49), p.27749-27758 |
issn | 1932-7447 1932-7455 |
language | eng |
recordid | cdi_crossref_primary_10_1021_acs_jpcc_5b08116 |
source | American Chemical Society:Jisc Collections:American Chemical Society Read & Publish Agreement 2022-2024 (Reading list) |
title | Strain-Induced Tunable Band Gap and Morphology-Dependent Photocurrent in RGO–CdS Nanostructures |
url | http://sfxeu10.hosted.exlibrisgroup.com/loughborough?ctx_ver=Z39.88-2004&ctx_enc=info:ofi/enc:UTF-8&ctx_tim=2024-12-26T07%3A24%3A38IST&url_ver=Z39.88-2004&url_ctx_fmt=infofi/fmt:kev:mtx:ctx&rfr_id=info:sid/primo.exlibrisgroup.com:primo3-Article-acs_cross&rft_val_fmt=info:ofi/fmt:kev:mtx:journal&rft.genre=article&rft.atitle=Strain-Induced%20Tunable%20Band%20Gap%20and%20Morphology-Dependent%20Photocurrent%20in%20RGO%E2%80%93CdS%20Nanostructures&rft.jtitle=Journal%20of%20physical%20chemistry.%20C&rft.au=Mondal,%20Supriya&rft.date=2015-12-10&rft.volume=119&rft.issue=49&rft.spage=27749&rft.epage=27758&rft.pages=27749-27758&rft.issn=1932-7447&rft.eissn=1932-7455&rft_id=info:doi/10.1021/acs.jpcc.5b08116&rft_dat=%3Cacs_cross%3Ei82244801%3C/acs_cross%3E%3Cgrp_id%3Ecdi_FETCH-LOGICAL-a346t-c8b0f9123f456f6808edef2c3c0ad1a83f39f921731f82983e4cee3a23f5ad03%3C/grp_id%3E%3Coa%3E%3C/oa%3E%3Curl%3E%3C/url%3E&rft_id=info:oai/&rft_id=info:pmid/&rfr_iscdi=true |