Direct observation of single-charge-detection capability of nanowire field-effect transistors
A single localized charge can quench the luminescence of a semiconductor nanowire 1 , but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interac...
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creator | Salfi, J Savelyev, I. G Blumin, M Nair, S. V Ruda, H. E |
description | A single localized charge can quench the luminescence of a semiconductor nanowire
1
, but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interaction and excitonic binding energy are much larger than the corresponding values when embedded in a material with the same dielectric permittivity
2
,
3
. The stronger Coulomb interaction is also predicted to limit the carrier mobility in nanowires
4
. Here, we experimentally isolate and study the effect of individual localized electrons on carrier transport in InAs nanowire field-effect transistors, and extract the equivalent charge sensitivity. In the low carrier density regime, the electrostatic potential produced by one electron can create an insulating weak link in an otherwise conducting nanowire field-effect transistor, modulating its conductance by as much as 4,200% at 31 K. The equivalent charge sensitivity, 4 × 10
−5
e
Hz
−1/2
at 25 K and 6 × 10
−5
e
Hz
−1/2
at 198 K, is orders of magnitude better than conventional field-effect transistors
5
and nanoelectromechanical systems
6
,
7
, and is just a factor of 20–30 away from the record sensitivity for state-of-the-art single-electron transistors operating below 4 K (ref.
8
). This work demonstrates the feasibility of nanowire-based single-electron memories
9
and illustrates a physical process of potential relevance for high performance chemical sensors
10
,
11
. The charge-state-detection capability we demonstrate also makes the nanowire field-effect transistor a promising host system for impurities (which may be introduced intentionally or unintentionally) with potentially long spin lifetimes
12
,
13
, because such transistors offer more sensitive spin-to-charge conversion readout than schemes based on conventional field-effect transistors
13
.
A single electron can modulate the conductance of an InAs nanowire field-effect transistor by as much as 4,200% at 31 K, and has a charge sensitivity of 6 × 10
−5
e
Hz
−1/2
up to ∼200 K. |
doi_str_mv | 10.1038/nnano.2010.180 |
format | Article |
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1
, but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interaction and excitonic binding energy are much larger than the corresponding values when embedded in a material with the same dielectric permittivity
2
,
3
. The stronger Coulomb interaction is also predicted to limit the carrier mobility in nanowires
4
. Here, we experimentally isolate and study the effect of individual localized electrons on carrier transport in InAs nanowire field-effect transistors, and extract the equivalent charge sensitivity. In the low carrier density regime, the electrostatic potential produced by one electron can create an insulating weak link in an otherwise conducting nanowire field-effect transistor, modulating its conductance by as much as 4,200% at 31 K. The equivalent charge sensitivity, 4 × 10
−5
e
Hz
−1/2
at 25 K and 6 × 10
−5
e
Hz
−1/2
at 198 K, is orders of magnitude better than conventional field-effect transistors
5
and nanoelectromechanical systems
6
,
7
, and is just a factor of 20–30 away from the record sensitivity for state-of-the-art single-electron transistors operating below 4 K (ref.
8
). This work demonstrates the feasibility of nanowire-based single-electron memories
9
and illustrates a physical process of potential relevance for high performance chemical sensors
10
,
11
. The charge-state-detection capability we demonstrate also makes the nanowire field-effect transistor a promising host system for impurities (which may be introduced intentionally or unintentionally) with potentially long spin lifetimes
12
,
13
, because such transistors offer more sensitive spin-to-charge conversion readout than schemes based on conventional field-effect transistors
13
.
A single electron can modulate the conductance of an InAs nanowire field-effect transistor by as much as 4,200% at 31 K, and has a charge sensitivity of 6 × 10
−5
e
Hz
−1/2
up to ∼200 K.</description><identifier>ISSN: 1748-3387</identifier><identifier>EISSN: 1748-3395</identifier><identifier>DOI: 10.1038/nnano.2010.180</identifier><identifier>PMID: 20852638</identifier><language>eng</language><publisher>London: Nature Publishing Group UK</publisher><subject>639/925/357/1016 ; 639/925/357/995 ; 639/925/927/1007 ; 639/925/927/356 ; Chemistry and Materials Science ; Conductance ; Electrons ; letter ; Luminescence ; Materials Science ; Molecular beam epitaxy ; Nanotechnology ; Nanotechnology and Microengineering ; Nanowires ; Sensors ; Transistors</subject><ispartof>Nature nanotechnology, 2010-10, Vol.5 (10), p.737-741</ispartof><rights>Springer Nature Limited 2010</rights><rights>Copyright Nature Publishing Group Oct 2010</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c456t-d1c903bcebd2b0bd3218ee5e445132308cf494182128ffc98c6fb0fe0668411a3</citedby><cites>FETCH-LOGICAL-c456t-d1c903bcebd2b0bd3218ee5e445132308cf494182128ffc98c6fb0fe0668411a3</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktopdf>$$Uhttps://link.springer.com/content/pdf/10.1038/nnano.2010.180$$EPDF$$P50$$Gspringer$$H</linktopdf><linktohtml>$$Uhttps://link.springer.com/10.1038/nnano.2010.180$$EHTML$$P50$$Gspringer$$H</linktohtml><link.rule.ids>314,780,784,2727,27924,27925,41488,42557,51319</link.rule.ids><backlink>$$Uhttps://www.ncbi.nlm.nih.gov/pubmed/20852638$$D View this record in MEDLINE/PubMed$$Hfree_for_read</backlink></links><search><creatorcontrib>Salfi, J</creatorcontrib><creatorcontrib>Savelyev, I. G</creatorcontrib><creatorcontrib>Blumin, M</creatorcontrib><creatorcontrib>Nair, S. V</creatorcontrib><creatorcontrib>Ruda, H. E</creatorcontrib><title>Direct observation of single-charge-detection capability of nanowire field-effect transistors</title><title>Nature nanotechnology</title><addtitle>Nature Nanotech</addtitle><addtitle>Nat Nanotechnol</addtitle><description>A single localized charge can quench the luminescence of a semiconductor nanowire
1
, but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interaction and excitonic binding energy are much larger than the corresponding values when embedded in a material with the same dielectric permittivity
2
,
3
. The stronger Coulomb interaction is also predicted to limit the carrier mobility in nanowires
4
. Here, we experimentally isolate and study the effect of individual localized electrons on carrier transport in InAs nanowire field-effect transistors, and extract the equivalent charge sensitivity. In the low carrier density regime, the electrostatic potential produced by one electron can create an insulating weak link in an otherwise conducting nanowire field-effect transistor, modulating its conductance by as much as 4,200% at 31 K. The equivalent charge sensitivity, 4 × 10
−5
e
Hz
−1/2
at 25 K and 6 × 10
−5
e
Hz
−1/2
at 198 K, is orders of magnitude better than conventional field-effect transistors
5
and nanoelectromechanical systems
6
,
7
, and is just a factor of 20–30 away from the record sensitivity for state-of-the-art single-electron transistors operating below 4 K (ref.
8
). This work demonstrates the feasibility of nanowire-based single-electron memories
9
and illustrates a physical process of potential relevance for high performance chemical sensors
10
,
11
. The charge-state-detection capability we demonstrate also makes the nanowire field-effect transistor a promising host system for impurities (which may be introduced intentionally or unintentionally) with potentially long spin lifetimes
12
,
13
, because such transistors offer more sensitive spin-to-charge conversion readout than schemes based on conventional field-effect transistors
13
.
A single electron can modulate the conductance of an InAs nanowire field-effect transistor by as much as 4,200% at 31 K, and has a charge sensitivity of 6 × 10
−5
e
Hz
−1/2
up to ∼200 K.</description><subject>639/925/357/1016</subject><subject>639/925/357/995</subject><subject>639/925/927/1007</subject><subject>639/925/927/356</subject><subject>Chemistry and Materials Science</subject><subject>Conductance</subject><subject>Electrons</subject><subject>letter</subject><subject>Luminescence</subject><subject>Materials Science</subject><subject>Molecular beam epitaxy</subject><subject>Nanotechnology</subject><subject>Nanotechnology and Microengineering</subject><subject>Nanowires</subject><subject>Sensors</subject><subject>Transistors</subject><issn>1748-3387</issn><issn>1748-3395</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2010</creationdate><recordtype>article</recordtype><sourceid>ABUWG</sourceid><sourceid>AFKRA</sourceid><sourceid>AZQEC</sourceid><sourceid>BENPR</sourceid><sourceid>CCPQU</sourceid><sourceid>DWQXO</sourceid><sourceid>GNUQQ</sourceid><recordid>eNp1kM1LAzEQxYMotlavHmURr9vma7fZo9RPKHjRoyxJdlJTttmapEr_e3fdWkHwNDPM770HD6FzgscEMzFxTrpmTHF3C3yAhmTKRcpYkR3udzEdoJMQlhhntKD8GA0oFhnNmRii1xvrQcekUQH8h4y2cUljkmDdooZUv0m_gLSC2DLdS8u1VLa2cdtRXfZnq0-MhbpKwZjOKnrpgg2x8eEUHRlZBzjbzRF6ubt9nj2k86f7x9n1PNU8y2NaEV1gpjSoiiqsKkaJAMiA84wwyrDQhhecCEqoMEYXQudGYQM4zwUnRLIRuux9175530CI5bLZeNdGliIXrGAUT1to3EPaNyF4MOXa25X025Lgsiuz_C6z7Mos2zJbwcXOdaNWUO3xn_ZaYNIDoX25Bfjf2H8tr3qFk3HjYW_5B_sC1TiONw</recordid><startdate>20101001</startdate><enddate>20101001</enddate><creator>Salfi, J</creator><creator>Savelyev, I. 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G</au><au>Blumin, M</au><au>Nair, S. V</au><au>Ruda, H. E</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Direct observation of single-charge-detection capability of nanowire field-effect transistors</atitle><jtitle>Nature nanotechnology</jtitle><stitle>Nature Nanotech</stitle><addtitle>Nat Nanotechnol</addtitle><date>2010-10-01</date><risdate>2010</risdate><volume>5</volume><issue>10</issue><spage>737</spage><epage>741</epage><pages>737-741</pages><issn>1748-3387</issn><eissn>1748-3395</eissn><abstract>A single localized charge can quench the luminescence of a semiconductor nanowire
1
, but relatively little is known about the effect of single charges on the conductance of the nanowire. In one-dimensional nanostructures embedded in a material with a low dielectric permittivity, the Coulomb interaction and excitonic binding energy are much larger than the corresponding values when embedded in a material with the same dielectric permittivity
2
,
3
. The stronger Coulomb interaction is also predicted to limit the carrier mobility in nanowires
4
. Here, we experimentally isolate and study the effect of individual localized electrons on carrier transport in InAs nanowire field-effect transistors, and extract the equivalent charge sensitivity. In the low carrier density regime, the electrostatic potential produced by one electron can create an insulating weak link in an otherwise conducting nanowire field-effect transistor, modulating its conductance by as much as 4,200% at 31 K. The equivalent charge sensitivity, 4 × 10
−5
e
Hz
−1/2
at 25 K and 6 × 10
−5
e
Hz
−1/2
at 198 K, is orders of magnitude better than conventional field-effect transistors
5
and nanoelectromechanical systems
6
,
7
, and is just a factor of 20–30 away from the record sensitivity for state-of-the-art single-electron transistors operating below 4 K (ref.
8
). This work demonstrates the feasibility of nanowire-based single-electron memories
9
and illustrates a physical process of potential relevance for high performance chemical sensors
10
,
11
. The charge-state-detection capability we demonstrate also makes the nanowire field-effect transistor a promising host system for impurities (which may be introduced intentionally or unintentionally) with potentially long spin lifetimes
12
,
13
, because such transistors offer more sensitive spin-to-charge conversion readout than schemes based on conventional field-effect transistors
13
.
A single electron can modulate the conductance of an InAs nanowire field-effect transistor by as much as 4,200% at 31 K, and has a charge sensitivity of 6 × 10
−5
e
Hz
−1/2
up to ∼200 K.</abstract><cop>London</cop><pub>Nature Publishing Group UK</pub><pmid>20852638</pmid><doi>10.1038/nnano.2010.180</doi><tpages>5</tpages></addata></record> |
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subjects | 639/925/357/1016 639/925/357/995 639/925/927/1007 639/925/927/356 Chemistry and Materials Science Conductance Electrons letter Luminescence Materials Science Molecular beam epitaxy Nanotechnology Nanotechnology and Microengineering Nanowires Sensors Transistors |
title | Direct observation of single-charge-detection capability of nanowire field-effect transistors |
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