Single-electron transistor: Difference between revisions

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Fixed a link target to point to the tunnel junction page, rather than just quantum tunelling itself. Moved link earlier in article.
 
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{{Short description|Electronic device}}
[[File:SET schematic2.jpg|thumb|Schematic of a basic SET and its internal electrical components]]
 
A '''single-electron transistor''' ('''SET''') is a sensitive electronic device based on the [[Coulomb blockade]] effect. In this device the electrons flow through a [[tunnel junction]] between source/drain to a [[quantum dot]] (conductive island). Moreover, the electrical potential of the island can be tuned by a third electrode, known as the gate, which is capacitively coupled to the island. The conductive island is sandwiched between two tunnel junctions<ref>{{cite journal|last1=Mahapatra|first1=S.|last2=Vaish|first2=V.|last3=Wasshuber|first3=C.|last4=Banerjee|first4=K.|last5=Ionescu|first5=A.M.|title=Analytical Modeling of Single Electron Transistor for Hybrid CMOS-SET Analog IC Design|journal=IEEE Transactions on Electron Devices|volume=51|issue=11|year=2004|pages=1772–1782|issn=0018-9383|doi=10.1109/TED.2004.837369|bibcode=2004ITED...51.1772M|s2cid=15373278}}</ref> modeled by capacitors, <math>C_{\rm D}</math> and <math>C_{\rm S}</math>, and resistors, <math>R_{\rm D}</math> and <math>R_{\rm S}</math>, in parallel.
 
== History ==
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[[File:Single electron transistor.svg|thumb|right|Left to right: energy levels of source, island and drain in a single-electron transistor for the blocking state (upper part) and transmitting state (lower part).]]
 
The SET has, like the [[field-effect transistor|FET]], three electrodes: source, drain, and a gate. The main technological difference between the transistor types is in the channel concept. While the channel changes from insulated to conductive with applied gate voltage in the FET, the SET is always insulated. The source and drain are coupled through two [[Quantum tunnelling|tunnel junctions]], separated by a metallic or semiconductor-based [[quantum dot|quantum nanodot]] (QD),<ref name="UchidaMatsuzawa2000">{{cite journal|last1=Uchida|first1=Ken|last2=Matsuzawa|first2=Kazuya|last3=Koga|first3=Junji|last4=Ohba|first4=Ryuji|last5=Takagi|first5=Shin-ichi|last6=Toriumi|first6=Akira|title=Analytical Single-Electron Transistor (SET) Model for Design and Analysis of Realistic SET Circuits|journal=Japanese Journal of Applied Physics|volume=39|issue=Part 1, No. 4B|year=2000|pages=2321–2324|issn=0021-4922|doi=10.1143/JJAP.39.2321|bibcode=2000JaJAP..39.2321U}}</ref> also known as the "island". The electrical potential of the QD can be tuned with the capacitively coupled gate electrode to alter the resistance, by applying a positive voltage the QD will change from blocking to non-blocking state and electrons will start tunnelling to the QD. This phenomenon is known as the [[Coulomb blockade]].
 
The current, <math>I,</math> from source to drain follows [[Ohm's law]] when <math>V_{\rm SD}</math> is applied, and it equals <math>\tfrac{V_{\rm SD}}{R},</math> where the main contribution of the resistance, <math>R,</math> comes from the tunnelling effects when electrons move from source to QD, and from QD to drain. <math>V_{\rm G}</math> regulates the resistance of the QD, which regulates the current. This is the exact same behaviour as in regular FETs. However, when moving away from the macroscopic scale, the quantum effects will affect the current, <math>I.</math>
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At zero temperatures, only transitions with negative free energy are allowed: <math>\Delta F_{\rm S} < 0</math> or <math>\Delta F_{\rm D} < 0</math>. These conditions can be used to find areas of stability in the plane <math>V_{\rm bias} - V_{\rm G}.</math>
 
With increasing voltage at the gate electrode, when the supply voltage is maintaintedmaintained below the voltage of the Coulomb blockade (i.e. <math>V_{\rm bias} < \tfrac{e}{C_{\rm S} + C_{\rm D}}</math>), the drain output current will oscillate with a period <math>\tfrac{e}{C_{\rm S} + C_{\rm D}}.</math> These areas correspond to failures in the field of stability. The oscillations of the tunnelling current occur in time, and the oscillations in two series-connected junctions have a periodicity in the gate control voltage. The thermal broadening of the oscillations increases to a large extent with increasing temperature.
 
=== Temperature dependence ===
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The level of the electrical current of the SET can be amplified enough to work with available [[CMOS]] technology by generating a hybrid SET–[[field-effect transistor|FET]] device.<ref name="IonescuMahapatra2004">{{cite journal|last1=Ionescu|first1=A.M.|last2=Mahapatra|first2=S.|last3=Pott|first3=V.|title=Hybrid SETMOS Architecture With Coulomb Blockade Oscillations and High Current Drive|journal=IEEE Electron Device Letters|volume=25|issue=6|year=2004|pages=411–413|issn=0741-3106|doi=10.1109/LED.2004.828558|bibcode=2004IEDL...25..411I|s2cid=42715316}}</ref><ref name="AmatBausells2017">{{cite journal|last1=Amat|first1=Esteve|last2=Bausells|first2=Joan|last3=Perez-Murano|first3=Francesc|title=Exploring the Influence of Variability on Single-Electron Transistors Into SET-Based Circuits|journal=IEEE Transactions on Electron Devices|volume=64|issue=12|year=2017|pages=5172–5180|issn=0018-9383|doi=10.1109/TED.2017.2765003|bibcode=2017ITED...64.5172A|s2cid=22082690}}</ref>
 
The EU funded, in 2016, project IONS4SET (#688072)<ref>{{cite web|url=http://www.ions4set.eu|title=IONS4SET Website|access-date=2019-09-17}}</ref> looks for the manufacturability of SET–FET circuits operative at room temperature. The main goal of this project is to design a SET-manufacturability process-flow for large-scale operations seeking to extend the use of the hybrid SET–CMOS architectures. To assure room temperature operation, single dots of diameters below 5&nbsp;nm have to be fabricated and located between source and drain with tunnel distances of a few nanometers.<ref name="KlupfelBurenkov2016">{{cite book|last1=Klupfel|first1=F. J.|title=2016 International Conference on Simulation of Semiconductor Processes and Devices (SISPAD)|last2=Burenkov|first2=A.|last3=Lorenz|first3=J.|chapter=Simulation of silicon-dot-based single-electron memory devices|year=2016|pages=237–240|doi=10.1109/SISPAD.2016.7605191|isbn=978-1-5090-0818-6|s2cid=15721282}}</ref> Up to now there is no reliable process-flow to manufacture a hybrid SET–FET circuit operative at room temperature. In this context, this EU project explores a more feasible way to manufacture the SET–FET circuit by using pillar dimensions of approximately 10&nbsp;nm.<ref name="Xu2019">{{cite arXivjournal |eprintarxiv=1906.09975v2|last1=Xu|first1=Xiaomo|title=Morphology modification of Si nanopillars under ion irradiation at elevated temperatures: Plastic deformation and controlled thinning to 10 nm|last2=Heinig|first2=Karl-Heinz|last3=Möller|first3=Wolfhard|last4=Engelmann|first4=Hans-Jürgen|last5=Klingner|first5=Nico|last6=Gharbi|first6=Ahmed|last7=Tiron|first7=Raluca|author8=Johannes von Borany|last9=Hlawacek|first9=Gregor|classjournal=physics.app-phSemiconductor Science and Technology |year=2019|volume=35 |issue=1 |page=015021 |doi=10.1088/1361-6641/ab57ba |bibcode=2020SeScT..35a5021X }}</ref>
 
== See also ==