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Stability Diagrams of Triple-Dot Single-Electron Device with Single Common Gate
Triple-dot single-electron devices with a single common gate have been studied. The overall stability diagram of the single-electron device with a homogeneous tunnel capacitance $C_{\text{j}}$ and a homogeneous gate capacitance $C_{\text{g}}$ is derived algebraically. If the set of excess electron n...
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Published in: | Japanese Journal of Applied Physics 2011-03, Vol.50 (3), p.034302-034302-9 |
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description | Triple-dot single-electron devices with a single common gate have been studied. The overall stability diagram of the single-electron device with a homogeneous tunnel capacitance $C_{\text{j}}$ and a homogeneous gate capacitance $C_{\text{g}}$ is derived algebraically. If the set of excess electron numbers in the three islands $(n_{1}, n_{2}, n_{3})$ is $(n, n, n)$, $(n, n + 1, n)$, or $(n, n - 1, n)$, where $n$ is an arbitrary integer, the corresponding stability region $\mathrm{S}(n_{1}, n_{2}, n_{3})$ exists for any $C_{\text{g}}/C_{\text{j}}$. $\mathrm{S}(n, n, n)$, $\mathrm{S}(n, n + 1, n)$, and $\mathrm{S}(n, n - 1, n)$ for all $n$ are arranged along the $V_{\text{g}}$ axis in the order of $n_{1} + n_{2} + n_{3}$, where $V_{\text{g}}$ is gate voltage, and neighboring stability regions overlap for any $C_{\text{g}}/C_{\text{j}}$ ratio. Overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ for all $n$ have identical kite-like shapes. Overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ for all $n$ have identical rhombus shapes. Turnstile operations are possible by alternating gate voltage around overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ and around overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$, though the sequences of single-electron transfers are different. The range of drain voltage and the swing of gate voltage for turnstile operation are estimated. The overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ seems superior to the overlap between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ because of the larger ratio of the drain voltage range to the gate voltage swing, though the overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ might require higher reliability against the nonuniformity of gate capacitances. |
doi_str_mv | 10.1143/JJAP.50.034302 |
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The overall stability diagram of the single-electron device with a homogeneous tunnel capacitance $C_{\text{j}}$ and a homogeneous gate capacitance $C_{\text{g}}$ is derived algebraically. If the set of excess electron numbers in the three islands $(n_{1}, n_{2}, n_{3})$ is $(n, n, n)$, $(n, n + 1, n)$, or $(n, n - 1, n)$, where $n$ is an arbitrary integer, the corresponding stability region $\mathrm{S}(n_{1}, n_{2}, n_{3})$ exists for any $C_{\text{g}}/C_{\text{j}}$. $\mathrm{S}(n, n, n)$, $\mathrm{S}(n, n + 1, n)$, and $\mathrm{S}(n, n - 1, n)$ for all $n$ are arranged along the $V_{\text{g}}$ axis in the order of $n_{1} + n_{2} + n_{3}$, where $V_{\text{g}}$ is gate voltage, and neighboring stability regions overlap for any $C_{\text{g}}/C_{\text{j}}$ ratio. Overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ for all $n$ have identical kite-like shapes. Overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ for all $n$ have identical rhombus shapes. Turnstile operations are possible by alternating gate voltage around overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ and around overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$, though the sequences of single-electron transfers are different. The range of drain voltage and the swing of gate voltage for turnstile operation are estimated. The overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ seems superior to the overlap between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ because of the larger ratio of the drain voltage range to the gate voltage swing, though the overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ might require higher reliability against the nonuniformity of gate capacitances.</description><identifier>ISSN: 0021-4922</identifier><identifier>EISSN: 1347-4065</identifier><identifier>DOI: 10.1143/JJAP.50.034302</identifier><language>eng</language><publisher>The Japan Society of Applied Physics</publisher><ispartof>Japanese Journal of Applied Physics, 2011-03, Vol.50 (3), p.034302-034302-9</ispartof><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><citedby>FETCH-LOGICAL-c274t-af980c05c48dab9f5557419a8990946abf4318da9053c09ff0a53e3ddae4d3a83</citedby><cites>FETCH-LOGICAL-c274t-af980c05c48dab9f5557419a8990946abf4318da9053c09ff0a53e3ddae4d3a83</cites></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><link.rule.ids>314,776,780,27898,27899</link.rule.ids></links><search><creatorcontrib>Imai, Shigeru</creatorcontrib><title>Stability Diagrams of Triple-Dot Single-Electron Device with Single Common Gate</title><title>Japanese Journal of Applied Physics</title><description>Triple-dot single-electron devices with a single common gate have been studied. The overall stability diagram of the single-electron device with a homogeneous tunnel capacitance $C_{\text{j}}$ and a homogeneous gate capacitance $C_{\text{g}}$ is derived algebraically. If the set of excess electron numbers in the three islands $(n_{1}, n_{2}, n_{3})$ is $(n, n, n)$, $(n, n + 1, n)$, or $(n, n - 1, n)$, where $n$ is an arbitrary integer, the corresponding stability region $\mathrm{S}(n_{1}, n_{2}, n_{3})$ exists for any $C_{\text{g}}/C_{\text{j}}$. $\mathrm{S}(n, n, n)$, $\mathrm{S}(n, n + 1, n)$, and $\mathrm{S}(n, n - 1, n)$ for all $n$ are arranged along the $V_{\text{g}}$ axis in the order of $n_{1} + n_{2} + n_{3}$, where $V_{\text{g}}$ is gate voltage, and neighboring stability regions overlap for any $C_{\text{g}}/C_{\text{j}}$ ratio. Overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ for all $n$ have identical kite-like shapes. Overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ for all $n$ have identical rhombus shapes. Turnstile operations are possible by alternating gate voltage around overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ and around overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$, though the sequences of single-electron transfers are different. The range of drain voltage and the swing of gate voltage for turnstile operation are estimated. The overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ seems superior to the overlap between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ because of the larger ratio of the drain voltage range to the gate voltage swing, though the overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ might require higher reliability against the nonuniformity of gate capacitances.</description><issn>0021-4922</issn><issn>1347-4065</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2011</creationdate><recordtype>article</recordtype><recordid>eNqFkMFPwjAUhxujiRO9eu7ZZPN1bWE9koEoIcEEPDePrsWajS1do-G_ZwTunt57-X6_d_gIeWaQMSb463I5_cwkZMAFh_yGJIyLSSpgLG9JApCzVKg8vycPff8znGMpWELWm4g7X_t4pDOP-4BNT1tHt8F3tU1nbaQbf9gP67y2Job2QGf21xtL_3z8vjJatk0zkAVG-0juHNa9fbrOEfl6m2_L93S1XnyU01Vq8omIKTpVgAFpRFHhTjkp5UQwhYVSoMQYd05wNiAFkhtQzgFKbnlVoRUVx4KPSHb5a0Lb98E63QXfYDhqBvqsQ591aAn6omMovFwKvsPuv_AJmUdfZQ</recordid><startdate>20110301</startdate><enddate>20110301</enddate><creator>Imai, Shigeru</creator><general>The Japan Society of Applied Physics</general><scope>AAYXX</scope><scope>CITATION</scope></search><sort><creationdate>20110301</creationdate><title>Stability Diagrams of Triple-Dot Single-Electron Device with Single Common Gate</title><author>Imai, Shigeru</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-c274t-af980c05c48dab9f5557419a8990946abf4318da9053c09ff0a53e3ddae4d3a83</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2011</creationdate><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Imai, Shigeru</creatorcontrib><collection>CrossRef</collection><jtitle>Japanese Journal of Applied Physics</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Imai, Shigeru</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Stability Diagrams of Triple-Dot Single-Electron Device with Single Common Gate</atitle><jtitle>Japanese Journal of Applied Physics</jtitle><date>2011-03-01</date><risdate>2011</risdate><volume>50</volume><issue>3</issue><spage>034302</spage><epage>034302-9</epage><pages>034302-034302-9</pages><issn>0021-4922</issn><eissn>1347-4065</eissn><abstract>Triple-dot single-electron devices with a single common gate have been studied. The overall stability diagram of the single-electron device with a homogeneous tunnel capacitance $C_{\text{j}}$ and a homogeneous gate capacitance $C_{\text{g}}$ is derived algebraically. If the set of excess electron numbers in the three islands $(n_{1}, n_{2}, n_{3})$ is $(n, n, n)$, $(n, n + 1, n)$, or $(n, n - 1, n)$, where $n$ is an arbitrary integer, the corresponding stability region $\mathrm{S}(n_{1}, n_{2}, n_{3})$ exists for any $C_{\text{g}}/C_{\text{j}}$. $\mathrm{S}(n, n, n)$, $\mathrm{S}(n, n + 1, n)$, and $\mathrm{S}(n, n - 1, n)$ for all $n$ are arranged along the $V_{\text{g}}$ axis in the order of $n_{1} + n_{2} + n_{3}$, where $V_{\text{g}}$ is gate voltage, and neighboring stability regions overlap for any $C_{\text{g}}/C_{\text{j}}$ ratio. Overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ for all $n$ have identical kite-like shapes. Overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ for all $n$ have identical rhombus shapes. Turnstile operations are possible by alternating gate voltage around overlaps between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ and around overlaps between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$, though the sequences of single-electron transfers are different. The range of drain voltage and the swing of gate voltage for turnstile operation are estimated. The overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ seems superior to the overlap between $\mathrm{S}(n, n, n)$ and $\mathrm{S}(n, n \pm 1, n)$ because of the larger ratio of the drain voltage range to the gate voltage swing, though the overlap between $\mathrm{S}(n, n + 1, n)$ and $\mathrm{S}(n + 1, n, n + 1)$ might require higher reliability against the nonuniformity of gate capacitances.</abstract><pub>The Japan Society of Applied Physics</pub><doi>10.1143/JJAP.50.034302</doi></addata></record> |
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title | Stability Diagrams of Triple-Dot Single-Electron Device with Single Common Gate |
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