2006
DOI: 10.1063/1.2388134
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An ultrasensitive radio-frequency single-electron transistor working up to 4.2 K

Abstract: We present the fabrication and measurement of a radio frequency single electron transistor (rf-SET), that displays a very high charge sensitivity of 1.9 µe/ √ Hz at 4.2 K. At 40 mK, the charge sensitivity is 0.9 and 1.0 µe/ √ Hz in the superconducting and normal state respectively. The sensitivity was measured as a function of radio frequency amplitude at three different temperatures; 40 mK, 1.8 K and 4.2 K.

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Cited by 70 publications
(93 citation statements)
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“…3(a)]. From the height of the sidebands above the noise floor, the sensitivity is given by S C ¼ ð1= ffiffi ffi 2 p ÞδCðΔfÞ −1=2 10 −SNR=20 , where SNR is the sideband signal-to-noise ratio expressed in decibels, and Δf is the resolution bandwidth [21]. Over the range of varactor settings measured, S C is found to change by a factor > 15, with the best sensitivity close to perfect matching as expected [ Fig.…”
Section: Characterizing the Capacitance Sensitivitymentioning
confidence: 99%
“…3(a)]. From the height of the sidebands above the noise floor, the sensitivity is given by S C ¼ ð1= ffiffi ffi 2 p ÞδCðΔfÞ −1=2 10 −SNR=20 , where SNR is the sideband signal-to-noise ratio expressed in decibels, and Δf is the resolution bandwidth [21]. Over the range of varactor settings measured, S C is found to change by a factor > 15, with the best sensitivity close to perfect matching as expected [ Fig.…”
Section: Characterizing the Capacitance Sensitivitymentioning
confidence: 99%
“…We obtain a charge sensitivity of ␦q = 2.3ϫ 10 −6 e / ͱ Hz, which is nearly as good as the best Al/ AlO x results. 9 It represents an enhancement of at least a factor of 7 compared to previous carbon nanotube rf-SETs. [15][16][17] Very recently, comparable sensitivities were achieved with other types of SETs: ͑1͒ InAs/InP heterostructured nanowires 27 and ͑2͒ electrostatically defined Si quantum dots.…”
Section: Discussionmentioning
confidence: 99%
“…30 For Al/ AlO x junction SETs, the improvements at 40 mK were ␦q = 0.9e / ͱ Hz in the superconducting state and ␦q = 1.0e / ͱ Hz in the normal state. 9 To improve the bandwidth, the only option is to increase the resonance frequency of the LC-circuit. The limit set by the Bode-Fano criterium states that the maximum achievable bandwidth is ͑2R ⌺ C͒ −1 , which in our case amounts to ϳ170 MHz.…”
Section: Discussionmentioning
confidence: 99%
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“…3,4 In the so-called sequential tunneling regime, the blockade can be lifted and electrons may tunnel one-by-one through two small tunnel junctions under the control of a gate electrode, which couples to the SET island via a capacitance C g . As such the device current can be modulated periodically by a gate voltage with a period, V g = e/C g .…”
Section: Introductionmentioning
confidence: 99%