2018
DOI: 10.1088/1674-1056/27/9/097310
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Transport spectroscopy through dopant atom array in silicon junctionless nanowire transistors

Abstract: We demonstrate electron transport spectroscopy through a dopant atom array in n-doped silicon junctionless nanowire transistors within a temperature range from 6 K to 250 K. Several current steps are observed at the initial stage of the transfer curves below 75 K, which result from the electron transport from Hubbard bands to one-dimensional conduction band. The current-off voltages in the transfer curves have a strikingly positive shift below 20 K and a negative shift above 20 K due to the electrostatic scree… Show more

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Cited by 5 publications
(3 citation statements)
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“…where k B is the Boltzmann's constant and E a represents the activation energy. [13] The activation energy E a has the minima at the current peak positions and the maxima at the current valley positions. Within the higher temperature range of 30-70 K, the linear dependence of the activation energy shows a good gate conversion factor α = 0.113 for the gate voltage range from 1.0 V to 1.25 V, in which the tunneling barrier height is modulated linearly for an isolated dopant-induced QD by the gate voltage.…”
Section: Resultsmentioning
confidence: 99%
“…where k B is the Boltzmann's constant and E a represents the activation energy. [13] The activation energy E a has the minima at the current peak positions and the maxima at the current valley positions. Within the higher temperature range of 30-70 K, the linear dependence of the activation energy shows a good gate conversion factor α = 0.113 for the gate voltage range from 1.0 V to 1.25 V, in which the tunneling barrier height is modulated linearly for an isolated dopant-induced QD by the gate voltage.…”
Section: Resultsmentioning
confidence: 99%
“…With the gate voltage increasing, the Fermi energy level of electrons in the quantum confined channel is allowed to enter the conduction subbands, resulting in the current steps. [28,29] In order to study the temperature-dependent conductance G characteristics in Fig. 2(a), we firstly extract the experimental conductance data for different temperatures according to the initial g m peak at the gate voltage V g1 , in which the effective mobility of hopping electrons is the highest in the impu-rity band.…”
Section: Resultsmentioning
confidence: 99%
“…[13,14] However, the design of CMOS qubitcontrol circuits at cryogenic temperatures is a difficult task, since the physical modeling of cryogenic temperature MOS-FETs operation is not so fully developed due to the sophisticated physics at 4.2 K compared to room temperature. [15][16][17][18][19] Thus, the cryo-CMOS device modeling and simulation down to 4.2 K are not adequate yet.…”
Section: Introductionmentioning
confidence: 99%