Performance of Single-Electron Transistor Logic Composed of Multi-gate Single-Electron Transistors

1997 ◽  
Vol 36 (Part 1, No. 11) ◽  
pp. 6706-6710 ◽  
Author(s):  
Moon-Young Jeong ◽  
Yoon-Ha Jeong ◽  
Sung-Woo Hwang ◽  
Dae M. Kim
2006 ◽  
Vol 961 ◽  
Author(s):  
Christian Dubuc ◽  
Jacques Beauvais ◽  
Dominique Drouin

ABSTRACTWe report a single-electron transistor concept and its related process enabling the fabrication of ultrasmall junction capacitance. The method utilizes a nanodamascene approach where trenches in silicon oxide are covered with a filling material and planarized with chemical mechanical polishing. Single-electron transistors fabricated with this approach were characterized up to 433 K and demonstrated that the nanodamascene process has high resolution, is relatively simple and is highly scalable.


2002 ◽  
Vol 49 (4) ◽  
pp. 627-635 ◽  
Author(s):  
Dae Hwan Kim ◽  
Suk-Kang Sung ◽  
Kyung Rok Kim ◽  
Jong Duk Lee ◽  
Byung-Gook Park ◽  
...  

2002 ◽  
Vol 12 (04) ◽  
pp. 1101-1133 ◽  
Author(s):  
M. A. KASTNER

The single electron transistor (SET) is a nanometer-size device that turns on and off again every time one electron is added to it. In this article, the physics of the SET is reviewed. The consequences of confining electrons to a small region of space are that both the charge and energy are quantized. We review how the charge states and energy states of the confined electrons, sometimes called an artificial atom, are measured, and how the precision of these measurements depends on temperature. We also discuss the coupling of electrons inside the artificial atom to those in the leads of the SET, which results in the Kondo effect. We review measurements of the Kondo effect, which demonstrate that the Anderson Hamiltonian provides a quantitative description of the SET.


Author(s):  
Yoshiaki Iwata ◽  
Tomoki Nishimura ◽  
Alka Singh ◽  
Hiroaki Satoh ◽  
Hiroshi Inokawa

Abstract Metallic single-electron transistors (SETs) with niobium nanodots were fabricated, and their high-frequency rectifying characteristics were evaluated. By reducing the gap size of the electrodes and film deposition area to nanometer scale, improved SET characteristics with gate control, and better frequency response of the rectifying current with gentler decrease than 1/f at high frequency were achieved. The comparison between the characteristics of micrometer- and nanometer-size devices are made, and the reason for their differences are discussed with a help of simulation based on the experimentally extracted parameters.


VLSI Design ◽  
2001 ◽  
Vol 13 (1-4) ◽  
pp. 189-192 ◽  
Author(s):  
Xiaohui Wang ◽  
Wolfgang Porod

We present an analytical model for the I–V characteristics of a single-electron transistor, which may be incorporated in a conventional circuit simulator, such as SPICE. Our model takes as its input the physical SET characteristics (capacitances and tunnel resistances, which may be determined experimentally), and it yields I–V curves which are in excellent agreement with the ones obtained from full-scale Monte Carlo simulations.


Low power consumption, small device size and better controlled onto the charge carriers are the factors, that made Single-electron transistor (SET) a suitable candidate for molecular electronics; yet there are some improvements that can be done in order to use it practically. The single electron transistor (SET) operates through the tunnelling of electron via two tunnel junctions. Choosing a suitable island material plays a key role in the tunnelling of electron through the tunnel junctions. In the present work, the First principle calculations of carbon-nanotube and boron-nanotube based Single-Electron Transistors have been performed. The three types of configurations of nanotubes i.e. zigzag (5,0), armchair (3,3) and chiral (4,2), of the smallest possible diameter (approximately 4A ),have been used. The calculations have been carried out using Atomistic toolkit (ATK-VNL) simulation package which is a density functional theory (DFT) based package. In the present work, local density approximations (LDA) as well as generalized gradient approximation(GGA) have been used to demonstrate the properties of nanotubes-based SET. These approaches have been implemented for a nanotube that is lying just above the gate dielectric. On the either side of the dielectric the electrodes are present, source in the left and drain in the right. The metallic electrodes made of gold (W=5.28eV) and the dielectric material of the dielectric constant have been used. The charging energies and additional energies of both types of nanotubes-based SET in the isolated as well as in the electrostatic environment have been calculated using the approximations. The calculated values of the charging energies in the electrostatic environment have been found to be less than the charging energies in isolated configuration that shows the renormalization of molecular energy levels. Variations of total energies against gate voltages and Charge stability diagrams (CSD) have been discussed.


Author(s):  
Stephanus Hanurjaya ◽  
Miftahul Anwar ◽  
Meiyanto Eko Sulistyo ◽  
Irwan Iftadi ◽  
Subuh Pramono

<p class="Abstract">Single electron transistor (SET) has high potential for the development of quantum computing technologies in order to provide low power consumption electronics. For that purpose, many studies have been conducted to develop SET using dopants as quantum dots (QD). The working principle of SET basically is a single electron tunneling one by one through tunnel junction based on the coulomb blockade effect. This research will simulate various configurations of triple quantum dots single electron transistors (TQD-SET) using SIMON 2.0 with an experimental approach of MOSFET with dopants QD. The configurations used are series, parallel, and triangle configuration. The mutual capacitance (Cm), tunnel junctions (TJ), and temperature values of TQD-SET configurations are varied. The I-V characteristics are observed and analyzed for typical source-drain voltage (Vsd). it is found that the TQD series requires larger Vsd than parallel or triangular TQDs. On the other hands, the current in parallel TQD tends to be stable even though Cm is changed, and the current in the TQD triangle is strongly influenced by the Cm. By comparing these three configurations, it is observed that the tunnelling rate is higher for parallel TQD due to higher probability current moves through three dots by applying Vds.</p>


AIP Advances ◽  
2018 ◽  
Vol 8 (10) ◽  
pp. 105005
Author(s):  
Mitsuki Ito ◽  
Mamiko Yagi ◽  
Moe Shimada ◽  
Jun-ichi Shirakashi

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