1998
DOI: 10.1116/1.590412
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Direct patterning of single electron tunneling transistors by high resolution electron beam lithography on highly doped molecular beam epitaxy grown silicon films

Abstract: Articles you may be interested inSingle-electron transistor structures based on silicon-on-insulator silicon nanowire fabrication by scanning probe lithography and wet etching

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Cited by 8 publications
(4 citation statements)
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“…However, some oscillation peaks remain up to about 60 K for both devices. Since the CB effect becomes prominent if the charging energy exceeds the thermal energy , there is a relation between and , , where is the Boltzmann constant and is the maximum temperature for the CB operation [30]. From this relationship, the charging energy is calculated to be 5.2 meV.…”
Section: Device Characteristicsmentioning
confidence: 99%
“…However, some oscillation peaks remain up to about 60 K for both devices. Since the CB effect becomes prominent if the charging energy exceeds the thermal energy , there is a relation between and , , where is the Boltzmann constant and is the maximum temperature for the CB operation [30]. From this relationship, the charging energy is calculated to be 5.2 meV.…”
Section: Device Characteristicsmentioning
confidence: 99%
“…One approach to avoid such a complex feature might be the use of doped Si wires on SOI wafers. Many groups have reported SETs based on doped Si wires [39][40][41][42][43]. Some of them utilized multiple-island structures originating from the random fluctuation in a Si wire, which might be related to the doping level or in the wire width [39,40].…”
Section: Island Formation By Lithographymentioning
confidence: 99%
“…Many groups have reported SETs based on doped Si wires [39][40][41][42][43]. Some of them utilized multiple-island structures originating from the random fluctuation in a Si wire, which might be related to the doping level or in the wire width [39,40]. Another reported rather periodical CB oscillations similar to those of SETs with a single metal island [41][42][43].…”
Section: Island Formation By Lithographymentioning
confidence: 99%
“…Silicon [or silicon-on insulator (SOI)] is, in principle, an attractive material for QD experiments due to its highly developed fabrication technology and the potential integration of QD devices with conventional electronics circuits. , Previous approaches toward building QD systems on SOI substrates have mainly focused on obtaining ultrathin NWs from lithography followed by etching procedures to reduce the NW width. Single-electron effects have been observed in these devices, but the results disagree with the designed device geometry; the etching processes introduce defects and roughness that, in turn, lead to the random formation of QDs within the nanostructure and irreproducible transport characteristics. For example, Coulomb blockade diamond diagrams, a signature of single-electron charging, are typically not obtainable because the change of signal in consecutive scans can be much larger than the gate influence .…”
Section: Introduction and Experimental Backgroundmentioning
confidence: 99%