Nanoelectronics and Nanosystems 2004
DOI: 10.1007/978-3-662-05421-5_12
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Nanoelectronics with Tunneling Devices

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Cited by 5 publications
(6 citation statements)
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“…These single-electron nanodevices ,, are possible due to the carrier confinement and Coulomb blockade effects exhibited by the very narrow SiNWs and/or very small SiNDs in the nano regime. Indeed, 15 nm wide silicon nanowire channel and 5−10 nm isolated silicon islands were used in the work of Tsutsumi, et al This is a fast-developing technology; the reader is referred to many excellent reviews and books in the literature. ,
105 SEM photograph of the Si nanowire and side gates fabricated by using inorganic electron beam (EB) resist process. The width, height, and length of the Si nanowire are 15, 20, and 438 nm, respectively.
…”
Section: 1 Top-down Approachmentioning
confidence: 99%
“…These single-electron nanodevices ,, are possible due to the carrier confinement and Coulomb blockade effects exhibited by the very narrow SiNWs and/or very small SiNDs in the nano regime. Indeed, 15 nm wide silicon nanowire channel and 5−10 nm isolated silicon islands were used in the work of Tsutsumi, et al This is a fast-developing technology; the reader is referred to many excellent reviews and books in the literature. ,
105 SEM photograph of the Si nanowire and side gates fabricated by using inorganic electron beam (EB) resist process. The width, height, and length of the Si nanowire are 15, 20, and 438 nm, respectively.
…”
Section: 1 Top-down Approachmentioning
confidence: 99%
“…Extensive theoretical work to calculate current-voltage (I-V) characteristics of single molecules was developed [1][2][3][4][5][6] right after the first break-junction experiment addressing a single molecule was reported [7]. Most of these theoretical techniques involved the use of the Landauer formalism [8] in order to have a relation between the response current of an applied voltage to a nano-sized molecular junction.…”
mentioning
confidence: 99%
“…where without loss of generality we have considered zero ground state energy of H − 0 and the two partner potentials V ∓ 0 can be written in terms of superpotential W 0 and mass function, as 4) which implies that for a physically acceptable mass function 1 the superpotential and hence two partner potentials V ∓ 0 are free from singularity (provided the given potential V − 0 is without any singularity). It is well established that when SUSY is unbroken then the spectrum of the two PDM partner Hamiltonians H ∓ are degenerate except for the lowest energy of H − 0 .…”
Section: A Usual Factorizationmentioning
confidence: 99%
“…The concept of position dependent mass comes from the effective mass approximation [3] which is an useful tool for studying the motion of carrier electrons in pure crystals and also for the virtual-crystal approximation in the treatment of homogeneous alloys as well as in graded mixed semiconductors. This field has also arisen due to the impressive development in crystallographic growth techniques [4] which allow the production of non uniform semiconductor specimen with abrupt heterojunctions (see e.g., [5] for a review). In different areas of possible applications of low dimensional structures as already mentioned, there is need to have Hamiltonians with predetermined energy spectrum.…”
Section: Introductionmentioning
confidence: 99%