2004
DOI: 10.1002/cta.288
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Quantum transport, quantum effects and circuit functionality of nanostructured electronic circuits

Abstract: SUMMARYThis paper presents a discussion of the impact of quantum e ects to classical circuits. We will provide you with a brief introduction to our developed numerical tools to simulate electron tunnelling and energy discretization in MOS structures. Regarding these results a few arguments for simulating circuits including these e ects will be given.

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Cited by 7 publications
(7 citation statements)
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“…where J0 is the Josephson oscillating frequency according to (4). The resonant circuit consisting of L 1 , C 1 is considered to be the signal circuit, and the resonant circuit built by L 2 , C 2 represents the idler circuit.…”
Section: Langevin Theory Of the Dissipative Josephson Parametric Amplmentioning
confidence: 99%
“…where J0 is the Josephson oscillating frequency according to (4). The resonant circuit consisting of L 1 , C 1 is considered to be the signal circuit, and the resonant circuit built by L 2 , C 2 represents the idler circuit.…”
Section: Langevin Theory Of the Dissipative Josephson Parametric Amplmentioning
confidence: 99%
“…The whole structure is discretized in many square elements with a uniform grid spacing of a , along both x and z directions. On the basis of the ballistic transport model with NEGF method (a detailed introduction to it can be found in [7] [2]), the BPs are implemented in the device along the transport direction ( x ‐direction) for modeling the scattering effects.…”
Section: Theorymentioning
confidence: 99%
“…Σ S and Σ D are the so‐called self‐energy matrices which describe the coupling to the reservoir at the left end and the right end of the device . Ignoring all scattering processes in first approximation, the retarded Green's function relevant to the 1D ballistic transport is given with G(El)=[ElIHCΣS+ΣD]1.…”
Section: Theorymentioning
confidence: 99%
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“…where the energy E n ¼ E þ iZ is shifted in the complex plain by Z; ðZ ! 0Þ to ensure the invertibility of the coefficient matrix in Equation (12). Note that the overall Green's function G is a matrix of infinite size, due to coupling of semi-infinite contacts.…”
Section: Numerical Modellingmentioning
confidence: 99%