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Superlattices and Microstructures, 1986
Abstract The electronic Schroedinger Equation for devices which are small compared to the inelastic scattering length of electrons is solved by a transformation to an equivalent quantum circuit which is numerically tractable. The method is applied to dirty wires and reveals the existence of anomalously conductive states.
T.J. Godin, Roger Haydock
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Abstract The electronic Schroedinger Equation for devices which are small compared to the inelastic scattering length of electrons is solved by a transformation to an equivalent quantum circuit which is numerically tractable. The method is applied to dirty wires and reveals the existence of anomalously conductive states.
T.J. Godin, Roger Haydock
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Circuit Theory in Circuit Simulation
IEEE Circuits and Systems Magazine, 2016This paper stresses the importance of applying circuit theory in circuit simulation. Circuit simulation is a combination of circuit theory and numerical analysis. Both the theoretical basis and the numerical algorithms should be robust and accurate to produce reliable and correct results.
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Circuit Theory of Andreev Conductance
Physical Review Letters, 1994Conductance of small normal metal structures adjacent to a superconductor is determined by coherent Andreev reflection. We show that under certain limitations the conductance can be found by means of an extended circuit theory. The theory deals with two types of elements: tunnel junctions and diffusive conductors and provides the basis for practical ...
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Theory of three circuit transformers
Journal of the A.I.E.E., 1924The characteristics of three-circuit transformers, the literature of which is very meager, are discussed here in considerable detail. The features of the scheme of treatment are as follows: 1. The scope and general aspects of the problems of three-circuit transformers are reviewed. 2.
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1981
An emf is a device that always maintains the same voltage across its terminals regardless of the current passing through it. A steady emf is represented by the symbol shown in Figure 31.1, where the long bar indicates positive voltage (+) and the shorter bar negative voltage (—).
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An emf is a device that always maintains the same voltage across its terminals regardless of the current passing through it. A steady emf is represented by the symbol shown in Figure 31.1, where the long bar indicates positive voltage (+) and the shorter bar negative voltage (—).
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Journal of the Physical Society of Japan, 1952
The electric current \(\dot{I}\) and the volage \(\dot{V}\) on the imagined surface S are defined by \(\dot{I}\textbf{\itshape F}=\textbf{\itshape H}^{t}\), \(\dot{P}=\dot{V}\tilde{I}\) or \(\dot{I}\textbf{\itshape F}=\textbf{\itshape E}\), \(\tilde{P}=\dot{V}\tilde{I}\), where H t , E t are tangential magnetic and electric field components on S , and ...
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The electric current \(\dot{I}\) and the volage \(\dot{V}\) on the imagined surface S are defined by \(\dot{I}\textbf{\itshape F}=\textbf{\itshape H}^{t}\), \(\dot{P}=\dot{V}\tilde{I}\) or \(\dot{I}\textbf{\itshape F}=\textbf{\itshape E}\), \(\tilde{P}=\dot{V}\tilde{I}\), where H t , E t are tangential magnetic and electric field components on S , and ...
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