2007
DOI: 10.1103/physrevb.76.085419
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Manipulation of resonances in an open three-terminal interferometer with an embedded quantum dot

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Cited by 22 publications
(16 citation statements)
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“…Hence, the general incoming and outgoing wave functions in the leads from the solution of Eq. (7) may be written as [25,26] ψ n = e inθ + re −inθ , n 0,…”
Section: Theoretical Model and Calculationsmentioning
confidence: 99%
“…Hence, the general incoming and outgoing wave functions in the leads from the solution of Eq. (7) may be written as [25,26] ψ n = e inθ + re −inθ , n 0,…”
Section: Theoretical Model and Calculationsmentioning
confidence: 99%
“…Consider an extension of the two-terminal continuum model described in section 3.1 to the case of three terminals. In a mesoscopic system or in the absence of magnetic fields, such devices have been considered by several groups (see [134][135][136][137][138][139][140][141][142][143][144]). An illustration of the three-terminal set-up is given in figure 7.…”
Section: Three-terminal Devicesmentioning
confidence: 99%
“…Each pole is connected with a resonance level (or a quasibound state). According to the Breit-Wigner formalism, the real part of a pole presents the energy of a quasibound state, and the imaginary part is related to the lifetime of the resonance level [20,21]. In Fig.…”
Section: B Scattering In Subspace With All Spin Downmentioning
confidence: 99%