2018
DOI: 10.1103/physrevb.97.241302
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Incipient singlet-triplet states in a hybrid mesoscopic system

Abstract: In the present work we provide an easily accessible way to achieve the singlet-triplet Kondo effect in a hybrid system consisting of a quantum point contact (QPC) coupled to an electronic cavity. We show that by activating the coupling between the QPC and cavity, a zero-bias anomaly occurs in a low conductance regime, a coexistence of zero-bias and finite-bias anomaly (FBA) in a medium conductance regime, and a FBA-only anomaly in a high conductance regime. The latter two observations are due to the singlet-tr… Show more

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Cited by 5 publications
(4 citation statements)
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“…This also applies to the case of the lateral quantization with the gap of ω x . Consequently, we can explain the diamond structure of the SBE lines in the V sd -V g plane observed in several QPC experiments [47][48][49][50][51][52][53][54][55][56][57][58]. The crossing points are at V sd = ±E Z /e, thus, as already employed [47], we can deduce the magnitude of the Zeeman gap, or the lateral quantization gap ( ω x ) from the diamond structure.…”
Section: B Zeeman Splitting Casementioning
confidence: 62%
See 1 more Smart Citation
“…This also applies to the case of the lateral quantization with the gap of ω x . Consequently, we can explain the diamond structure of the SBE lines in the V sd -V g plane observed in several QPC experiments [47][48][49][50][51][52][53][54][55][56][57][58]. The crossing points are at V sd = ±E Z /e, thus, as already employed [47], we can deduce the magnitude of the Zeeman gap, or the lateral quantization gap ( ω x ) from the diamond structure.…”
Section: B Zeeman Splitting Casementioning
confidence: 62%
“…This model attributes the disputed small plateau observed at approximately 0.7 •2e 2 /h to the perturbation effect: the perturbation effect opens a small gap at the crossing point (V sd = 0) of the SOI dispersion relation, which causes a small plateaulike conductance change. Furthermore, the peculiar SBE lines in the V g -V sd plane, which have been observed in many experiments such as [47][48][49][50][51][54][55][56][57], were reproduced comprehensively. The important features that agree with the experimental results are as follows: First, the SBE lines of the first diamond do not converge to V sd = 0 V, because the minima of the Rashba SOI dispersion deviate from V sd = 0.…”
Section: Soi Splitting Casementioning
confidence: 92%
“…* cgold@phys.ethz.ch However, we recently found a method to significantly enhance the sensitivity at non-depleting voltages (weaklyinvasive regime) [15], thus reducing the influence of the tip onto the unperturbed system. This method utilizes a gate-defined open cavity structure [16][17][18], which concentrates the scattering density of states behind the quantum point contact and thereby enables scanning gate experiments at strongly reduced voltages applied to the scanning gate. In this paper, we operate such a structure in the nonlinear bias regime and find the interaction effects previously observed for electron injection into an open two-dimensional electron gas [13] in this modified setting.…”
Section: Introductionmentioning
confidence: 99%
“…Recently, an accommodation for these two competing requirements of weakly invasive tip-potential and sufficient signal strength was found [26,30]. An open resonator structure of intermediate size [31][32][33] confines only fundamental one-dimensional cavity modes which can be uniquely identified and addressed [30]. This holds true even in slightly less open resonators [26].…”
Section: Introductionmentioning
confidence: 99%