2014
DOI: 10.1088/1367-2630/16/4/043018
|View full text |Cite
|
Sign up to set email alerts
|

Multiple quasiparticle Hall spectroscopy investigated with a resonant detector

Abstract: We investigate the finite frequency (FF) noise properties of edge states in the quantum Hall regime. We consider the measurement scheme of a resonant detector coupled to a quantum point contact in the weak-backscattering limit. A detailed analysis of the difference between the 'measured' noise, due to the presence of the resonant detector, and the symmetrized FF noise is presented. We discuss both the Laughlin and Jain sequences, studying the tunnelling excitations in these hierarchical models. We argue that t… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
39
0

Year Published

2016
2016
2021
2021

Publication Types

Select...
7

Relationship

1
6

Authors

Journals

citations
Cited by 31 publications
(39 citation statements)
references
References 75 publications
(281 reference statements)
0
39
0
Order By: Relevance
“…Starting from the lowest temperature case (T = 0.1 mK, black curves) we observe that both models show a flat behaviour at ω 0 /ω ≈ 0, which is a clear signature of the lack of contribution of ground states fluctuations in the considered measurement scheme [36]. The little deviation from zero are associated to the mismatch between the systems and detector temperature which can be always cancelled when T = T c [38]. Steep jumps associated to the 2-agglomerate contribution appear at |ω 0 |/ω = 1/2 showing an identical profile in both models, which reflects the same scaling dimension of the two model for that excitation (see (10)).…”
Section: Noise Properties In Qpc At Finite Frequencymentioning
confidence: 81%
See 2 more Smart Citations
“…Starting from the lowest temperature case (T = 0.1 mK, black curves) we observe that both models show a flat behaviour at ω 0 /ω ≈ 0, which is a clear signature of the lack of contribution of ground states fluctuations in the considered measurement scheme [36]. The little deviation from zero are associated to the mismatch between the systems and detector temperature which can be always cancelled when T = T c [38]. Steep jumps associated to the 2-agglomerate contribution appear at |ω 0 |/ω = 1/2 showing an identical profile in both models, which reflects the same scaling dimension of the two model for that excitation (see (10)).…”
Section: Noise Properties In Qpc At Finite Frequencymentioning
confidence: 81%
“…The previous behaviours can be explained in a simple way in the quantum limit (k B T c ω) for the detector and the shot-noise limit (k B T ω 0 ) for the system. In this case one has the contributions of single and double excitations for the two models (l = P,AP) [38] S meas (ω 0 ) ≈ α 1 Γ…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…We define the zero frequency noise as 56,80,[86][87][88] S =2 (−d, t), with J L2 the current operator of the inner channel on the left-moving edge [see Fig. 1(a)].…”
Section: A Single Voltage Pulsementioning
confidence: 99%
“…Experimental milestones have already been obtained, with the demonstration of on-demand coherent sources [19][20][21] able to inject single electrons in quantum Hall channels [22][23][24]. Moreover, interferometric setups with one or more quantum point contacts (QPCs) [25][26][27][28][29][30][31][32][33][34][35][36] have also been investigated. Possible extensions to topological insulators, where spin momentum locking plays an important role, have been also theoretically considered [37][38][39][40][41][42][43][44][45][46] and recently realized [47,48].…”
Section: Introductionmentioning
confidence: 99%