2018
DOI: 10.1103/physrevlett.121.257701
|View full text |Cite
|
Sign up to set email alerts
|

Supercurrent in a Double Quantum Dot

Abstract: We demonstrate the Josephson effect in a serial double quantum dot defined in a nanowire with epitaxial superconducting leads. The supercurrent stability diagram adopts a honeycomb pattern with electron-hole and left-right reflection symmetry. We observe sharp discontinuities in the magnitude of the critical current, Ic, as a function of dot occupation, related to doublet to singlet ground state transitions. Detuning of the energy levels offers a tuning knob for Ic, which attains a maximum at zero detuning. Th… 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

2
62
0

Year Published

2019
2019
2023
2023

Publication Types

Select...
6
2
1

Relationship

1
8

Authors

Journals

citations
Cited by 56 publications
(67 citation statements)
references
References 61 publications
2
62
0
Order By: Relevance
“…where n kσ (0) = [1 + exp ((ε Nkσ − µ N )/k B T )] −1 is the Fermi distribution function for the normal lead electrons. We have solved numerically these coupled differential equations (8)(9)(10)(11)(12)(13)(14)(15)(16)(17) subject to the specific initial conditions. For convenience, we have assumed that till t < 0 both external reservoirs were isolated from the quantum dots.…”
Section: Equations Of Motionmentioning
confidence: 99%
“…where n kσ (0) = [1 + exp ((ε Nkσ − µ N )/k B T )] −1 is the Fermi distribution function for the normal lead electrons. We have solved numerically these coupled differential equations (8)(9)(10)(11)(12)(13)(14)(15)(16)(17) subject to the specific initial conditions. For convenience, we have assumed that till t < 0 both external reservoirs were isolated from the quantum dots.…”
Section: Equations Of Motionmentioning
confidence: 99%
“…Their main effect is to smooth out these phase transitions, which is already observable at typical base temperatures of 𝑇 ≈ 15-50 mK being small against Γ/𝑘 𝐵 (ranging from 0.1-1 meV/k B ≈ 1-10 K). 24,26,87 For instance, this can be appreciated in figure 4(a) showing the total spin quantum number 𝑠 obtained from the thermal average 𝑺 2 POL = ℏ 2 𝑠(𝑠 + 1) over the electronic subsystem. 88 Here, 𝑺 = (ℏ/2) 𝛼𝑠𝑠 𝑑 † 𝛼𝑠 𝝈 𝑠𝑠 𝑑 𝛼𝑠 denotes the spin operator with 𝝈 being the vector of Pauli matrices.…”
Section: Thermal Broadening Of Phase Transitionsmentioning
confidence: 99%
“…[11][12][13][14] The QDs' highly tunable electronic spectra [15][16][17][18] makes them in particular interesting for low-dissipation superconducting spintronics 19,20 and quantum computation. 21,22 Ground-state (GS) transitions in such systems have been observed [23][24][25][26] and discussed in terms of the spin-orbit interaction 27,28 , topological protection, [29][30][31][32][33] and nonequilibrium transport. [34][35][36][37] Remarkably, it was recently demonstrated in carbon nanotube (CNT) quantum dot setups that the electron-phonon interaction can be tailored electrostatically, to even attain attractive electron interaction.…”
Section: Introductionmentioning
confidence: 99%
“…S1. Lever-arm parameter calibration, demonstration of G tunability by the plunger gate, supercurrent enhancement of the linear conductance, and determination of U. References (36)(37)(38)(39)(40)…”
Section: Supplementary Materialsmentioning
confidence: 99%