2019
DOI: 10.1063/1.5082894
|View full text |Cite
|
Sign up to set email alerts
|

Low-temperature tunable radio-frequency resonator for sensitive dispersive readout of nanoelectronic devices

Abstract: We present a sensitive, tunable radio-frequency resonator designed to detect reactive changes in nanoelectronic devices down to dilution refrigerator temperatures. The resonator incorporates GaAs varicap diodes to allow electrical tuning of the resonant frequency and the coupling to the input line. We find a resonant frequency tuning range of 8.4 MHz at 55 mK that increases to 29 MHz at 1.5 K. To assess the impact on performance of different tuning conditions, we connect a quantum dot in a silicon nanowire fie… Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
1
1
1
1

Citation Types

0
18
0

Year Published

2020
2020
2024
2024

Publication Types

Select...
5
1
1

Relationship

2
5

Authors

Journals

citations
Cited by 17 publications
(18 citation statements)
references
References 30 publications
0
18
0
Order By: Relevance
“…From the fit and our experimentally measured inductance value L = 47 nH [34], we deduce a total parasitic capacitance C p = 150 fF, a characteristic impedance Z r = L/C p = 560 Ω, an internal (external) decay rate κ int /(2π) = 1.31 MHz (κ ext /(2π) = 1.76 MHz) and a total photon decay rate of κ/(2π) = 3.07 MHz. Moreover, we plot the phase shift φ across the resonance (blue trace) and observe a 2π phase shift confirming that photons predominantly escape the resonator before decaying [35].…”
Section: Architecturementioning
confidence: 59%
“…From the fit and our experimentally measured inductance value L = 47 nH [34], we deduce a total parasitic capacitance C p = 150 fF, a characteristic impedance Z r = L/C p = 560 Ω, an internal (external) decay rate κ int /(2π) = 1.31 MHz (κ ext /(2π) = 1.76 MHz) and a total photon decay rate of κ/(2π) = 3.07 MHz. Moreover, we plot the phase shift φ across the resonance (blue trace) and observe a 2π phase shift confirming that photons predominantly escape the resonator before decaying [35].…”
Section: Architecturementioning
confidence: 59%
“…However, the measurement bandwidth of these devices typically has a high-frequency cut-off of less than 100 kHz due to the time constant of the cryogenic wiring and to the limited bandwidth of the current-to-voltage converter. To overcome these limitations, radio-frequency (rf) SET reflectometry was developed [ 47 , 48 , 49 , 50 , 51 , 52 ]. Fast and high-fidelity readout of the DQD is obtained by incorporating the charge sensor into an impedance matching tank circuit: changes to the electrostatic potential of the charge sensor alter its conductance and therefore generate measurable changes to the reflection coefficient of the circuit ( Figure 4 ).…”
Section: Dqd Broadband Microwave Photon Detectorsmentioning
confidence: 99%
“…When g < 1(g > 1), one operates in an undercoupled (overcoupled) regime where more (less) power is dissipated in the resonator than in the external circuits. To operate close to perfect matching, one needs to tweak the coupling capacitor C c , so that g ∼ 1 [84].…”
Section: Operating Close To Perfect Matchingmentioning
confidence: 99%