2007
DOI: 10.1140/epjb/e2007-00035-5
|View full text |Cite
|
Sign up to set email alerts
|

Double SQUID tunable flux qubit manipulated by fast pulses: operation requirements, dissipation and decoherence

Abstract: A double SQUID manipulated by fast magnetic flux pulses can be used as a tunable flux qubit. In this paper we study the requirements for the qubit operation, and evaluate dissipation and decoherence due to the manipulation for a typical system. Furthermore, we discuss the possibility to use an integrated Rapid Single Flux Quantum logic for the qubit control.

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1

Citation Types

1
13
0

Year Published

2007
2007
2022
2022

Publication Types

Select...
9

Relationship

2
7

Authors

Journals

citations
Cited by 12 publications
(14 citation statements)
references
References 29 publications
1
13
0
Order By: Relevance
“…The potential has been used to implement an Otto cycle, enabled by energy quantization and operating by adiabatic insertion and removal of the barrier. A possible candidate to realize our model of the quantum Stirling engine involves superconducting flux qubits where the symmetric potential can be controlled at very low temperatures [46,47] with well defined heat baths and the possibility of measurement of heat power [48].…”
Section: Discussionmentioning
confidence: 99%
“…The potential has been used to implement an Otto cycle, enabled by energy quantization and operating by adiabatic insertion and removal of the barrier. A possible candidate to realize our model of the quantum Stirling engine involves superconducting flux qubits where the symmetric potential can be controlled at very low temperatures [46,47] with well defined heat baths and the possibility of measurement of heat power [48].…”
Section: Discussionmentioning
confidence: 99%
“…The device we consider is the so-called double SQUID [31], consisting of a superconducting loop of inductance L interrupted by a dc SQUID, a second smaller superconducting loop of inductance l interrupted by two identical Josephson junctions, each of (nominally) identical critical current i 0 and capacitance c [ Fig. 1(a) , being 0 = h/2e the flux quantum), which is controlled by a magnetic flux c applied to the small loop (this approximation holds if the loop is small enough, i.e., for li 0 0 ).…”
Section: Double Squidmentioning
confidence: 99%
“…In our case it is E C / h = 0.22 GHz, E L / h = 1920 GHz and E J / h = 7940 GHz leading to β 0 = 4.1. Depending on the value of β(ϕ c ), the potential U (ϕ) has a single-well or a double-well shape, with ϕ c controlling the barrier height in the double well (figure 1(b)) and the concavity in the single-well case (figures 1(c) and (d)), and ϕ x controlling the potential symmetry (figure 1(e)) [23,24]. The described potential presents a periodic behaviour in x and c [20].…”
Section: The Double Squid Qubit Manipulated By Fast Pulsesmentioning
confidence: 99%
“…The energy gaphε = E L ϕ ϕ x between them is almost constant in a large range of values of β(ϕ c ) because of the weak dependence of ϕ on β(ϕ c ). Approximate analytical expressions for the important quantities related to this case have been reported in [24].…”
Section: The Double Squid Qubit Manipulated By Fast Pulsesmentioning
confidence: 99%