2016
DOI: 10.1103/physreva.94.012307
|View full text |Cite
|
Sign up to set email alerts
|

Single-shot optical readout of a quantum bit using cavity quantum electrodynamics

Abstract: We propose a method to perform single-shot optical readout of a quantum bit (qubit) using cavity quantum electrodynamics. We selectively couple the optical transitions associated with different qubit basis states to the cavity, and utilize the change in cavity transmissivity to generate a qubit readout signal composed of many photons. We show that this approach enables single-shot optical readout even when the qubit does not have a good cycling transition that is required for standard resonance fluorescence me… 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
21
0

Year Published

2016
2016
2023
2023

Publication Types

Select...
7
2

Relationship

2
7

Authors

Journals

citations
Cited by 25 publications
(21 citation statements)
references
References 68 publications
0
21
0
Order By: Relevance
“…Integration of these defects into cavities should improve readout by increasing the collection efficiency and by Purcell enhancement of the radiative transitions relative to the ISC. Cavity enhancement of different optical transitions in semiconductor QDs has been successful in improving the fidelity of both readout and initialization [45][46][47].…”
Section: Discussionmentioning
confidence: 99%
“…Integration of these defects into cavities should improve readout by increasing the collection efficiency and by Purcell enhancement of the radiative transitions relative to the ISC. Cavity enhancement of different optical transitions in semiconductor QDs has been successful in improving the fidelity of both readout and initialization [45][46][47].…”
Section: Discussionmentioning
confidence: 99%
“…Let us assume our initial state is predetermined and restricted to the { 0 m s ñ | and 1 m s + ñ | } subspace, but that the fidelity decays exponentially in the number of photon pulses. The probability of each state after n pulses is then given by Bayes' theorem and a binomial distribution (similar to the treatment of a Poisson-distribution in [122]). The probability of a detection event from 0 m s ñ | and 1 m s + ñ | will be p 0 and p 1 + respectively.…”
Section: Single Photon Pulsesmentioning
confidence: 99%
“…Recently an alternative approach based on dipole-induced transparency has been proposed [118][119][120][121][122] wherein the state of the NV center changes the resonance properties of an optical cavity. More specifically, if the electronic spin in its 0 m s ñ | state, an incident photon is reflected from the cavity, while for the 1 m s + ñ | electronic spin state the photon enters the cavity where it is scattered but not absorbed by the NV center.…”
Section: Introductionmentioning
confidence: 99%
“…Many confined spin systems such as quantum dot spins 16 , fluorine impurities 17 , and silicon-vacancy centers in diamond 18,19 , do not possess a good branching ratio due to non-radiative decay mechanisms or poor selection rules. In addition, the external magnetic field direction to achieve optimal branching ratio for these confined spin systems typically conflict with the condition that allows coherent optical spin manipulations 20- 23 . These qubit systems therefore require new methods for readout.…”
Section: Introductionmentioning
confidence: 99%