Generation of a multi-qubit W entangled state through spatially separated semiconductor quantum-dot-molecules in cavity-quantum electrodynamics arrays

2014 ◽  
Vol 115 (13) ◽  
pp. 134312 ◽  
Author(s):  
Siping Liu ◽  
Rong Yu ◽  
Jiahua Li ◽  
Ying Wu
Keyword(s):  
Quantum Dot ◽  
Quantum Electrodynamics ◽  
Cavity Quantum Electrodynamics ◽  
Entangled State ◽  
Semiconductor Quantum Dot ◽  
Quantum Dot Molecules

scholarly journals Quantum Dot Spectroscopy Using Cavity Quantum Electrodynamics

2008 ◽  
Vol 101 (22) ◽  
Author(s):  
Martin Winger ◽  
Antonio Badolato ◽  
Kevin J. Hennessy ◽  
Evelyn L. Hu ◽  
Ataç Imamoğlu
Keyword(s):  
Quantum Dot ◽  
Quantum Electrodynamics ◽  
Cavity Quantum Electrodynamics

scholarly journals IBM Q Experience as a versatile experimental testbed for simulating open quantum systems

2020 ◽  
Vol 6 (1) ◽  
Author(s):  
Guillermo García-Pérez ◽  
Matteo A. C. Rossi ◽  
Sabrina Maniscalco
Keyword(s):  
Quantum Electrodynamics ◽  
Quantum Physics ◽  
Open Quantum Systems ◽  
Cavity Quantum Electrodynamics ◽  
Quantum Systems ◽  
Entangled State ◽  
Specific Class ◽  
Linear Optics ◽  
Open Quantum ◽  
State Generation

AbstractThe advent of noisy intermediate-scale quantum (NISQ) technology is changing rapidly the landscape and modality of research in quantum physics. NISQ devices, such as the IBM Q Experience, have very recently proven their capability as experimental platforms accessible to everyone around the globe. Until now, IBM Q Experience processors have mostly been used for quantum computation and simulation of closed systems. Here, we show that these devices are also able to implement a great variety of paradigmatic open quantum systems models, hence providing a robust and flexible testbed for open quantum systems theory. During the last decade an increasing number of experiments have successfully tackled the task of simulating open quantum systems in different platforms, from linear optics to trapped ions, from nuclear magnetic resonance (NMR) to cavity quantum electrodynamics. Generally, each individual experiment demonstrates a specific open quantum system model, or at most a specific class. Our main result is to prove the great versatility of the IBM Q Experience processors. Indeed, we experimentally implement one and two-qubit open quantum systems, both unital and non-unital dynamics, Markovian and non-Markovian evolutions. Moreover, we realise proof-of-principle reservoir engineering for entangled state generation, demonstrate collisional models, and verify revivals of quantum channel capacity and extractable work, caused by memory effects. All these results are obtained using IBM Q Experience processors publicly available and remotely accessible online.

Magneto-Optical Cavity Quantum Electrodynamics Effects in Quantum Dot Micropillar Systems

2010 ◽  
Author(s):  
Stephan Reitzenstein ◽  
Steffen Munch ◽  
Philipp Franeck ◽  
Arash Rahimi-Iman ◽  
Tobias Heindel ◽  
...  
Keyword(s):  
Quantum Dot ◽  
Quantum Electrodynamics ◽  
Optical Cavity ◽  
Cavity Quantum Electrodynamics

The influence of excitation number of photon-added coherent state field on the entanglement swapping process

2017 ◽  
Vol 31 (27) ◽  
pp. 1750198 ◽  
Author(s):  
M. Soltani ◽  
M. K. Tavassoly ◽  
R. Pakniat
Keyword(s):  
Coherent State ◽  
Quantum Electrodynamics ◽  
Coherent States ◽  
Success Probability ◽  
Entanglement Swapping ◽  
Cavity Quantum Electrodynamics ◽  
Linear Entropy ◽  
Entangled State ◽  
Maximally Entangled State ◽  
Coherent Field

In this paper, we outline a scheme for the entanglement swapping procedure based on cavity quantum electrodynamics using the Jaynes–Cummings model consisting of the coherent and photon-added coherent states. In particular, utilizing the photon-added coherent states ([Formula: see text][Formula: see text][Formula: see text][Formula: see text], where [Formula: see text] is the Glauber coherent state) in the scheme, enables us to investigate the effect of [Formula: see text], i.e., the number of excitations corresponding to the photon-added coherent field on the entanglement swapping process. In the scheme, two two-level atoms [Formula: see text] and [Formula: see text] are initially entangled together, and distinctly two exploited cavity fields [Formula: see text] and [Formula: see text] are prepared in an entangled state (a combination of coherent and photon-added coherent states). Interacting the atom [Formula: see text] with field [Formula: see text] (via the Jaynes–Cummings model) and then making detection on them, transfers the entanglement from the two atoms [Formula: see text], [Formula: see text] and the two fields [Formula: see text], [Formula: see text] to the atom-field “[Formula: see text]-[Formula: see text]”, i.e., entanglement swapping occurs. In the continuation, we pay our attention to the evaluation of the fidelity of the swapped entangled state relative to a suitable maximally entangled state, success probability of the performed detections and linear entropy as the degree of entanglement of the swapped entangled state. It is demonstrated that, an increase in the number of excitations, [Formula: see text], leads to the increment of fidelity as well as the amount of entanglement. According to our numerical results, the maximum values of fidelity (linear entropy) 0.98 (0.46) is obtained for [Formula: see text], however, the maximum value of success probability does not significantly change by increasing [Formula: see text].

Cavity Quantum Electrodynamics in Quantum Dot-Photonic Crystal Nanocavity Coupled System with Large g/κ

CLEO: 2014 ◽  
2014 ◽  
Author(s):  
Satoshi Iwamoto ◽  
Yasutomo Ota ◽  
Hiroyuki Takagi ◽  
Daisaku Takamiya ◽  
Yasuhiko Arakawa
Keyword(s):  
Photonic Crystal ◽  
Quantum Dot ◽  
Quantum Electrodynamics ◽  
Coupled System ◽  
Cavity Quantum Electrodynamics
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