Generation ofSU(1, 1) andSU(2) entangled states in a quantized cavity field by strong-driving-assisted classical field approach

Laser Physics ◽  
2015 ◽  
Vol 25 (5) ◽  
pp. 055203 ◽  
Author(s):  
R N Daneshmand ◽  
M K Tavassoly
2021 ◽  
Author(s):  
eied khalil ◽  
S. Abdel-Khalek ◽  
M.Y. Abd-Rabbou ◽  
Mohamed Omri ◽  
Maged Faihan Alotibi

2014 ◽  
Vol 112 (11) ◽  
Author(s):  
Justin Dressel ◽  
Konstantin Y. Bliokh ◽  
Franco Nori

Author(s):  
Alyssa Ney

In quantum mechanics, entangled states are not exotic or rare. Rather, entanglement is the norm and so the metaphysical consequences of entanglement are a central issue for anyone wishing to provide an ontological interpretation of the various formulations of quantum mechanics. This chapter presents the argument for wave function realism from quantum entanglement, which says that wave function realism is necessary if one wants an ontological interpretation that does not conflate distinct quantum states. It explains quantum entanglement and how postulating a wave function in higher dimensions can help to metaphysically ground the phenomenon. The chapter ultimately concludes that the argument from quantum entanglement fails as there are several rival positions that can also explain quantum entanglement and recover the distinctions between different entangled states. These include the primitive ontology approach, various other holisms, ontic structural realism, spacetime state realism, and the multi-field approach.


2009 ◽  
Vol 07 (08) ◽  
pp. 1459-1467 ◽  
Author(s):  
LIN-LIN XU ◽  
YA-FEI YU ◽  
ZHI-MING ZHANG

In this paper, we present a scheme to prepare the W state and the GHZ state of many atomic ensembles based on the dynamics of the atomic system of a single control atom and an atomic ensemble dispersively coupling with a cavity, where the control atom is illuminated by a highly detuned auxiliary classical field at the same time. The dynamics of the atomic system can be described by an effective Jaynes–Cummings model (JCM) with the atomic ensemble as the bosonic mode. The preparation of the entangled states is deterministic. Because the cavity is always in the vacuum state during the whole evolution process, our scheme is less sensitive to the cavity decay.


2013 ◽  
pp. 191-202 ◽  
Author(s):  
Mirosław Brewczyk ◽  
Mariusz Gajda ◽  
Kazimierz Rzążewski

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