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Enhancement of magnon-photon-phonon entanglement in a cavity magnomechanics with coherent feedback loop
Quantum Physics · Submitted 30 Nov 2022
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the entanglement can be significantly improved with coherent feedback using a suitable tuning of the reflective parameter of the beam splitter.
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The abstract, sentence by sentence
We propose a scheme to improve magnon-photon-phonon entanglement in cavity magnomechanics using coherent feedback loop. In addition, we prove that the steady state and dynamical state of the system is a genuine tripartite entanglement state. We use the logarithmic negativity as the witness of quantum correlations to quantify the entanglement of all bipartite subsystem, and genuine tripartite entanglement via the nonzero minimum residual contangle, in steady and dynamical regime. We consider the feasible experiment parameters to realize the tripartite entanglement. We show that the entanglement can be significantly improved with coherent feedback using a suitable tuning of the reflective parameter of the beam splitter. The entanglement is robust against the thermal effects. Our proposal scheme to improve the entanglement can be of interest to applications in quantum information.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We propose a scheme to improve magnon-photon-phonon entanglement in cavity magnomechanics using coherent feedback loop. | contribution 1.00 | 0.69 | 0.28 | asserted 0.42 |
| s1 | In addition, we prove that the steady state and dynamical state of the system is a genuine tripartite entanglement state. | result 0.96 | 0.94 | 0.30 | asserted 1.00 |
| s2 | We use the logarithmic negativity as the witness of quantum correlations to quantify the entanglement of all bipartite subsystem, and genuine tripartite entanglement via the nonzero minimum residual contangle, in steady and dynamical regime. | method 0.99 | 0.92 | 0.12 | asserted 0.97 |
| s3 | We consider the feasible experiment parameters to realize the tripartite entanglement. | method 0.53 | 0.83 | 0.04 | asserted 0.70 |
| s4 | We show that the entanglement can be significantly improved with coherent feedback using a suitable tuning of the reflective parameter of the beam splitter. | result 0.99 | 0.93 | 0.59 | asserted 1.00 |
| s5 | The entanglement is robust against the thermal effects. | result 0.99 | 0.87 | 0.09 | asserted 1.00 |
| s6 | Our proposal scheme to improve the entanglement can be of interest to applications in quantum information. | interpretation 0.86 | 0.20 | 0.11 | hedged possibility 0.97 |
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The paper
Original abstract
We propose a scheme to improve magnon-photon-phonon entanglement in cavity magnomechanics using coherent feedback loop. In addition, we prove that the steady state and dynamical state of the system is a genuine tripartite entanglement state. We use the logarithmic negativity as the witness of quantum correlations to quantify the entanglement of all bipartite subsystem, and genuine tripartite entanglement via the nonzero minimum residual contangle, in steady and dynamical regime. We consider the feasible experiment parameters to realize the tripartite entanglement. We show that the entanglement can be significantly improved with coherent feedback using a suitable tuning of the reflective parameter of the beam splitter. The entanglement is robust against the thermal effects. Our proposal scheme to improve the entanglement can be of interest to applications in quantum information.
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How the literature uses it
2 arXiv papers cite this in 12 sentences
Papers citing it · 9 sentences without a confident label
Uses its data or values 1 paper
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In this section, we show the results and discuss the evolution of quantum correlations of the system by considering experimentally accessible parameters reported in [ref] : $ω_a/2π= 10$ GHz, $ω_m/2π= 10$ MHz , $γ_m/2π= 100$ Hz, $γ_a/2π= γ_b/2π= 1$ MHz, $g_Ga/2π= G_Gb/2π=3.2$ MHz, and at low temperature $T = 10$ mK. $G_Gb = 2π×3.2$ MHz implies the drive magnetic field $B_0 ≈3.9×10^-5$ T for $g_Ga≈2π×0.2$ Hz, corresponding to the drive power $P =8.9$ mW.
Coherent feedback control of quantum correlations in cavity magnomechanical system with magnon squeezing · Results and Discusion · 1.00
Compares with it 1 paper
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We observe, that the entanglement is very strong ($E_ab>1.3$, $E_bm>0.8$ and $E_am>1.3$) in comprising with the results in Ref. [ref] .
Coherent feedback control of quantum correlations in cavity magnomechanical system with magnon squeezing · Results and Discusion · 1.00
What it cites
Cites as background 3 papers
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Magnon squeezing enhanced ground-state cooling in cavity magnomechanics [ref] .
Magnon squeezing enhanced ground-state cooling in cavity magnomechanics · Introduction · 0.89
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Recently, cavity magnomechanics offers a robust platform where ferrimagnetic cristal (e.g., yttrium iron garnet (YIG) sphere) is coupled with a microwave cavity [ref] .
Quantum magnonics: when magnon spintronics meets quantum information science · Introduction · 0.91
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Cooling the mechanical mode to their quantum ground states [ref] , photon blockade [ref] , generating mechanical quantum superposition states [ref] , enhancing precision measurements [ref] , gravitational-wave detectors [ref] and optomechanically induced transpency [ref] .
Strong photon antibunching effect in a double cavity optomechanical system with intracavity squeezed light · Introduction · 0.90
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