Teleportation of squeezed states in the absence and presence of dissipation
arXiv:2105.13757 · doi:10.1140/epjp/i2019-12907-4
Abstract
In this paper at first we successfully teleport the unknown quantum state which is a superposition of squeezed vacuum state and squeezed one-photon state using the beam splitter in the absence of dissipation. In the continuation, we try to implement the same teleportation protocol, however, in the presence of dissipation effects. To do this task, we use proper entangled channel to reach to perfect teleportation under the in uence of decoherence. Finally, we consider another superposition of two squeezed vacuum states with separation in phase and teleport it with a different appropriate entangled channel. In fact, we will observe that, one can successfully teleport the considered superposition of squeezed states by choosing proper entangled channels in the presence and absence of dissipation in appropriate chosen conditions.
References in corpus (8)
- Experimental quantum teleportation
- Quantum Teleportation Between Distant Matter Qubits
- GHZ-type and W-type entangled coherent states: generation and Bell-type inequality tests without photon counting
- Dissipative entanglement swapping in the presence of detuning and Kerr medium: Bell state measurement method
- Entanglement properties of optical coherent states under amplitude damping
- Quantum repeater protocol in mixed single- and two-mode Tavis-Cummings models
- Dissipative quantum repeater
- Quantum repeater using three-level atomic states in the presence of dissipation: stability of entanglement