2020
DOI: 10.1039/d0cp03945d
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Spin-momentum entanglement in a Bose–Einstein condensate

Abstract: Entanglement is at the core of quantum information processing and may prove essential for quantum speed-up. Inspired by both theoretical and experimental studies of spin-momentum coupling in systems of ultra-cold...

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Cited by 3 publications
(3 citation statements)
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“…This process induces, in addition, a change in the momentum of the atom by 2 k r , where k r is the photon recoil momentum. , Thus, the atoms are dressed into a superposition of hyperfine spin and mechanical momenta. In our previous work, we analyzed the spin–orbit coupling in the BECs that realize a pair of qutrits. The Hamiltonian , that describes such a spin ( m f )momentum ( K ) coupling can be written in the coupled basis | m f , K ⟩ = {|−1, q + 2 K r ⟩, |0, q ⟩, |+1, q – 2 k r ⟩} as Here, m is the mass of 87 Rb, q is the quasi-momentum (usually at the minimum of the BEC’s lowest energy band), Ω r is the strength of the Raman coupling (which determines the Rabi frequency for the Raman transition between two hyperfine m f states), δ­( B ) is the detuning of the Raman laser, ϵ­( B ) = 0.65 E r is the quadratic Zeeman shift (at | B ⃗ bias | ≈ 5 G ), E r = ℏ k r 2 /2 m is the recoil energy, and B is the strength of the external magnetic field.…”
Section: Using Raman Coupling To Achieve Superpositionmentioning
confidence: 99%
See 1 more Smart Citation
“…This process induces, in addition, a change in the momentum of the atom by 2 k r , where k r is the photon recoil momentum. , Thus, the atoms are dressed into a superposition of hyperfine spin and mechanical momenta. In our previous work, we analyzed the spin–orbit coupling in the BECs that realize a pair of qutrits. The Hamiltonian , that describes such a spin ( m f )momentum ( K ) coupling can be written in the coupled basis | m f , K ⟩ = {|−1, q + 2 K r ⟩, |0, q ⟩, |+1, q – 2 k r ⟩} as Here, m is the mass of 87 Rb, q is the quasi-momentum (usually at the minimum of the BEC’s lowest energy band), Ω r is the strength of the Raman coupling (which determines the Rabi frequency for the Raman transition between two hyperfine m f states), δ­( B ) is the detuning of the Raman laser, ϵ­( B ) = 0.65 E r is the quadratic Zeeman shift (at | B ⃗ bias | ≈ 5 G ), E r = ℏ k r 2 /2 m is the recoil energy, and B is the strength of the external magnetic field.…”
Section: Using Raman Coupling To Achieve Superpositionmentioning
confidence: 99%
“…12,13 Thus, the atoms are dressed into a superposition of hyperfine spin and mechanical momenta. In our previous work, 14 we analyzed the spin−orbit coupling in the BECs that realize a pair of qutrits. The Hamiltonian 12,13 that describes such a spin (m f )momentum (K) coupling can be written in the coupled basis |m f , K⟩ = {|−1, q + 2K r ⟩, |0, q⟩, | +1, q − 2k r ⟩} as i k j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j j y { z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z z…”
mentioning
confidence: 99%
“…This article focuses on achieving the ground state of Kagome lattices using a variational quantum eigensolver (VQE). Such quantum simulations, variational and otherwise, have become quite popular in recent years and been performed for a variety of other systems using diverse methodologies. However, even constructing the ground state of a single plaquette within the Kagome lattice requires 12 qubits. Various studies , have demonstrated that when attempting to attain the ground state of Hamiltonians with a significant number of qubits (>8), any Hamiltonian-agnostic ansatz, beyond a certain depth, inevitably leads to a barren plateau.…”
Section: Introductionmentioning
confidence: 99%