277 research outputs found
Proposal for demonstrating the Hong-Ou-Mandel effect with matter waves
The Hong-Ou-Mandel (HOM) effect is a striking demonstration of destructive
quantum interference between pairs of indistinguishable bosons, realised so far
only with massless photons. Here we propose an experiment which can realise
this effect in the matter-wave regime using pair-correlated atoms produced via
a collision of two Bose-Einstein condensates and subjected to two laser induced
Bragg pulses. We formulate a novel measurement protocol appropriate for the
multimode matter-wave field, which---unlike the typical two-mode optical
case---bypasses the need for repeated measurements under different displacement
settings of the beam-splitter, thus dramatically reducing the number of
experimental runs required to map out the interference visibility. The protocol
can be utilised in related matter-wave schemes; here we focus on condensate
collisions and by simulating the entire experiment we predict a HOM-dip
visibility of ~69%. By being larger than 50%, such a visibility highlights
strong quantum correlations between the atoms and paves the way for a possible
demonstration of a Bell inequality violation with massive particles in a
related Rarity-Tapster setup.Comment: Essentially the same version as v2, except in Nature Communications
style; for Supplementary Information see the source fil
Proposal for a motional-state Bell inequality test with ultracold atoms
We propose and theoretically simulate an experiment for demonstrating a
motional-state Bell inequality violation for pairs of momentum-entangled atoms
produced in Bose-Einstein condensate collisions. The proposal is based on
realizing an atom-optics analog of the Rarity-Tapster optical scheme: it uses
laser-induced Bragg pulses to implement two-particle interferometry on the
underlying Bell-state for two pairs of atomic scattering modes with equal but
opposite momenta. The collision dynamics and the sequence of Bragg pulses are
simulated using the stochastic Bogoliubov approach in the positive-P
representation. We predict values of the Clauser-Horne-Shimony-Holt (CHSH)
parameter up to S~2.5 for experimentally realistic parameter regimes, showing a
strong violation of the CSHS-Bell inequality bounded classically by S<2.Comment: Final published version; 11 pages, 6 figure
Sensitivity to thermal noise of atomic Einstein-Podolsky-Rosen entanglement
We examine the prospect of demonstrating Einstein-Podolsky-Rosen (EPR) entanglement for massive particles using spin-changing collisions in a spinor Bose-Einstein condensate. Such a demonstration has recently been attempted by Gross et al. [Nature (London) 480, 219 (2011)] using a condensate of Rb-87 atoms trapped in an optical lattice potential. For the condensate initially prepared in the (F, m(F)) = (2,0) hyperfine state, with no population in the m(F) = +/- 1 states, we predict a significant suppression of the product of inferred quadrature variances below the Heisenberg uncertainty limit, implying strong EPR entanglement. However, such EPR entanglement is lost when the collisions are initiated in the presence of a small (currently undetectable) thermal population (n) over bar (th) in the m(F) = +/- 1 states. For condensates containing 150-200 atoms, we predict an upper bound of (n) over bar (th) similar or equal to 1 that can be tolerated in this experiment before EPR entanglement is lost
Engineering spin squeezing in a 3D optical lattice with interacting spin-orbit-coupled fermions
One of the most important tasks in modern quantum science is to coherently
control and entangle many-body systems, and to subsequently use these systems
to realize powerful quantum technologies such as quantum-enhanced sensors.
However, many-body entangled states are difficult to prepare and preserve since
internal dynamics and external noise rapidly degrade any useful entanglement.
Here, we introduce a protocol that counterintuitively exploits inhomogeneities,
a typical source of dephasing in a many-body system, in combination with
interactions to generate metrologically useful and robust many-body entangled
states. Motivated by current limitations in state-of-the-art three-dimensional
(3D) optical lattice clocks (OLCs) operating at quantum degeneracy, we use
local interactions in a Hubbard model with spin-orbit coupling to achieve a
spin-locking effect. In addition to prolonging inter-particle spin coherence,
spin-locking transforms the dephasing effect of spin-orbit coupling into a
collective spin-squeezing process that can be further enhanced by applying a
modulated drive. Our protocol is fully compatible with state-of-the-art 3D OLC
interrogation schemes and may be used to improve their sensitivity, which is
currently limited by the intrinsic quantum noise of independent atoms. We
demonstrate that even with realistic experimental imperfections, our protocol
may generate -- dB of spin squeezing in second with
-- atoms. This capability allows OLCs to enter a new era of
quantum enhanced sensing using correlated quantum states of driven
non-equilibrium systems.Comment: 20 pages, 12 figure
Verification of a many-ion simulator of the Dicke model through slow quenches across a phase transition
We use a self-assembled two-dimensional Coulomb crystal of ions in
the presence of an external transverse field to engineer a simulator of the
Dicke Hamiltonian, an iconic model in quantum optics which features a quantum
phase transition between a superradiant/ferromagnetic and a normal/paramagnetic
phase. We experimentally implement slow quenches across the quantum critical
point and benchmark the dynamics and the performance of the simulator through
extensive theory-experiment comparisons which show excellent agreement. The
implementation of the Dicke model in fully controllable trapped ion arrays can
open a path for the generation of highly entangled states useful for enhanced
metrology and the observation of scrambling and quantum chaos in a many-body
system.Comment: 6 + 5 pages, 2 + 5 figures. arXiv admin note: substantial text
overlap with arXiv:1711.0739
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