12 research outputs found
Multiplexed on-demand storage of polarization qubits in a crystal
A long-lived and multimode quantum memory is a key component needed for the
development of quantum communication. Here we present temporally multiplexed
storage of 5 photonic polarization qubits encoded onto weak coherent states in
a rare-earth-ion doped crystal. Using spin refocusing techniques we can
preserve the qubits for more than half a millisecond. The temporal multiplexing
allows us to increase the effective rate of the experiment by a factor of 5,
which emphasizes the importance of multimode storage for quantum communication.
The fidelity upon retrieval is higher than the maximum classical fidelity
achievable with qubits encoded onto single photons and we show that the memory
fidelity is mainly limited by the memory signal-to-noise ratio. These results
show the viability and versatility of long-lived, multimode quantum memories
based on rare-earth-ion doped crystals
Cavity-enhanced storage in an optical spin-wave memory
We report on the experimental demonstration of an optical spin-wave memory,
based on the atomic frequency comb (AFC) scheme, where the storage efficiency
is strongly enhanced by an optical cavity. The cavity is of low finesse, but
operated in an impedance matching regime to achieve high absorption in our
intrinsically low-absorbing Eu3+:Y2SiO5 crystal. For storage of optical pulses
as an optical excitation (AFC echoes), we reach efficiencies of 53% and 28% for
2 and 10 microseconds delays, respectively. For a complete AFC spin-wave memory
we reach an efficiency of 12%, including spin-wave dephasing, which is a
12-fold increase with respect to previous results in this material. This result
is an important step towards the goal of making efficient and long-lived
quantum memories based on spin waves, in the context of quantum repeaters and
quantum networks
Coherent spin control at the quantum level in an ensemble-based optical memory
Long-lived quantum memories are essential components of a long-standing goal
of remote distribution of entanglement in quantum networks. These can be
realized by storing the quantum states of light as single-spin excitations in
atomic ensembles. However, spin states are often subjected to different
dephasing processes that limit the storage time, which in principle could be
overcome using spin-echo techniques. Theoretical studies have suggested this to
be challenging due to unavoidable spontaneous emission noise in ensemble-based
quantum memories. Here we demonstrate spin-echo manipulation of a mean spin
excitation of 1 in a large solid-state ensemble, generated through storage of a
weak optical pulse. After a storage time of about 1 ms we optically read out
the spin excitation with a high signal-to-noise ratio. Our results pave the way
for long-duration optical quantum storage using spin-echo techniques for any
ensemble-based memory.Comment: 5 pages, 2 figures, 1 tabl
Towards highly multimode optical quantum memory for quantum repeaters
Long-distance quantum communication through optical fibers is currently
limited to a few hundreds of kilometres due to fiber losses. Quantum repeaters
could extend this limit to continental distances. Most approaches to quantum
repeaters require highly multimode quantum memories in order to reach high
communication rates. The atomic frequency comb memory scheme can in principle
achieve high temporal multimode storage, without sacrificing memory efficiency.
However, previous demonstrations have been hampered by the difficulty of
creating high-resolution atomic combs, which reduces the efficiency for
multimode storage. In this article we present a comb preparation method that
allows one to increase the multimode capacity for a fixed memory bandwidth. We
apply the method to a Eu-doped YSiO crystal, in which we
demonstrate storage of 100 modes for 51 s using the AFC echo scheme (a
delay-line memory), and storage of 50 modes for 0.541 ms using the AFC
spin-wave memory (an on-demand memory). We also briefly discuss the ultimate
multimode limit imposed by the optical decoherence rate, for a fixed memory
bandwidth.Comment: 10 pages, 8 figure
Optically probing the detection mechanism in a molybdenum silicide superconducting nanowire single-photon detector
We experimentally investigate the detection mechanism in a meandered molybdenum silicide superconducting nanowire single-photon detector by characterising the detection probability as a function of bias current in the wavelength range of 750–2050 Onm. Contrary to some previous observations on niobium nitride or tungsten silicide detectors, we find that the energy-current relation is nonlinear in this range. Furthermore, thanks to the presence of a saturated detection efficiency over the whole range of wavelengths, we precisely quantify the shape of the curves. This allows a detailed study of their features, which are indicative of both Fano fluctuations and position-dependent effects
Spectroscopic investigations of Eu<sup>3+</sup>:Y<sub>2</sub>SiO<sub>5</sub> for quantum memory applications
Rare-earth-ion-doped solids are promising materials as light-matter interfaces for quantum applications. Europium doped into an yttrium orthosilicate crystal in particular has interesting coherence properties and a suitable ground-state energy-level structure for a quantum memory for light. In this paper we report on spectroscopic investigations of this material from the perspective of implementing an atomic frequency comb (AFC)-type quantum memory with spin-wave storage. For this goal we determine the order of the hyperfine levels in the 7 F0 ground state and 5 D0 excited state, and we measure the relative strengths of the optical transitions between these levels. We also apply spectral hole burning techniques in order to prepare the system as a well-defined Λ system, as required for further quantum memory experiments. Furthermore, we measure the optical Rabi frequency on one of the strongest hyperfine transitions, a crucial experimental parameter for the AFC protocol. From this we also obtain a value for the transition dipole moment which is consistent with that obtained from absorption measurements