Abstract:Quantum light–matter interfaces are at the heart of photonic quantum technologies. Quantum memories for photons, where non-classical states of photons are mapped onto stationary matter states and preserved for subsequent retrieval, are technical realizations enabled by exquisite control over interactions between light and matter. The ability of quantum memories to synchronize probabilistic events makes them a key component in quantum repeaters and quantum computation based on linear optics. This critical featu… Show more
“…We consider ensemble-based memories due to their strong light-matter coupling and, in several cases, the possibility of long coherence times (up to seconds [38]) and high bandwidths (up to several GHz [35]). Furthermore, they offer the possibility of multi-mode storage [7,11]. By multi-mode we are referring to memories that can simultaneously store more than one qubit during a single storage event by encoding many qubits each into a different mode.…”
“…There are a variety of systems that have been utilized for optical quantum memories; see [11] for a recent overview. We consider ensemble-based memories due to their strong light-matter coupling and, in several cases, the possibility of long coherence times (up to seconds [38]) and high bandwidths (up to several GHz [35]).…”
“…The former involves many excitations, in which each individual excitation occupies a single distinguishable mode (or a pair as required for a qubit), while the latter concerns many excitations that occupy a single mode and thus each excitation may not be distinguished. Motivated by their impressive, and continually-improving, experimental record, we specifically consider warm vapor (Cs and Rb atomic gas) and cold atom (Rb atoms in a magneto-optical trap or atomic lattice) systems [11] that rely on the so-called Raman quantum memory protocol [60] as well as cryogenicallycooled rare-earth-ion-doped crystals that utilize atomic frequency combs [61].…”
“…Probabilistic quantum repeaters offer a solution to extend the communication distance to over thousands of kilometers [4][5][6][7][8][9][10]. However, such quantum repeaters rely on quantum memory modules [11] with characteristics that are hard to achieve with the current technology. This does not necessarily mean that the existing quantum memories cannot offer any advantages.…”
Section: Introductionmentioning
confidence: 99%
“…Early investigations suggest that quantum memories with large storage-bandwidth products as well as short access and entangling times are necessary for MA-MDI-QKD [13]. These requirements may be achieved by quantum memories based on atomic ensembles [11], with the added benefit of strong light-matter coupling offering the possibility for efficient implementations. Ensemble-based quantum memories may, however, allow for storage of multiple excitations [14], which have been shown to be deleterious to their performance [15].…”
Memory-assisted measurement-device-independent quantum key distribution (MA-MDI-QKD) has recently been proposed as a technique to improve the rate-versus-distance behavior of QKD systems by using existing, or nearly-achievable, quantum technologies. The promise is that MA-MDI-QKD would require less demanding quantum memories than the ones needed for probabilistic quantum repeaters. Nevertheless, early investigations suggest that, in order to beat the conventional memoryless QKD schemes, the quantum memories used in the MA-MDI-QKD protocols must have high bandwidth-storage products and short interaction times. Among different types of quantum memories, ensemble-based memories offer some of the required specifications, but they typically suffer from multiple excitation effects. To avoid the latter issue, in this paper, we propose two new variants of MA-MDI-QKD both relying on single-photon sources for entangling purposes. One is based on known techniques for entanglement distribution in quantum repeaters. This scheme turns out to offer no advantage even if one uses ideal single-photon sources. By finding the root cause of the problem, we then propose another setup, which can outperform single memory-less setups even if we allow for some imperfections in our single-photon sources. For such a scheme, we compare the key rate for different types of ensemble-based memories and show that certain classes of atomic ensembles can improve the rate-versus-distance behavior.
“…We consider ensemble-based memories due to their strong light-matter coupling and, in several cases, the possibility of long coherence times (up to seconds [38]) and high bandwidths (up to several GHz [35]). Furthermore, they offer the possibility of multi-mode storage [7,11]. By multi-mode we are referring to memories that can simultaneously store more than one qubit during a single storage event by encoding many qubits each into a different mode.…”
“…There are a variety of systems that have been utilized for optical quantum memories; see [11] for a recent overview. We consider ensemble-based memories due to their strong light-matter coupling and, in several cases, the possibility of long coherence times (up to seconds [38]) and high bandwidths (up to several GHz [35]).…”
“…The former involves many excitations, in which each individual excitation occupies a single distinguishable mode (or a pair as required for a qubit), while the latter concerns many excitations that occupy a single mode and thus each excitation may not be distinguished. Motivated by their impressive, and continually-improving, experimental record, we specifically consider warm vapor (Cs and Rb atomic gas) and cold atom (Rb atoms in a magneto-optical trap or atomic lattice) systems [11] that rely on the so-called Raman quantum memory protocol [60] as well as cryogenicallycooled rare-earth-ion-doped crystals that utilize atomic frequency combs [61].…”
“…Probabilistic quantum repeaters offer a solution to extend the communication distance to over thousands of kilometers [4][5][6][7][8][9][10]. However, such quantum repeaters rely on quantum memory modules [11] with characteristics that are hard to achieve with the current technology. This does not necessarily mean that the existing quantum memories cannot offer any advantages.…”
Section: Introductionmentioning
confidence: 99%
“…Early investigations suggest that quantum memories with large storage-bandwidth products as well as short access and entangling times are necessary for MA-MDI-QKD [13]. These requirements may be achieved by quantum memories based on atomic ensembles [11], with the added benefit of strong light-matter coupling offering the possibility for efficient implementations. Ensemble-based quantum memories may, however, allow for storage of multiple excitations [14], which have been shown to be deleterious to their performance [15].…”
Memory-assisted measurement-device-independent quantum key distribution (MA-MDI-QKD) has recently been proposed as a technique to improve the rate-versus-distance behavior of QKD systems by using existing, or nearly-achievable, quantum technologies. The promise is that MA-MDI-QKD would require less demanding quantum memories than the ones needed for probabilistic quantum repeaters. Nevertheless, early investigations suggest that, in order to beat the conventional memoryless QKD schemes, the quantum memories used in the MA-MDI-QKD protocols must have high bandwidth-storage products and short interaction times. Among different types of quantum memories, ensemble-based memories offer some of the required specifications, but they typically suffer from multiple excitation effects. To avoid the latter issue, in this paper, we propose two new variants of MA-MDI-QKD both relying on single-photon sources for entangling purposes. One is based on known techniques for entanglement distribution in quantum repeaters. This scheme turns out to offer no advantage even if one uses ideal single-photon sources. By finding the root cause of the problem, we then propose another setup, which can outperform single memory-less setups even if we allow for some imperfections in our single-photon sources. For such a scheme, we compare the key rate for different types of ensemble-based memories and show that certain classes of atomic ensembles can improve the rate-versus-distance behavior.
Herein, it is demonstrated that ultrashort spatially structured beams can sculpt a sample of gas‐phase molecules like a 4D material to produce a spatial pattern of aligned molecules whose shape and temporal evolution allow to restore the spatial light information on a time‐delayed reading pulse. To do so, the spatial phase and amplitude information of ultrashort light beams are encoded into rotational coherences of molecules by exploiting the interplay between spin angular momentum and orbital angular momentum. The field‐free molecular alignment resulting from the interaction leads to an inhomogeneous spatial structuring of the sample allowing to transfer the encoded information into a time‐delayed probe beam. The demonstration is conducted in molecules. Besides applications in terms of THz bandwidth buffer memory, the strategy features interesting prospects for establishing versatile optical processing of orbital angular momentum (OAM) fields, for studying various molecular processes, or for designing new photonic devices enabling to impart superpositions of OAM modes to light beams.
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