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Frontiers in Optics

Efficient THz-bandwidth Quantum Memory in Atomic Barium

Kai Shinbrough, B. D. Hunt, Sehyun Park, Kathleen Oolman, J. Gary Eden, Virginia O. Lorenz

Published Jan 1, 2022• 0 citations
Publisher

Abstract

We report record storage efficiencies in the first atomic THz-bandwidth quantum memory. Near-off-resonant orbital transitions in collisionally broadened hot atomic barium vapor allow for 83% storage efficiency, 25% total efficiency, and a time-bandwidth-product of 800.
DOI
10.1364/fio.2022.fth3c.7

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Optical quantum memory describes the process of on-demand storage and retrieval of single photon-level quantum states, and is a critical enabling technology for many quantum applications. Memory bandwidth plays an important role in these applications, as it determines the pulse durations compatible with the memory and places an upper bound on the clock rate and processing speed of a quantum device. Here we present experimental results of an atomic barium quantum memory that enables storage and retrieval of ultra-broadband(>800(> 800(>800GHz) signal photons with high storage efficiency [95.6(3)%] and low noise [3.8(6)×10−5\times 10^{-5}×10−5noise photons]. Experimental Results.- The quantum memory operation is based on the ground(6s2 1S0)(6s^{2}\ {}^{1}S_{0})(6s2 1S0​), excited(6s6p 1P1)(6s6p \ {}^{1}P_{1})(6s6p 1P1​), and metastable(6s5d 1D2)(6s5d \ {}^{1}D_{2})(6s5d 1D2​)orbital states of atomic barium in aΛ\LambdaΛ-type configuration. The barium vapor is created in an 800–900 °C barium heat pipe oven with 0–1000 torr tunable argon buffer gas pressure. The ground-excited transition at 553.5 nm features large and tunable homogeneous collisional broadening due to the argon buffer gas and a peak optical depth ofd=50d=50d=50. The memory operates in the so-called absorb-then-transfer (ATT) regime, in which the signal field is linearly absorbed along the ground-excited transition, whose collisionally broadened lineshape enables efficient absorption of ultra-broadband photons; the resulting atomic polarization is transferred into a so-called spin wave by application of a strong[O(10 uJ),100 fs][O(10 \ \text{uJ}),100\ \text{fs}][O(10 uJ),100 fs]control pulse along the excited-metastable transition at 1500 nm. The storage state has a 0(0.1) second coherence lifetime in the bare atom [1], but this is reduced to theO(ns)O(\text{ns})O(ns)level due to motional dephasing [0.49(1) ns measured memory lifetime]. The memory experiment is repeated at a repetition rate of 1 kHz. The total end-to-end efficiency of the memory at 900°C is 31(1)%, which is limited by available control field power.
We present a demonstration of simultaneous high-efficiency, high-speed, and low-noise operation of a photonic quantum memory. By leveraging controllable collisional dephasing in a neutral barium atomic vapor, we demonstrate a significant improvement in memory efficiency and bandwidth over existing techniques. We achieve greater than 95% storage efficiency and 26% total efficiency of 880 GHz bandwidth photons, with O(10−5)\mathcal{O}(10^{-5})O(10−5) noise photons per retrieved pulse. These ultrabroad bandwidths enable rapid quantum information processing and contribute to the development of practical quantum memories with potential applications in quantum communication, computation, and networking.
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