Fast, noise-free memory for photon synchronization at room temperature

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Presentation transcript:

Fast, noise-free memory for photon synchronization at room temperature by Ran Finkelstein, Eilon Poem, Ohad Michel, Ohr Lahad, and Ofer Firstenberg Science Volume 4(1):eaap8598 January 12, 2018 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 1 FLAME scheme. FLAME scheme. (A) A ladder-level structure comprising purely orbital transitions (the surface colors display the phase structure of the orbitals 5s, 5p, and 5d) is achieved by optical pumping (purple) of the nuclear and electronic spins (green arrows) to the maximally polarized state. Nonzero detuning Δ from the intermediate level can be introduced. (B) To keep the ladder within the maximally polarized subspace, the counter-propagating signal and control beams are circularly polarized using quarter-wave plates (QWP; polarizations shown by green arrows). The collimated optical pump beams enter the cell at a small angular deviation. After storage and retrieval, a polarizing beam-splitter (PBS) picks out the signal. Scattered control light and spontaneous emission are filtered out spectrally by laser-line (LL) filters and spatially by a single-mode fiber coupled to the photodetector. (C) The parameters governing the synchronization capability of the memory are pulse duration τp, memory lifetime τs, retrieval efficiency η, and noise ν. Ran Finkelstein et al. Sci Adv 2018;4:eaap8598 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 2 FLAME operation for different storage times t, off resonance (left) and on resonance (right). FLAME operation for different storage times t, off resonance (left) and on resonance (right). (A and D) Typical pulse sequence, presented for t = 40 ns. The incoming pulse is shown for reference. (B and E) Traces from the single-photon counter for different storage times (colors). The blackened areas mark the portion of the leaked signal. (C and F) Decay of memory efficiency with t. Continuous optical pumping [yellow symbols in (C)] demonstrates the vanishing of beating for a fully polarized ensemble (while introducing more noise). Gray area in (F) marks the delay of the signal because of the reduced group velocity while the control pulse is on. Ran Finkelstein et al. Sci Adv 2018;4:eaap8598 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 3 Efficiency and noise dependence on control power (bottom axis) or control Rabi frequency Ω (top axis). Efficiency and noise dependence on control power (bottom axis) or control Rabi frequency Ω (top axis). (A) Memory efficiency for t = 40 ns. (B) Total photons in the collection window absent an incoming signal (shaded areas are 1σ statistical uncertainty). Note that the collection window is larger by 45% in the Δ = 0 case (for accommodating the wider retrieved signal). The arrows mark the operating powers of Fig. 2. Ran Finkelstein et al. Sci Adv 2018;4:eaap8598 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 4 Projected performance of reported quantum memories for synchronizing six heralded single-photon sources: High production rate and low noise (top-right quarter) are desired. Projected performance of reported quantum memories for synchronizing six heralded single-photon sources: High production rate and low noise (top-right quarter) are desired. The vertical dotted line marks the value 10−3 used as the success probability of the sources (thus indicating their intrinsic noise-to-signal ratio). The labels present the group, year, and memory protocol. AFC, full atomic frequency comb; EIT, EIT storage; GEM, gradient echo memory; Raman, far-detuned Raman storage; SL, storage loop. The calculation takes the source repetition rate as the minimum between and 50 GHz, the latter estimating the current limit of the required feed-forward electronics. Source data, references, and additional details are provided in section S3. Ran Finkelstein et al. Sci Adv 2018;4:eaap8598 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).

Fig. 5 Experimental setup. Experimental setup. EOAM, electro-optic amplitude modulator; EOPM, electro-optic phase modulator; Glan, Glan-laser polarizer; HWP, half-wave plate; LIA, lock-in amplifier; PD, photodetector; SPCM, single-photon counting module. Ran Finkelstein et al. Sci Adv 2018;4:eaap8598 Copyright © 2018 The Authors, some rights reserved; exclusive licensee American Association for the Advancement of Science. No claim to original U.S. Government Works. Distributed under a Creative Commons Attribution NonCommercial License 4.0 (CC BY-NC).