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Experimental demonstration of memory-enhanced quantum communication

MetadataDetails
Publication Date2020-03-23
JournalNature
AuthorsM K Bhaskar, R. Riedinger, B Machielse, D. S. Levonian, Nguyen Ct
InstitutionsCambridge Electronics (United States), Harvard University
Citations522
AnalysisFull AI Review Included

This analysis summarizes the experimental demonstration of memory-enhanced quantum communication using a solid-state spin memory integrated into a diamond nanophotonic cavity.

  • Core Achievement: Successful realization of asynchronous photonic Bell-State Measurements (BSM) using a single silicon-vacancy (SiV) color center in diamond as a quantum memory node.
  • Performance Breakthrough: Achieved a four-fold increase (factor of 4.1 ± 0.5) in the secure secret key rate (Rs) compared to the theoretical maximum of loss-equivalent direct-transmission Measurement Device Independent Quantum Key Distribution (MDI-QKD).
  • Scalability and Range: The system operates efficiently in the high-loss regime (88 dB effective channel loss), equivalent to approximately 350 km of telecommunications fiber, demonstrating viability for long-distance quantum networks.
  • High-Speed Operation: The memory-assisted BSM enables MDI-QKD competitive with an ideal unassisted system, operating at an average clock rate of 1.2 MHz.
  • Device Quality: The SiV-cavity system exhibits exceptional performance metrics, including a cooperativity (C) of 105 ± 11, a high Q-factor (2 x 104), and a long electronic spin coherence time (T2 > 0.2 ms).
  • Security Verification: The system maintains a low Quantum Bit Error Rate (QBER) (as low as 0.097 ± 0.006) and successfully violates the Bell-CHSH inequality (S+ = 2.21 ± 0.04), confirming fundamental security.
ParameterValueUnitContext
Operating Temperature100-300mKBSM measurements performed in dilution refrigerator
Electronic Spin Coherence Time (T2)> 0.2msUnder XY8-1 dynamical decoupling sequence
Cavity Quality Factor (Q)2 x 104-Nanophotonic diamond resonator
Cooperativity (C)105 ± 11-Key figure-of-merit for spin-photon interaction
Single-Photon Rabi Frequency (g)8.38 ± 0.05GHzAtom-cavity coupling strength
Spin Readout Fidelity (F)0.9998-Nondestructive single-shot readout in 30 ”s
Spin Initialization Fidelity (F)0.998 ± 0.001-Projective feedback-based initialization
Overall Heralding Efficiency (η)0.423 ± 0.004-Efficiency of successful reflection
Microwave π Pulse Duration (Tπ)32nsUsed for coherent spin control
Time-Bin Separation (ÎŽt)142nsPhotonic qubit encoding interval
Average QBER (Unbiased)0.116 ± 0.002-For all random bit strings
Lowest QBER (Specific Patterns)0.097 ± 0.006-Falls within threshold for unconditional security
Effective Channel Loss (PA→B)88dBEquivalent to ~350 km of telecom fiber
Average Clock Rate (N=248)1.2MHzTotal photonic qubits sent per experiment time
Bell-CHSH Violation (S+)2.21 ± 0.04-Violation of classical limit (S ≀ 2)

The memory-enhanced quantum communication relies on integrating a SiV color center within a diamond nanophotonic cavity and performing asynchronous BSM.

  1. Device Fabrication and Environment:

    • The SiV color center is integrated into a diamond nanophotonic cavity, fabricated at Harvard CNS.
    • The device is housed within a BlueFors BF-LD250 dilution refrigerator (DR) operating at 100-300 mK (base temperature 20 mK).
    • A superconducting vector magnet is used for magnetic field control.
  2. Spin Initialization and Control:

    • The SiV spin is initialized into the |↓> state with high fidelity (0.998 ± 0.001) using projective feedback-based initialization (optical readout and microwave control).
    • Coherent control of the spin qubit (fq ≈ 12 GHz) is achieved using microwave fields delivered via an on-chip gold coplanar waveguide.
    • Dynamical decoupling sequences (e.g., XY8-N) are used to maintain spin coherence (T2 > 0.2 ms) during the waiting period.
  3. Spin-Photon Interface:

    • The SiV-cavity system is critically coupled (C = 105 ± 11) to a waveguide, enabling spin-dependent modulation of cavity reflection.
    • The spin state is read out nondestructively in 30 ”s by observing electron spin quantum jumps via cavity reflection at the probe frequency (f0).
  4. Asynchronous Bell-State Measurement (BSM):

    • Photonic time-bin qubits from Alice and Bob arrive asynchronously at the central node (Charlie).
    • The state of the first photon is efficiently stored in the SiV spin memory via a heralded spin-photon gate.
    • The second photon arrives and interacts with the stored spin state.
    • Two heralding events (detection of reflected photons in the X basis via a Time-Delay Interferometer, TDI) combined with a final spin-state readout (m3) complete the asynchronous photon-photon BSM.
  5. Synchronization and Stability:

    • All microwave and optical fields are synchronized by a single device (HSDIO) and time-tagger (TT).
    • The TDI, crucial for X-basis measurements, is actively locked every ~200 ms to maintain interference visibility > 99% and minimize thermal drift.
    • A preselection procedure monitors the laser resonance with the SiV frequency to ensure high-fidelity operations over several days without human intervention.

This technology, centered on high-performance solid-state quantum memory nodes, is foundational for next-generation quantum communication infrastructure.

  • Quantum Key Distribution (QKD) Networks:
    • Enables ultra-secure, long-distance QKD by breaking the fundamental repeaterless communication bound (Rmax = PA→B/2), making MDI-QKD viable over continental distances (>350 km).
  • Scalable Quantum Repeaters:
    • The memory node is a crucial component for building scalable quantum repeaters, allowing for polynomial scaling of communication rate with distance, necessary for a global quantum internet.
  • Star Network Topology:
    • A single memory device can serve as the central hub in a star network, enabling quantum communication between multiple distant parties (Alice, Bob, etc.) beyond the metropolitan scale.
  • Modular Quantum Computing:
    • The demonstrated multi-photon gate operations can be adapted to engineer large cluster states of entangled photons, which are essential building blocks for modular quantum computing architectures.
  • Quantum Metrology and Sensing:
    • The high-fidelity spin-photon entanglement and long coherence times are applicable to non-local quantum metrology and distributed quantum sensing applications.