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Microwave mode cooling and cavity quantum electrodynamics effects at room temperature with optically cooled nitrogen-vacancy center spins

MetadataDetails
Publication Date2022-11-02
Journalnpj Quantum Information
AuthorsYuan Zhang, Qilong Wu, Hao Wu, Xun Yang, Shi‐Lei Su
InstitutionsAarhus University, Beijing Institute of Technology
Citations11
AnalysisFull AI Review Included

This research details a theoretical and computational study predicting significant improvements in microwave mode cooling and Cavity Quantum Electrodynamics (C-QED) effects using optically cooled Nitrogen-Vacancy (NV) centers in diamond at room temperature.

  • Core Achievement: Predicted a reduction of the microwave photon number to 261, corresponding to an effective mode temperature of 116 K (compared to the ambient 293 K).
  • Performance Gain: This predicted cooling is approximately five times better than previously reported NV center cooling results (188 K).
  • Mechanism: Utilizes optical pumping of NV center spins (specifically the 0 → +1 Zeeman transition at 9.22 GHz) to collectively cool a coupled dielectric microwave resonator.
  • Enhanced Design: The proposed setup uses a high-frequency (9.22 GHz) resonator with a low damping rate (1.88 MHz), which enhances the spin-resonator energy transfer rate and suppresses thermalization by an order of magnitude compared to previous low-frequency setups.
  • Advanced Modeling: A comprehensive multi-level Jaynes-Cumming (JC) model was developed, solved using a second-order mean-field approach, to accurately simulate the collective effects of trillions of NV spins.
  • C-QED Control: Demonstrated that laser power can be used to control the collective coupling strength, enabling the observation of C-QED effects (Rabi oscillations and mode splitting) across weak-to-strong coupling regimes at room temperature.
ParameterValueUnitContext
Ambient Operating Temperature (T)293KRoom temperature operation.
Predicted Minimum Effective Mode Temperature (Tmode)116KAchieved via optical spin cooling.
Predicted Minimum Photon Number (nmin)261PhotonsEquivalent to 116 K effective temperature.
Thermal Photon Number (nth)661PhotonsThermal background at 293 K for the 9.22 GHz mode.
Resonator Frequency (ωm)9.22GHzResonant with the NV center 0 → +1 spin transition.
Resonator Photon Damping Rate (Îș)1.88MHzRate of thermalization/photon loss in the resonator.
Single Spin-Resonator Coupling (g31)2π * 0.64MHzCoupling strength between one NV spin and the mode.
Spin Dephasing Rate (Îł3)2π * 0.64MHzDephasing rate for the +1 spin level.
Optical Excitation Wavelength532nmUsed for optical pumping and spin initialization.
Optical Pumping Rate (Ο) Range10-3 to 103HzRate proportional to the input laser power (P).
Spin Ensemble Size (N)TrillionsSpinsSimulated using a mean-field approach.

The study employed a detailed theoretical model and computational simulation to predict system performance, moving beyond simplified two-level models.

  1. System Definition: Modeled NV centers in diamond coupled to a high-Q dielectric ring microwave resonator (9.22 GHz) within a copper cavity, subjected to a magnetic field to Zeeman-split the spin levels.
  2. Multi-Level Jaynes-Cumming (JC) Model: Developed an extended JC Hamiltonian incorporating the full electronic structure of the NV center: the triplet ground state (3A2, levels 0, ±1), the triplet excited state (3E), and a fictitious level (7k) representing the singlet excited states (1A1, 1E).
  3. Dissipation and Pumping: The quantum master equation included comprehensive dissipative superoperators accounting for:
    • Optical excitation and stimulated emission (rate Ο).
    • Spontaneous emission (ksp).
    • Inter-system crossing (ISC) between triplet and singlet states (kij).
    • Spin-lattice relaxation (kij) and spin dephasing (χ).
    • Thermal photon emission/absorption (rate Îșnth).
  4. Simulation Technique: The quantum master equation was solved for the reduced density operator (ρ) using a mean-field approach (QuantumCumulant.jl package).
  5. Collective Effects: The simulation utilized a second-order cumulant expansion to accurately capture spin-photon and spin-spin quantum correlations, which are crucial for modeling the collective behavior of trillions of NV centers.
  6. Performance Quantification: Cooling performance was quantified by calculating the steady-state mean intra-resonator photon number (⟹a†a⟩) and converting this to an effective mode temperature (Tmode).

The ability to achieve near-cryogenic microwave performance at room temperature using a bench-top device has significant implications for quantum technologies and high-sensitivity measurements.

  • Quantum Sensing and Metrology:
    • Enhanced NMR/ESR: Improved measurement sensitivity in Electron and Nuclear Spin Resonance experiments by reducing thermal noise in the microwave detection chain.
    • Quantum Metrology: Potential application in high-precision frequency standards, leveraging the 9.22 GHz frequency (relevant to Cesium clocks).
  • Quantum Information Processing:
    • Quantum Gates: Enables the study and implementation of quantum gate operations and quantum entanglement using purer, less noisy quantum states.
    • Solid-State QED: Provides a robust, room-temperature platform for studying C-QED effects (Rabi splitting, superradiance) in solid-state spin systems.
  • Quantum Thermodynamics:
    • Heat Engines: Facilitates experimental demonstration and study of quantum effects in the operation of microscopic heat engines at non-equilibrium temperatures.
  • Cryogenics Replacement: Offers a compact, bench-top solution for cooling microwave components, potentially replacing bulky and expensive dilution refrigerators in specific applications.