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Cyclic cooling of quantum systems at the saturation limit

MetadataDetails
Publication Date2021-06-03
Journalnpj Quantum Information
AuthorsSebastian Zaiser, Chun Tung Cheung, Sen Yang, Durga Bhaktavatsala Rao Dasari, Sadegh Raeisi
InstitutionsUniversity of Stuttgart, Chinese University of Hong Kong
Citations14
AnalysisFull AI Review Included

Technical Documentation & Analysis: Cyclic Cooling of Quantum Systems

Section titled “Technical Documentation & Analysis: Cyclic Cooling of Quantum Systems”

Reference: Zaiser, S. et al. Cyclic cooling of quantum systems at the saturation limit. npj Quantum Information 7, 92 (2021).


This research successfully demonstrates the experimental saturation of the theoretical limit for Heat-Bath Algorithmic Cooling (HBAC) using solid-state spins in diamond Nitrogen-Vacancy (NV) centers. This achievement is critical for advancing quantum computing and sensing applications requiring high spin polarization.

FeatureAchievementCore Value Proposition
HyperpolarizationAchieved polarization beyond the limits set by Boltzmann distribution or Dynamic Nuclear Polarization (DNP).Enables superior initialization of quantum registers and enhanced quantum sensor sensitivity.
Material SystemUtilized a single NV center (electron spin) coupled to three nuclear spins (one 14N, two 13C) in a Type IIa CVD diamond crystal.Validates diamond as a robust platform for complex, multi-qubit quantum thermodynamic experiments.
MethodologyImplemented cyclic entropy compression via quantum operations (Toffoli/CNOT gates mediated by the electron spin) and subsequent reset (cooling) of the 13C spins.Provides a blueprint for iterative, high-fidelity quantum control in solid-state systems.
Control FidelityDemonstrated high nuclear spin initialization fidelity (~99%) and long coherence times (T2n ≈ 8.5 ms, T1n ~ 1s).Confirms the necessity of high-purity, low-defect CVD diamond for maintaining quantum coherence.
Application PotentialDirectly applicable to boosting Signal-to-Noise Ratio (SNR) in Nanoscale Nuclear Magnetic Resonance (NMR) and initializing large quantum registers.Opens pathways for commercializing diamond-based quantum technologies.

The following hard data points were extracted from the experimental setup and results, highlighting the stringent material and operational requirements.

ParameterValueUnitContext
Diamond MaterialType IIa CVDN/ASubstrate for NV center creation.
Crystal Orientation[100]N/ASurface orientation used for growth.
Isotopic Concentration0.2%13CUsed for surrounding nuclear spin bath.
NVC Depth~15”mBelow the diamond surface.
Static Magnetic Field (B0)~540mTAligned along the NV symmetry (z) axis.
Laser Excitation Wavelength532nmUsed for optical polarization and readout.
Electron Spin Decoherence TimeT2e ≈ 500”sLimiting factor for gate fidelity.
Nuclear Spin Decoherence TimeT2n ≈ 8.5msCoherence of the target 14N spin.
Nuclear Spin Relaxation TimeT1n ~ 1sEnables long-term storage of polarization.
14N Hyperfine Coupling-2.16MHzCoupling strength to the electron spin.
Nearest 13C Hyperfine Couplings90, 414kHzCoupling strengths to the electron spin.
Single Iteration Time~6msTotal time for compression (Ue) and reset (R).
Readout Fidelity~97%Ability to distinguish the two 14N spin states.

The experiment relies on high-precision material engineering and advanced quantum control techniques:

  1. Material Preparation: A Type IIa CVD diamond crystal with a [100] surface orientation and a controlled 0.2% 13C concentration was used. NV centers were created and located approximately 15 ”m below the surface.
  2. Device Fabrication: A coplanar waveguide (made of copper) was fabricated onto the diamond surface using optical lithography to deliver Microwave (MW) and Radio Frequency (RF) excitation pulses.
  3. Magnetic Field Control: An external static magnetic field of ~540 mT was applied along the NV center’s symmetry axis (z-axis) using a permanent magnet.
  4. Optical Pumping and Readout: A 532 nm laser was focused via an oil immersion objective to optically polarize the electron spin (S=1 ground state to ms=0) and perform single-photon counting detection for readout.
  5. Quantum Gate Implementation: Nuclear-nuclear quantum gates (required for HBAC compression Ue) were mediated by the electron spin. These gates were realized using optimized, shaped MW pulses derived from the DYNAMO optimal control platform to achieve fast, spectrally selective rotations and avoid cross-talk in the dense hyperfine spectrum.
  6. Cyclic HBAC Protocol: The core algorithm involved repeating a fixed set of operations: (1) Entropy compression (Ue) from the target 14N spin to the two 13C reset spins, and (2) Reset (R) of the 13C spins via SWAP gates with the optically polarized electron spin (the active heat-bath).

The successful replication and extension of this groundbreaking HBAC research depend entirely on access to high-quality, custom-engineered MPCVD diamond substrates. 6CCVD is uniquely positioned to supply the required materials and fabrication services.

The research utilized a Type IIa CVD diamond with specific isotopic control (0.2% 13C). 6CCVD offers the following materials to meet or exceed these requirements:

6CCVD MaterialSpecification MatchCustomization Potential
Optical Grade SCDHigh-purity, low-defect single crystal diamond (SCD) is essential for achieving the long T2n and T1n times observed.We offer SCD with ultra-low nitrogen content (Type IIa equivalent) for maximum coherence.
Isotopically Pure SCDThe experiment requires precise 13C concentration (0.2%).6CCVD provides custom isotopic engineering, including ultra-low 13C (for maximizing T2) or precisely doped 13C (e.g., 0.2% ± 0.05%) for tailored spin bath engineering.
Boron-Doped Diamond (BDD)While not used in the core experiment, BDD is crucial for integrated quantum devices.We supply BDD films for creating conductive layers, enabling integrated on-chip microwave/RF circuitry (like the coplanar waveguide) directly adjacent to the NV centers.

The experimental setup required specialized fabrication, including the integration of a coplanar waveguide and precise control over material dimensions. 6CCVD’s in-house capabilities directly address these needs:

  • Custom Dimensions and Thickness: The experiment requires small, high-quality wafers. 6CCVD supplies SCD plates from 0.1 ”m up to 500 ”m thick, and custom substrates up to 10 mm thick, ensuring compatibility with confocal microscopy and solid immersion lens integration.
  • Surface Engineering: The optical access and NV center proximity (~15 ”m) demand exceptional surface quality. We guarantee Ra < 1 nm polishing for SCD, minimizing scattering and maximizing optical collection efficiency.
  • Integrated Metalization: The coplanar waveguide fabrication requires precise metal deposition. 6CCVD offers internal metalization services, including Au, Pt, Pd, Ti, W, and Cu, allowing researchers to integrate high-fidelity microwave/RF structures directly onto the diamond surface.
  • Precision Shaping: For integrating diamond into complex setups (e.g., mounting, waveguide alignment), 6CCVD provides custom laser cutting and shaping services for plates up to 125mm.

The successful implementation of HBAC relies on optimizing the diamond material properties (purity, isotopic concentration, defect density) to match the required quantum control parameters (T1n, T2n, coupling strengths).

6CCVD’s in-house PhD team specializes in the physics and engineering of MPCVD diamond for quantum applications. We offer consultation services to assist researchers in:

  • Material Selection: Determining the optimal 13C concentration and nitrogen purity for maximizing coherence in similar Quantum Thermodynamics and Algorithmic Cooling projects.
  • Defect Control: Tailoring growth parameters to achieve specific NV center densities and depths necessary for ensemble or single-spin experiments.
  • Device Integration: Advising on metalization schemes and surface preparation for robust on-chip quantum control circuitry.

For custom specifications or material consultation, visit 6ccvd.com or contact our engineering team directly.