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The NV metamaterial - Tunable quantum hyperbolic metamaterial using nitrogen vacancy centers in diamond

MetadataDetails
Publication Date2021-07-21
JournalPhysical review. B./Physical review. B
AuthorsQing Ai, Fuli Li, Wei Qin, Jie-Xing Zhao, C. P. Sun
InstitutionsXi’an Jiaotong University, Beijing Normal University
Citations26
AnalysisFull AI Review Included
  • Core Innovation: Proposal for a novel quantum hyperbolic metamaterial (HMM) realized by embedding Nitrogen-Vacancy (NV) centers within a diamond host lattice.
  • Mechanism: The 3A2 -> 3E electronic transition of the NV centers provides a negative electric response in one principal direction, resulting in an indefinite permittivity tensor (ΔxΔz < 0) and hyperbolic dispersion.
  • Dynamic Tunability: The frequency window for negative refraction is dynamically tunable across a wide range (GHz domain) by varying the applied external magnetic field (B), which shifts the energy spectra of the NV centers.
  • Fabrication Solution: This NV-metamaterial approach overcomes the significant difficulty of fabricating classical sub-micron elements required for optical-frequency HMMs, utilizing standard diamond synthesis (CVD, ion implantation).
  • Critical Density: Negative refraction is theoretically feasible at low NV densities, requiring a minimum concentration of 5.00 ppb, which is well within current experimental fabrication capabilities (e.g., 16 ppm).
  • Engineering Value: The material enables applications including subwavelength imaging (superlens), enhanced spontaneous emission, and control over heat transport and acoustics.
ParameterValueUnitContext
Ground State Zero-Field Splitting (Dgs)2.88GHzElectronic ground state (3A2)
Excited State Zero-Field Splitting (Des)1.42GHzElectronic excited state (3E)
Strain-Related Coupling (Ο)70MHzExcited state Hamiltonian
Excited State Lifetime (Îł-1)10nsHomogeneous lifetime
Transition Dipole Moment (d)11DEstimated for 3A2 -> 3E transition
Relative Permittivity (Diamond, ΔD)5.7N/APure diamond background
Critical NV Density (nc)1.77 x 1021m-3Required for one permittivity component (Δ(1)) to equal 0
Minimum NV Density (nmin)5.00ppbRequired to demonstrate negative refraction
Negative Refraction Window (B=0 G, n0=0.5 ppm)(-1.46, 2.37)GHzFrequency range (Δω)
Negative Refraction Window (B=0 G, n0=16 ppm)Significantly broadenedN/AIncreased density broadens the window
NV Center Orientation Angle (α)109°28’DegreesAngle between any pair of the four possible orientations

The realization of the NV-metamaterial is based on detailed quantum mechanical and electromagnetic modeling:

  1. NV Center Hamiltonian Definition: The electronic ground state (3A2) and excited state (3E) Hamiltonians were established, incorporating zero-field splitting (D), magnetic field (B), and strain (Ο) effects.
  2. Optical Transition Selection Rules: Selection rules for the electric dipole-induced optical transition (3A2 -> 3E) were derived, ensuring conservation of spin and total angular momentum.
  3. Polarization Density Calculation: Linear response theory (Kubo formalism) was used to calculate the polarization density (P) induced by the incident electromagnetic field, dependent on the transition frequencies and NV density (n0).
  4. Permittivity Tensor Derivation: The relative permittivity tensor (Δr) was derived, showing that the 3A2 -> 3E transition causes one principal component (Δx) to become negative near resonance, while others (Δz) remain positive.
  5. Local Field Correction: The Lorentz local field theory was applied to account for dipole-dipole interactions, confirming that the local field effects do not qualitatively change the center or width of the negative refraction domain.
  6. Hyperbolic Dispersion Confirmation: The condition ΔxΔz < 0 was established, confirming the material exhibits hyperbolic (indefinite) dispersion, a prerequisite for negative refraction.
  7. Negative Refraction Proof: Maxwell’s equations were solved for a Transverse Magnetic (TH) incident mode at the interface, analytically proving that negative refraction occurs when the Poynting vector component (Stx) is negative.

This technology interlinks quantum devices (NV centers) and metamaterials, enabling advanced functionalities in several high-impact fields:

  • Subwavelength Optics & Imaging:
    • Construction of Superlenses capable of imaging objects far below the classical diffraction limit.
    • Subwavelength imaging and focusing applications.
  • Quantum Emitter Control:
    • Spontaneous Emission Enhancement (Purcell effect) by engineering the local electromagnetic environment.
    • Lifetime Engineering for quantum emitters, controlling radiative decay rates.
  • Quantum Sensing:
    • NV centers are highly sensitive quantum sensors; the metamaterial structure could enhance sensitivity to external signals (electric field, magnetic field, temperature).
  • Energy and Transport:
    • Advanced control over Heat Transport (thermal metamaterials).
  • Acoustic Engineering:
    • Potential application in Acoustic Metamaterials for magnifying or controlling sound waves (analogous to the electromagnetic hyperlens).
  • Fundamental Physics Simulation:
    • Used in Analogue Cosmology to simulate complex physical phenomena, such as metric signature transitions.
View Original Abstract

We show that nitrogen-vacancy (NV) centers in diamond can produce a novel\nquantum hyperbolic metamaterial. We demonstrate that a hyperbolic dispersion\nrelation in diamond with NV centers can be engineered and dynamically tuned by\napplying a magnetic field. This quantum hyperbolic metamaterial with a tunable\nwindow for the negative refraction allows for the construction of a superlens\nbeyond the diffraction limit. In addition to subwavelength imaging, this\nNV-metamaterial can be used in spontaneous emission enhancement, heat transport\nand acoustics, analogue cosmology, and lifetime engineering. Therefore, our\nproposal interlinks the two hotspot fields, i.e., NV centers and metamaterials.\n