Skip to content

Scattering of Ultrashort X-ray Pulses on Diamonds with NV Centers

MetadataDetails
Publication Date2022-10-08
JournalCrystals
AuthorsМ. К. Есеев, Ksenia Makarova, Д. Н. Макаров
InstitutionsNorthern (Arctic) Federal University
Citations8
AnalysisFull AI Review Included

This analysis focuses on the theoretical development for characterizing complex defect structures in diamond using Ultrashort X-ray Pulses (USPs), relevant for engineers working in quantum materials and advanced diagnostics.

  • Addressing XRD Limitations: The research develops a necessary theoretical framework for X-ray Diffraction (XRD) analysis using attosecond and femtosecond USPs, correcting inaccuracies inherent in traditional XRD models that assume infinite pulse duration.
  • Pulse Duration Criticality: It is demonstrated that the USP duration ($\tau$) must be explicitly included in scattering calculations, especially when the spatial pulse length ($c\tau$) is comparable to or smaller than the characteristic length ($L$) of the defect region (e.g., NV center clusters).
  • NV Center Diagnostics: The derived scattering spectra are shown to be highly sensitive to the concentration, orientation, and spatial arrangement of Nitrogen-Vacancy (NV) centers within the diamond lattice.
  • High Sensitivity Confirmed: Simulations show that the difference ($\delta$) in scattering spectra between pure diamond and NV-center diamond can exceed two orders of magnitude, confirming the method’s utility for low-concentration defect detection.
  • Quantum Material Characterization: This methodology provides a new, ultra-high resolution diagnostic tool essential for characterizing and optimizing diamond materials used in quantum technologies.
ParameterValueUnitContext
Incident Photon Energy ($\hbar\omega_0$)7.46keVEnergy used for USP scattering simulations.
Pulse Duration ($\tau$)10attoseconds (as)Ultra-short pulse duration used in calculations.
Coherent Scattering Condition$\tau\omega_0$ >> 1DimensionlessCondition required to extend sudden perturbation theory to X-ray USPs.
Magnetic Field Neglect Condition$E_0/c^2$ << 1DimensionlessEquivalent to intensity $I$ less than 1025 W/cm2.
NV Center Sensitivity (Single Cell)~1Order of MagnitudeDifference ($\delta$) in spectra between NV-diamond unit cell and pure diamond.
NV Center Sensitivity (8 Cells)>2Orders of MagnitudeDifference ($\delta$) in spectra for 8-unit cell structure (high sensitivity).
Coherent Emission Length$c\tau$LengthSpatial region of atoms emitting coherently; must be compared to defect size $L$.
Atomic System Time ($\tau_a$)~1Atomic Unit (a.u.)Characteristic time scale for electron evolution in an atom.
  1. Sudden Perturbation Approximation: The theoretical foundation relies on the sudden perturbation approximation, assuming the electron is “frozen” during the ultra-fast interaction, valid when the pulse duration ($\tau$) is much less than the characteristic atomic time ($\tau_a$).
  2. USP Field Modeling: The incident X-ray USP is modeled using a spatially inhomogeneous electromagnetic field strength $E(\mathbf{r}, t) = E_0h(t - \mathbf{n}_0\mathbf{r}/c)$, where $\mathbf{n}_0$ is the direction of incidence.
  3. Gaussian Pulse Profile: A Gaussian function was chosen to define the USP shape $h(t)$, which simplifies the Fourier transform $h(\omega)$ used in the scattering equations.
  4. Scattering Spectra Derivation: The scattered energy per unit solid angle ($d\epsilon/d\Omega_{\mathbf{k}}$) was calculated using a modified formula (Equation 3) that explicitly includes the pulse duration parameter $\mathbf{p}\tau$ and the coherence factor $\gamma{i,j}(\mathbf{p}0, \mathbf{p}\tau)$.
  5. Coherence Analysis: The factor $\gamma_{i,j}(\mathbf{p}0, \mathbf{p}\tau)$ was analyzed to quantify the deviation from traditional XRD theory. Significant deviation occurs when the spatial pulse duration ($c\tau$) is smaller than the distance between scattering atoms ($R_{A_i} - R_{A’_j}$).
  6. System Simulation: Calculations were performed on two model systems: (a) a single diamond unit cell with one NV center, and (b) an 8-unit cell (2 x 2 x 2) structure containing one NV center, to assess concentration sensitivity.
  • Quantum Computing and Qubit Manufacturing:
    • Provides high-precision structural diagnostics necessary for quality control of diamond substrates used to host solid-state qubits (NV- centers).
    • Enables characterization of NV center concentration and spatial clustering, which directly impacts qubit coherence and performance.
  • Advanced X-ray Free-Electron Laser (XFEL) Diagnostics:
    • The developed theory is crucial for accurately interpreting data from next-generation XFEL facilities that produce attosecond pulses, allowing for time-resolved studies of electronic motion.
  • Defect Engineering in Wide-Bandgap Semiconductors:
    • Applicable to the study and optimization of other color centers and point defects in wide-bandgap materials (like SiC or GaN) where defect concentration dictates electronic or optical properties.
  • Nanoscale Metrology and Sensing:
    • The sensitivity of the scattering spectra can be leveraged to map the orientation and distribution of NV centers, which are used as nanoscale magnetic and electric field sensors.
View Original Abstract

The scattering of ultra-short X-ray pulses (USPs) is an important component of diffraction analysis of matter. Usually, the specific scattering of such USPs is not taken into account to determine the structure of a substance. Taking into account the specifics of scattering on complex structures will give more accurate results when deciphering complex structures. In this work, it is shown that when X-ray USPs are scattered on diamond with NV centers, it is necessary to take into account the pulse duration. The results obtained can be very different from the widely used theory of diffraction analysis, which confirms the need to take into account the specifics of USP scattering when diagnosing complex structures. It is shown that the scattering spectra are very sensitive to the concentration of NV-centres in the diamond structure, and this can be used in diffraction analysis.

  1. 2018 - Crystallography: Atomic secrets [Crossref]
  2. 2021 - Diagnostics of Nanosystems with the Use of Ultrashort X-Ray Pulses: Theory and Experiment (Brief Review) [Crossref]
  3. 2019 - Recent advances in ultrafast X-ray sources [Crossref]
  4. 2020 - Tunable isolated attosecond X-ray pulses with gigawatt peak power from a free-electron laser [Crossref]
  5. 2020 - Attosecond pulse shaping using a seeded free-electron laser [Crossref]
  6. 2013 - Multidimensional attosecond resonant X-ray spectroscopy of molecules: Lessons from the optical regime [Crossref]
  7. 2012 - Imaging electronic quantum motion with light [Crossref]
  8. 2014 - What will it take to observe processes in “real time”? [Crossref]
  9. 2008 - Nanoscale imaging magnetometry with diamond spins under ambient conditions [Crossref]