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X-ray Spectrum Reconstruction by Diamond Detectors with Linear Response to Dose Rate

MetadataDetails
Publication Date2021-10-18
JournalCrystals
AuthorsD.M. Trucchi, P. Ascarelli
InstitutionsInstitute of Structure of Matter
Citations2
AnalysisFull AI Review Included

This research demonstrates the successful reconstruction of high-flux X-ray bremsstrahlung spectra using a polycrystalline CVD diamond detector, enabled by achieving a highly linear response to the radiation dose rate.

  • Core Achievement: Accurate reconstruction of the X-ray source spectrum (bremsstrahlung and Kα line) using the classic absorbers method, refined with a modern analytical model.
  • Critical Enabling Condition: The 50 ”m polycrystalline diamond detector achieved near-ideal linearity to the radiation dose rate, characterized by a linearity coefficient (Δ) of 0.997 ± 0.003.
  • Operational Requirement: This linear response was only achieved when the detector was biased at ≄90 V, corresponding to a high internal electric field (≄1.8 x 104 V/cm), ensuring complete collection of photogenerated charge carriers.
  • Material Advantage: The use of relatively cheap, large-area polycrystalline CVD diamond films is validated for high-flux spectrometry applications where current mode operation (not pulsed mode) is necessary.
  • Methodology: The absorbers method utilized variable thicknesses of Nichrome and Aluminum foils to selectively attenuate the X-ray beam based on energy-dependent attenuation coefficients.
  • Future Potential: The technique, once optimized with variable thickness Nickel filters, promises accurate disentanglement of closely spaced characteristic lines, such as the Copper Kα and KÎČ peaks.
ParameterValueUnitContext
Detector MaterialPolycrystalline CVD DiamondN/AFree-standing film
Film Thickness50”mActive volume dimension
Electrode MaterialSilver (Ag)N/AThermally evaporated contacts
Electrode Thickness200nmMinimized to reduce absorption perturbation
Electrode Size7 x 7mm2Sandwich configuration
Bias Voltage (Linearity Saturation)≄90VRequired for linear dose rate response
Electric Field (Linearity)≄1.8 x 104V/cmCalculated from 90 V bias / 50 ”m thickness
Linearity Coefficient (Δ)0.997 ± 0.003N/AResponse linearity to dose rate (Ideal = 1)
Diamond Bandgap (Eg)5.47eVIntrinsic material property
Mean Ionization Energy (w)13.1eVEnergy to generate one electron-hole pair
X-ray Source AnodeCopper (Cu)N/APhilips microfocus tube
X-ray Accelerating Voltage (Vacc)30, 40kVUsed for absorber tests
Fixed Filter Thickness20”mNickel (Ni) foil to suppress Cu KÎČ line
Copper Kα Energy8.05keVPrimary characteristic line
Absorber MaterialsAluminum (Al), Nichrome (80% Ni - 20% Cr)N/AUsed for attenuation measurements
  1. Film Synthesis and Preparation:

    • Growth: Polycrystalline diamond film was grown via Microwave CVD (MWCVD) heteroepitaxy on a <100> p-type silicon substrate.
    • Growth Parameters: 0.5% methane/hydrogen concentration at 700 °C.
    • Substrate Removal: Silicon was chemically etched using a standard HNO3:HF diluted solution.
    • Cleaning: Non-diamond phases were removed using a 1:1:1 HNO3:H2SO4:HClO4 solution.
  2. Device Fabrication:

    • Electrodes: Two 200 nm thick, 7 x 7 mm2 silver (Ag) contacts were thermally evaporated onto opposite sides of the 50 ”m film (transversal/sandwich configuration).
    • Electrical Behavior: The resulting contacts exhibited a nearly ohmic behavior at low bias voltages (<10 V) and a non-linear exponential behavior at higher voltages.
  3. Detector Stabilization (Priming):

    • The film was exposed to prolonged irradiation (approximately 10 Gy total dose) to saturate deep level traps, ensuring a stable, reproducible response.
  4. Dose Rate Linearity Measurement:

    • The photogenerated current (Iph) was measured as a function of the radiation dose rate (Ď) at various bias voltages (Vb).
    • Data was fitted using Fowler’s equation (Iph ∝ ĎΔ) to determine the linearity coefficient (Δ).
  5. Spectrum Reconstruction (Absorbers Method):

    • The X-ray beam was pre-filtered using a fixed 20 ”m Nickel foil.
    • Absorbers (Al or Nichrome) of variable thickness (x) were placed in the beam path to attenuate the radiation intensity.
    • The detector signal f(x) was measured and modeled as the sum of the Kα contribution (modeled by a Dirac delta function) and the continuous bremsstrahlung contribution.
    • The bremsstrahlung component was fitted using an approximated solution similar to a diffusion integral, allowing the reconstruction of the original spectrum Fbremm(E).

The demonstrated ability to achieve linear dose rate response in polycrystalline diamond detectors under high-flux conditions opens applications in several engineering and medical fields:

  • Medical Dosimetry: Monitoring radiation beams in advanced radiation therapy (e.g., Intensity Modulated Radiation Therapy—IMRT, Volumetric Modulated Arc Therapy—VMAT) and mammography, where high spatial resolution and fast response are critical.
  • Synchrotron and Accelerator Facilities: Used as beam monitors and dosimeters in high-energy physics experiments and synchrotron beamlines characterized by high photon fluxes (current mode operation).
  • Non-Destructive Testing (NDT): Integration into industrial X-ray systems requiring accurate spectral information for quality control and materials characterization.
  • Nuclear and Fusion Energy: Deployment as radiation-hard sensors for monitoring ionizing radiation and fast neutrons in fusion reactors (e.g., ITER, JET) and nuclear facilities.
  • Radiological Protection: Development of robust, radiation-resistant dosimeters for personnel and environmental monitoring in harsh radiation environments.
View Original Abstract

The absorbers method is here applied by interposing filters of variable thickness between the X-ray source and a detector so to attenuate the radiation intensity by using the attenuation coefficient as a selective photon energy operator. The analysis of the signal provided by a polycrystalline diamond thin film detector exposed to the energy-selectively-attenuated X-ray beam was used for the reconstruction of the radiation spectrum. The 50 ÎŒm thick diamond detector achieves conditions of linear response to the dose rate of the incident radiation (linearity coefficient of 0.997 ± 0.003) for a bias voltage ≄90 V, corresponding to an electric field ≄1.8 × 104 V/cm. Once the absorbers method is applied, only the detector signal linearity to dose rate allows reconstructing the source X-ray bremsstrahlung spectrum with sufficiently high accuracy.

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