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Test of Diamond sCVD Detectors at High Flux of Fast Neutrons

MetadataDetails
Publication Date2025-08-07
JournalParticles
AuthorsL. Weissman, A. Shor, Sergey Vaintraub
InstitutionsSoreq Nuclear Research Center, Israel Atomic Energy Commission
AnalysisFull AI Review Included

Technical Documentation & Analysis: High-Flux sCVD Diamond Detectors

Section titled “Technical Documentation & Analysis: High-Flux sCVD Diamond Detectors”

This research validates the exceptional performance of single-crystal Chemical Vapor Deposition (sCVD) diamond detectors for high-rate neutron spectroscopy and timing applications, directly supporting 6CCVD’s core market.

  • Extreme Flux Validation: SCD detectors maintained good spectroscopic and timing performance at fast neutron flux densities up to 1010 n/s/cm2 (14 MeV neutrons), significantly higher than previously reported tests.
  • Spectroscopic Excellence: Achieved an energy resolution of 13 keV FWHM for 5.5 MeV alpha particles, comparable to high-quality silicon detectors, demonstrating superior charge collection properties in sCVD.
  • Timing Capability: Confirmed the potential for sub-nanosecond time resolution, essential for Time-of-Flight (TOF) neutron energy tagging in pulsed accelerator environments like SARAF Phase II.
  • Active Target Utility: The detector serves a dual role: a high-rate neutron flux monitor and an active target for critical nuclear physics measurements, specifically the 12C(n,n’)3α cross-section.
  • Material Specification: The successful detectors were 140 ”m thick sCVD diamond, utilizing a 100 nm Titanium (Ti) electrode, a configuration 6CCVD can replicate and optimize.
  • Radiation Hardness: The findings reinforce sCVD diamond’s superior radiation hardness (cited up to 10 MGy), making it ideal for fusion reactor diagnostics and intense accelerator facilities.

The following hard data points were extracted from the experimental results, demonstrating the high-performance metrics achieved by the sCVD diamond detectors.

ParameterValueUnitContext
Detector MaterialSingle Crystal CVD (sCVD)N/AB3 Grade Diamond
Detector Thickness140”mActive volume used in tests
Detector Area10mm2Detector surface area
Neutron Energy (Tested)14MeVGenerated via t(d,n) reaction
Peak Neutron Flux Density (Validated)1010n/s/cm2Performance validated at 25 cm distance
Maximum Neutron Flux Density (Close)1.9 x 1011n/s/cm2Close geometry (5 cm)
Alpha Energy Resolution (FWHM)13keVUsing slow CX-L amplifier (1.2 ”s shaping)
Fast Timing Resolution (FWHM)35keVUsing fast C6 amplifier (10 ns shaping)
Bias Voltage+120VOperating voltage
Electrode MaterialTitanium (Ti)100 nmDetector dead layer
Vacuum Pressure3 x 10-5mbarTest chamber environment

The experiment successfully tested sCVD detectors under high-flux conditions using a combination of standard nuclear physics techniques and advanced pulsed neutron generation.

  1. Detector Preparation: Two 140 ”m thick, 10 mm2 sCVD diamond detectors (B3 grade) were acquired, featuring a 100 nm Titanium electrode.
  2. Source Calibration: Initial tests utilized standard spectroscopic triple alpha sources (239Pu, 241Am, 244Cm) and a 252Cf fission source for energy calibration and waveform analysis.
  3. Neutron Generation: An ING-031 pulsed neutron generator (t(d,n) reaction) produced 14 MeV neutrons in short bursts.
  4. Pulsed Parameters: Neutron pulses occurred at a frequency of 30 Hz, with a duration of approximately 0.5 ”s (above 10% maximum amplitude).
  5. Amplification Strategy: Both slow (CX-L, 1.2 ”s shaping time) and fast (C6, 10 ns shaping time) spectroscopic amplifiers were used to optimize for either energy resolution or timing speed.
  6. Geometry Testing: Detectors were placed at 5 cm (high flux, high pileup) and 25 cm (validated flux, resolved events) from the neutron generator frontal surface.
  7. Simulation: GEANT4 Monte-Carlo simulations (v4.11.0.0) were performed using the NRESP71 model to understand neutron interaction channels, including elastic, inelastic, and the critical 12C(n,n’)3α reaction.

6CCVD is uniquely positioned to supply the high-purity, custom-engineered sCVD diamond required to replicate, extend, and optimize the high-flux neutron detection research performed in this study.

To achieve the high spectroscopic resolution (13 keV FWHM) and fast timing demonstrated, the highest purity material is essential.

  • Optical Grade Single Crystal Diamond (SCD): This material is required to minimize defects and charge trapping, ensuring the high charge collection efficiency necessary for superior energy resolution in high-flux environments.
  • Custom Thickness SCD: The paper utilized 140 ”m thickness. 6CCVD offers SCD plates with precise thickness control from 0.1 ”m up to 500 ”m, allowing researchers to tune the active volume for optimal energy deposition of specific reaction products (e.g., 12C(n,n’)3α products).

The success of this research hinges on precise material dimensions and electrode engineering. 6CCVD provides comprehensive in-house customization capabilities.

Research Requirement6CCVD Solution & CapabilityTechnical Advantage
Custom DimensionsPlates/Wafers up to 125mm (PCD) & Custom SCD CuttingWe can supply the specific 10 mm2 detector area used, or larger arrays for improved counting statistics, using advanced laser cutting services.
Electrode MaterialIn-House Custom Metalization (Ti, Au, Pt, Pd, W, Cu)The paper used a 100 nm Titanium (Ti) electrode. 6CCVD offers internal deposition of Ti and other metals, ensuring low-resistance ohmic contacts and precise control over the detector dead layer thickness.
Surface QualityPrecision Polishing (Ra < 1nm)Our SCD material can be polished to an atomic-scale roughness (Ra < 1nm), minimizing surface defects that could contribute to noise or charge trapping, especially critical for fast timing applications.
Global LogisticsGlobal Shipping (DDU/DDP)We ensure reliable, fast delivery of sensitive diamond detectors worldwide, simplifying procurement for international research facilities like SARAF.

6CCVD’s in-house PhD team specializes in optimizing CVD diamond properties for extreme environments and complex nuclear physics applications.

  • Material Selection for Neutron Monitoring: Our experts can assist in selecting the optimal SCD thickness and crystal orientation to maximize the signal-to-noise ratio for high-rate neutron flux monitoring, particularly in the vicinity of strong accelerator sources.
  • TOF Optimization: We provide consultation on material specifications (e.g., thickness and electrode design) to achieve the sub-nanosecond time resolution required for future Time-of-Flight (TOF) tagging counters in nuclear physics experiments.
  • BDD for Alternative Applications: While this paper focused on SCD, 6CCVD also offers Boron-Doped Diamond (BDD), which is highly relevant for thermal and epithermal neutron detection (via 10B(n,α)7Li reaction), offering a complementary solution for broad-spectrum neutron facilities.

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

View Original Abstract

We have tested the performance of spectroscopic single-crystal Chemical Vapor-Deposited (sCVD) diamond detectors with radioactive sources and with a pulsed deuterium-tritium neutron generator. The tests demonstrate that the detectors could provide good timing and spectroscopic information at high neutron fluxes. The spectroscopic information can be obtained at a 14 MeV neutron rate as high as 1010 n/cm2/s, despite some limitations associated with pulse character of the used neutron generator. Monte-Carlo simulations were performed in order to achieve better understanding of neutron interaction with the detector material. Possible applications for the use of the detectors at Soreq Applied Research Accelerator Facility (SARAF) are considered. The detectors could be used as reliable neutron rate monitors in the vicinity of a strong accelerator-based source of energetic neutrons. The detectors could also be utilized as time-of-flight tagging counters in nuclear physics experiments under condition of high neutron fluxes during short beam pulses. In particular, measurement of the 12C(n,nâ€Č)3α cross-section is discussed.

  1. 2004 - A Fast Low-Noise Charged-Particle CVD Diamond Detector [Crossref]
  2. 2006 - Radiation hard diamond sensors for future tracking applications [Crossref]
  3. 2011 - Experimental response functions of a single-crystal diamond detector for 5-20.5 MeV neutrons [Crossref]
  4. 2016 - Ionization signals from diamond detectors in fast neutron fields [Crossref]
  5. 2016 - 13C(n,α0)10Be cross section measurement with sCVD diamond detector [Crossref]
  6. 2018 - Upgrade of the compact neutron spectrometer for high flux environments [Crossref]