Data Sheet
ScintIQ™ Readout & Electronics

SiPM-Based Alpha/Beta Detector

Thin-profile scintillation detector combining ZnS(Ag)+plastic scintillator with a SiPM array readout, integrated temperature-compensated bias generator, and charge-sensitive preamplifier. Designed for low-noise alpha and beta particle counting in a compact, self-contained module.

ZnS(Ag)+Plastic / EJ-444 SiPM Array Readout +5 to +16 V Supply LEMO ERA0S302 Output <50 keV Noise (betas)
Document ref: 51BM0.25_SIP-EJ444-E3-X2  |  Rev. 0  |  dc-20809102
51BM0.25/SIP-EJ444-E3-X2 thin-model SiPM alpha/beta scintillation detector

1Overview

Outline drawing of the detector showing the round Ø59 mm active head and cable stem
Outline of the detector head: Ø59 mm body, 79.5 mm overall length, 40 mm depth, with section line A-A.

The ScintIQ™ SiPM-Based Alpha/Beta Detector is a thin, self-contained scintillation probe engineered for simultaneous or separate alpha and beta surface contamination measurements. It replaces the traditional photomultiplier tube with a silicon photomultiplier (SiPM) array, eliminating the need for a high-voltage supply while delivering comparable sensitivity in a far more compact form factor.

The active element is a Ø51 mm x 0.25 mm ZnS(Ag)+plastic scintillator disc (EJ-444 grade). ZnS(Ag) is the industry standard phosphor for alpha detection, and the thin plastic substrate provides the beta response. A light-tight double aluminized mylar entrance window (0.9 mg/cm²) maximizes transmission for low-energy alpha and beta particles, while a 72% transmission stainless steel grid provides mechanical protection without substantially attenuating particle flux.

An on-board temperature-compensated bias generator sets the SiPM operating voltage automatically across the full +5 V to +16 V supply range. The integrated charge-sensitive preamplifier conditions the signal before it exits via the LEMO ERA0S302 connector. No external preamplifier, high-voltage module, or bias adjustment is required. Connect power and signal, and the detector is ready.

Photograph of the assembled SiPM alpha/beta detector with model label
The assembled detector module (51BM0.25/SIP-EJ444-E3-X2), showing the round entrance face and the integrated readout housing.

2Features

  • ZnS(Ag)+plastic scintillator, Ø51 mm x 0.25 mm (EJ-444 grade)
  • SiPM array readout (J-60035-4P): no high-voltage supply required
  • Built-in temperature-compensated bias generator, operating from +5 to +16 V
  • Integrated charge-sensitive preamplifier for direct signal output
  • Light-tight double aluminized mylar entrance window, 0.9 mg/cm²
  • 72% transmission stainless steel protective grid
  • Black polyester housing, fully light-tight
  • LEMO ERA0S302CLL connector with flying leads (50 cm, 4-core shielded LIYD11Y cable)
  • Low noise floor: <50 keV equivalent (betas) at 22 °C
  • Distinct pulse timing for alpha and beta discrimination
  • Low power draw: 3 mA nominal supply current

3Description

Scintillator Assembly

Cross-section A-A of the detector showing entrance window, lightguide, SiPM and cable
Cross-section A-A: 6 micron aluminized mylar entrance window and stainless steel protective mesh over a Ø51 x 15 mm PMMA lightguide, reflector, optical coupling, SiPM, and LiYD11Y 4-core cable.

The detector uses a phoswich-style layered scintillator: a ZnS(Ag) alpha-sensitive phosphor deposited on a thin plastic substrate that provides beta sensitivity. The complete disc measures 51 mm in diameter and just 0.25 mm thick. This geometry keeps the overall areal density low, allowing alpha particles with ranges in the milligram-per-centimeter-squared regime to reach the phosphor with minimal attenuation.

EJ-444 is a commercially established scintillator configuration matched to SiPM and photomultiplier readout. The emission spectrum of ZnS(Ag) peaks near 450 nm, aligning well with the spectral sensitivity of modern SiPM devices.

SiPM Readout and Bias

Rather than a conventional photomultiplier tube requiring hundreds of volts, this detector uses a J-60035-4P SiPM array operating from a low-voltage regulated supply. The temperature-compensated bias generator on the detector PCB tracks SiPM breakdown voltage shifts with temperature, maintaining consistent gain across operating conditions without external adjustment.

SiPM readout brings practical advantages for field and laboratory use: ruggedness against magnetic fields, insensitivity to orientation, and compatibility with battery-powered or portable electronics. The supply requirement of +5 to +16 V at 3 mA draws less than 50 mW and is met by standard laboratory supplies, USB-derived rails, or small battery packs.

Signal Conditioning and Output

The on-board preamplifier converts SiPM charge output to a voltage pulse presented at the LEMO ERA0S302CLL connector. Alpha events produce a slower, larger pulse (rise time approximately 530 ns, fall time approximately 530 ns) with a gain of approximately 500 mV per 5.48 MeV alpha. Beta events are faster and smaller (rise time approximately 150 ns, fall time 1/e approximately 1.2 µs) with a gain of approximately 75 mV/MeV. This timing difference allows downstream electronics or software to discriminate alpha from beta events using pulse-shape analysis.

Oscilloscope capture of a fast, low-amplitude beta output pulse
Beta output pulse on an oscilloscope (1 µs/div, 20 mV/div). Fast rise with a roughly 1.2 µs fall.
Oscilloscope capture of a slower, larger alpha output pulse
Alpha output pulse on an oscilloscope (1 µs/div, 200 mV/div). Larger amplitude with the slower alpha timing.

Housing and Window

The compact black polyester housing is fully light-tight, allowing operation in ambient lighting without signal contamination from optical photons. The entrance window is a double aluminized mylar film at 0.9 mg/cm², providing the low mass needed for alpha transmission while maintaining light exclusion. A stainless steel grid (72% transmission) over the window resists mechanical damage without meaningfully attenuating radiation.

4Technical Specifications

Detector

ParameterValue
Scintillation materialZnS(Ag)+plastic scintillator (EJ-444 grade)
Active area diameter51 mm
Scintillator thickness0.25 mm
Crystal readoutSiPM Array J-60035-4P
Entrance windowLight-tight double aluminized mylar, 0.9 mg/cm²
Window protectionStainless steel grid, 72% transmission
HousingBlack polyester, light-tight

Electrical

ParameterValue
Supply voltage+5 to +16 V
Supply current3 mA (nominal)
Bias generatorBuilt-in, temperature-compensated
PreamplifierCharge-sensitive, integrated
Output connectorLEMO ERA0S302CLL with flying leads
Pin 1+5 to +16 V (brown wire)
Pin 2Signal output (white wire)
Cable50 cm, 4-core shielded LIYD11Y

Performance

ParameterAlphaBeta
Pulse rise time (0–100%) 530 ns 150 ns
Pulse fall time (1/e) 530 ns 1.2 µs
Gain approx. 500 mV / 5.48 MeV approx. 75 mV/MeV
Noise level <50 keV equivalent (betas) at 22 °C
Conditions: Specifications are measured at 22 °C ambient unless noted. The temperature-compensated bias generator maintains nominal SiPM operating point over the rated temperature range (verify full temperature range with Berkeley Nucleonics). Contact info@berkeleynucleonics.com for application-specific characterization data.

5Performance Figures

The figures below are measured spectra and discrimination data for this detector configuration, taken under alpha, beta, and mixed alpha/beta irradiation.

241-Am alpha spectrum: counts versus channel
241-Am alpha spectrum (counts versus channel). Broad alpha distribution from the 5.48 MeV Am-241 source.
Cl-36 beta spectrum: counts versus channel
Cl-36 beta spectrum (counts versus channel). Continuous beta distribution from the Cl-36 source.
Mixed 241-Am / Cl-36 alpha/beta spectrum on a logarithmic count axis
Mixed 241-Am / Cl-36 alpha/beta spectrum (counts versus channel, logarithmic count axis). Beta events dominate the low channels and alpha events form the broad mid-channel feature.
2D PSD scatterplot of PSD parameter versus ADC channel under mixed alpha/beta irradiation
2D pulse-shape discrimination scatterplot (PSD parameter versus ADC channel) under mixed alpha and beta irradiation. The faster beta pulses and slower alpha pulses separate into distinct populations, enabling software discrimination of particle type.

6Applications

The SiPM-Based Alpha/Beta Detector is suited for laboratory and field environments where simultaneous or separate alpha and beta surface activity measurements are needed. Representative applications include:

  • Surface contamination surveys in nuclear facilities, decommissioning projects, and radiological laboratories
  • Alpha/beta ratio determination for source characterization and isotope identification workflows
  • Gross alpha and beta counting in water, air filter, and wipe sample analysis
  • Field portal and personnel monitoring where a compact, battery-compatible probe is required
  • Research and calibration using alpha reference sources (e.g., Am-241 at 5.48 MeV) and beta sources
  • Environmental monitoring and regulatory compliance measurements
  • Portable instrument integration with MCA, rate meters, and digital acquisition systems that accept preamplified output
Pulse-shape discrimination: The different rise and fall times for alpha versus beta events allow software-based PSD to separate particle types in a mixed-field environment without a coincidence guard detector. See the 2D PSD scatterplot in Section 5.

7Ordering & Contact

The ScintIQ™ SiPM-Based Alpha/Beta Detector is available from Berkeley Nucleonics. Contact the applications team to discuss supply voltage compatibility, connector variants, cable length options, and integration with Berkeley Nucleonics MCA and readout electronics.

Model Information

ReferenceDescription
51BM0.25/SIP-EJ444-E3-X2 Thin-model Alpha/Beta SiPM Scintillation Detector, ZnS(Ag)+plastic, Ø51 mm x 0.25 mm, SiPM Array J-60035-4P readout, integrated temperature-compensated bias and preamplifier, LEMO ERA0S302CLL output

Drawing number: V-1611. Contact Berkeley Nucleonics for custom configurations, alternate scintillator sizes, or modified cable assemblies.