Data Sheet
ScintIQ™ Readout & Electronics

SiPM Readout for Scintillation Detectors

Compact silicon photomultiplier readout modules for ScintIQ scintillation detectors. Low-voltage, magnetic-field-immune, with integrated bias generation and temperature-compensated preamplification.

Bias voltage: 25–30 V
Gain: 106
Supply: 5.2–16 V
Power: <30 mW
Berkeley Nucleonics Corporation · info@berkeleynucleonics.com · 800-234-7858
SiPM readout module for scintillation detectors

1Overview

Silicon photomultipliers (SiPMs) are a solid-state alternative to traditional photomultiplier tubes for reading out scintillation crystals. Where PMTs demand hundreds to thousands of volts and cannot tolerate magnetic fields, SiPMs operate from a modest 25–30 V bias and are entirely insensitive to magnetic environments. The result is a readout chain that is smaller, lighter, and compatible with applications where a PMT simply cannot fit or function.

Berkeley Nucleonics offers ScintIQ detectors with SiPM readout across a wide range of crystal types and sizes. Individual SiPM elements measure 3×3 mm or 6×6 mm and can be combined into arrays to cover larger crystal faces. The readout electronics include an integrated bias generator and preamplifier module that corrects for the temperature dependence of SiPM gain, delivering stable spectroscopic performance without external compensation circuitry.

SiPM scintillation detector assembly
SiPM-coupled scintillation detector assembly. Individual SiPM elements are tiled to match the crystal face area.

2Features

  • Low bias voltage: 25–30 V (no high-voltage supply required)
  • High gain: 106
  • Completely insensitive to magnetic fields
  • Mechanically compact, no fragile vacuum envelope
  • SiPM elements: 3×3 mm and 6×6 mm; configurable as arrays
  • Operable to 60 °C
  • Integrated bias generator / preamplifier module
  • Gain drift with temperature internally corrected
  • Supply voltage: 5.2–16 V
  • Power consumption: <30 mW
  • Compatible with NaI(Tl), CsI(Tl), and other ScintIQ crystals
  • Selectable termination (1 MΩ or 50 Ω) to suit downstream electronics

3Description

SiPM Technology

A silicon photomultiplier is a solid-state photodetector built from a dense array of avalanche photodiode microcells operated in Geiger mode. When a scintillation photon strikes a microcell, it triggers a Geiger discharge that produces a standardized charge pulse. The sum of all fired microcells constitutes the SiPM output pulse, whose amplitude is proportional to the number of detected photons, and therefore to the deposited radiation energy.

SiPM gain is a strong function of the applied bias voltage relative to the device breakdown voltage. Careful bias selection is critical: too low a bias reduces gain and degrades resolution; too high a bias increases dark count rate and nonlinearity. The operating point must be chosen to match the scintillator speed and the application's resolution requirements.

Termination and signal shape: The shape of the SiPM output pulse depends strongly on the termination resistor. A 1 MΩ termination produces a slow, large-amplitude pulse suitable for direct digitization. A 50 Ω termination yields a faster pulse with lower amplitude, compatible with pulse-processing electronics optimized for speed. Select the termination to match your MCA or shaping amplifier input.

Bias Generator / Preamplifier Module

Berkeley Nucleonics supplies an integrated bias generator and preamplifier module designed specifically for SiPM-coupled scintillation detectors. The module runs from a single low-voltage supply (5.2–16 V) and consumes less than 30 mW, making it compatible with battery-operated instruments and compact embedded systems. Critically, the module includes internal temperature compensation: gain drift as a function of temperature is corrected without any external circuitry, maintaining stable spectroscopic performance across the operating temperature range.

Array Configurations

For crystal faces larger than a single SiPM element can cover, multiple elements are tiled into an array. The number of SiPMs required depends on crystal dimensions and the fraction of light-exit face that must be instrumented. Berkeley Nucleonics configures SiPM arrays to suit each detector geometry, balancing coverage, capacitance, and electronic noise.

SiPM signal waveforms at different terminations
SiPM signal waveforms from a NaI(Tl) detector. Upper trace: 1 MΩ termination (slow, large amplitude). Lower trace: 50 Ω termination (fast, lower amplitude).
Thorium spectrum from CsI(Tl) SiPM detector
Thorium-series spectrum acquired with a 35×51 mm CsI(Tl) SiPM detector, demonstrating resolved peaks and clean baseline.

4Energy Resolution Performance

Energy resolution with SiPM readout depends on crystal type and dimensions, the fraction of light-exit area covered by SiPMs, and the operating bias point. The table below lists typical energy resolution values at 662 keV (Cs-137) for representative crystal sizes and types. Values are listed as the upper bound achievable with optimized readout.

Crystal Type Crystal Size (mm) Energy Resolution at 662 keV
NaI(Tl) 32 × 25 <8.0%
CsI(Tl) 25 × 25 <7.0%
CsI(Tl) 35 × 51 <7.5%
CsI(Tl) 48 × 35 <7.5%

Note: CsI(Tl) is an excellent match for SiPM readout because its 550 nm emission peak aligns well with the SiPM photon detection efficiency curve, and it is not hygroscopic, simplifying hermetic sealing of the detector assembly.

SiPM preamplifier module
Integrated bias generator and preamplifier module for SiPM scintillation detectors. Operates from 5.2–16 V, <30 mW, with internal temperature compensation.

5Technical Specifications

SiPM Sensor

ParameterValue
Bias voltage25–30 V
Gain106
Element sizes available3×3 mm, 6×6 mm
Maximum operating temperature60 °C
Magnetic field sensitivityNone (immune)
Array configurationCustom; number of elements per crystal geometry (verify)

Bias Generator / Preamplifier Module

ParameterValue
Supply voltage range5.2–16 V
Power consumption<30 mW
Temperature compensationInternal; gain drift corrected
Termination options1 MΩ, 50 Ω
Compatible crystal typesNaI(Tl), CsI(Tl), and other ScintIQ scintillators
Form factorCompact module, dimensions verify

Signal Characteristics

ConfigurationSignal Shape
1 MΩ termination Slow, large-amplitude pulse; suited to direct ADC or MCA input
50 Ω termination Fast pulse, lower amplitude; suited to shaping amplifiers and fast electronics
Linearity note: Pulse height linearity with SiPM readout depends strongly on the bias voltage setting and on the speed of the scintillator. Optimization of the bias operating point for the chosen crystal type is recommended before final system calibration.

6Applications

SiPM readout is the right choice when PMT high voltage is impractical, when the detector must operate inside or adjacent to a magnetic field, or when size and power constraints rule out vacuum-tube technology. Typical applications include:

  • Handheld and wearable radiation monitors (battery-powered, compact)
  • Detectors inside MRI, NMR, or other high-field environments
  • Unmanned aerial vehicle (UAV) payload gamma/neutron sensors
  • Embedded radiation monitors in nuclear facilities and research reactors
  • PET scanner detector modules (LYSO/GAGG with SiPM arrays)
  • Well-logging tools requiring rugged, vibration-tolerant readout
  • Environmental and portal monitoring with low-power requirements
  • Laboratory and field instruments where PMT fragility is a concern

7Ordering & Contact

ScintIQ SiPM readout detectors are configured to specification. Crystal type, dimensions, SiPM element size, array layout, housing, and preamplifier module options are all selected at time of order. To discuss your application and request a quotation, contact Berkeley Nucleonics directly.

Request a Quote or Speak with an Engineer

Berkeley Nucleonics Corporation
2955 Kerner Blvd, San Rafael, CA 94901

Email: info@berkeleynucleonics.com

Phone: 800-234-7858

Contact form at berkeleynucleonics.com

For complete ScintIQ crystal options, visit the ScintIQ documentation index or use the detector configurator to build your system step by step.