Data Sheet
ScintIQ™ Custom Scintillation Detectors

YAP:Ce Yttrium Aluminum Perovskite Scintillators

YAP:Ce (YAlO₃:Ce) is a cerium-doped oxide crystal optimized for fast X-ray and soft gamma-ray detection. A 27 ns decay time, absolute non-hygroscopicity, and a density of 5.55 g/cm³ make it the preferred choice when NaI(Tl) count-rate limits are a constraint. Detectors built with YAP:Ce crystals operate reliably at count rates in the MHz range.

Density5.55 g/cm³
Decay Time27 ns
Emission Max350 nm
HygroscopicNo
YAP:Ce scintillation crystal detector assembly

1Overview

YAP:Ce is Yttrium Aluminum Perovskite (YAlO₃) activated with cerium. Scintillation light arises from 5d→4f dipole transitions of the Ce³⁺ ion. Because these transitions are fully allowed, the decay is fast: 25–30 ns, with a typical value of 27 ns. That speed, combined with a density of 5.55 g/cm³ and a Mohs hardness of 8.5, positions YAP:Ce as a rugged, high-throughput alternative to NaI(Tl) for low-to-medium energy X-ray work.

The defining advantage over NaI(Tl) is the absence of hygroscopicity. YAP:Ce crystals are absolutely non-hygroscopic. They require no hermetic enclosure, and thin Mylar entrance windows are sufficient, which improves transmission at very low X-ray energies compared to the beryllium windows needed by NaI(Tl) housings. Optically polished surfaces eliminate "dead layers," so soft X-ray detection efficiency is not compromised by surface absorption.

The tradeoff is light output. Relative photoelectron yield is 35–40% of NaI(Tl) (roughly 3.5–4 photoelectrons per keV with a bialkali PMT at 25% quantum efficiency at 400 nm). Energy resolution is therefore broader than NaI(Tl), and the effective atomic number (Zavg = 36) limits detection efficiency for gamma rays above approximately 100 keV. Within its intended range, below 100 keV, YAP:Ce delivers reliable spectroscopy at count rates that would cause significant pile-up in slower crystals.

When to Choose YAP:Ce

  • Count rates exceed several hundred kHz and NaI(Tl) pile-up is a problem
  • The application targets low-energy X-rays (soft X-ray spectroscopy below 100 keV)
  • A hermetically sealed housing is impractical or adds unacceptable cost
  • Thin-window detection of soft X-rays demands minimum absorbing material at the crystal face
  • A rugged, hard crystal (Mohs 8.5) is needed in demanding environments
YAP:Ce crystal detector assembly
YAP:Ce scintillation crystal and detector assembly. The non-hygroscopic crystal surface allows thin Mylar entrance windows, maximizing soft X-ray transmission.

2Specifications

The table below lists physical and scintillation properties of YAP:Ce alongside NaI(Tl) for direct comparison. All YAP:Ce values are taken verbatim from the source datasheet.

Parameter YAP:Ce NaI(Tl) (reference)
Density (g/cm³)5.553.67
Effective atomic number (Zavg)3650
Relative photoelectron yield (%)35–40100
Refractive index1.941.85
Emission maximum (nm)350410
Decay time (ns)27230
Hardness (Mohs)8.52
HygroscopicNoYes
Maximum diameter (mm)50500
Scintillation mechanism5d→4f (Ce³⁺)Tl⁺ luminescence
Speed advantage: At 27 ns decay versus 230 ns for NaI(Tl), YAP:Ce is approximately ten times faster. Electronic shaping times below 100 ns are achievable with no signal loss, enabling detector operation in the MHz count-rate regime.

3Energy Resolution

The lower light output of YAP:Ce compared to NaI(Tl) means energy resolution is predominantly limited by photon statistics, particularly at low energies. Table 2 below lists measured energy resolution (FWHM) for a 1 mm thick YAP:Ce crystal across a range of X-ray sources. Values are taken verbatim from the source datasheet.

Source Energy (keV) Energy Resolution FWHM
Fe-555.969%
Co-5714.445%
I-12930.032%
Am-24159.520%

The lowest detectable energy above PMT noise is approximately 1 keV. Resolution improves steadily with increasing energy through the 5.9 to 59.5 keV range shown. For gamma applications requiring tighter resolution (below 10% FWHM at 662 keV), materials such as LaBr₃(Ce) or CeBr₃ are recommended. YAP:Ce is selected when speed and non-hygroscopicity outweigh resolution requirements.

Detector configuration note: Resolution figures above are for 1 mm thick crystals coupled to a bialkali PMT. Actual resolution in a fielded system will depend on crystal thickness, PMT quantum efficiency, optical coupling quality, and electronic shaping time. Contact Berkeley Nucleonics for application-specific resolution estimates.

4Typical Applications

  • Fast X-ray spectroscopy: Detection of low-energy X-rays and gamma rays in high-throughput instruments where count rates exceed NaI(Tl) capability (greater than 100 kHz, up to several MHz)
  • X-ray diffraction instruments: 1–3 mm thick crystal configurations common in XRD systems requiring simultaneous speed and adequate detection efficiency
  • Industrial gauging: Thickness, density, and composition measurement applications using X-ray transmission where fast response and ruggedness are priorities
  • Positron lifetime spectroscopy: Fast coincidence timing measurements in materials research, leveraging the sub-30 ns decay time
  • Electron microscopy: Beam-induced X-ray and secondary-electron detection where thin-window access and fast response are required
  • Medical X-ray imaging: Research and OEM detector modules where compact, fast, non-hygroscopic crystals are preferred over sealed assemblies
  • Security screening: Compact, rugged X-ray detection in field-deployed or portable instruments operating at elevated count rates
  • Nuclear physics experiments: Timing reference detectors and coincidence systems requiring a faster scintillator than NaI(Tl) in the low-Z regime

5Available Configurations

Berkeley Nucleonics ScintIQ YAP:Ce detectors are available in custom configurations to match specific instrument requirements. Standard formats are listed below. Contact our engineering team for sizes or assemblies outside the ranges shown.

Parameter Standard Range Notes
Crystal diameterUp to 50 mmPer source datasheet specification
Crystal thickness0.1 mm to verify1–3 mm common for X-ray applications; thicker for higher energy (verify)
Entrance windowMylar (thin)Non-hygroscopic crystal enables thin-window designs; Be window available on request (verify)
Optical couplingPMT (primary)Bialkali PMT standard; SiPM coupling available (verify)
Housing materialAluminum / stainless (verify)Custom flanged or threaded mounting on request (verify)
Surface finishOptically polishedNo dead layers; direct soft X-ray coupling
Hermetic sealingNot requiredCrystal is non-hygroscopic; simplifies assembly and reduces cost
Operating temperatureverifyConsult factory for high-temperature or cryogenic requirements
Items marked "verify" are general guidance based on YAP:Ce material properties and typical detector practice. Confirm with Berkeley Nucleonics engineering before specifying in critical designs.

6Request a Quote

Configure Your YAP:Ce Detector

ScintIQ detectors are built to order. Specify crystal dimensions, entrance window, readout (PMT or SiPM), housing, and quantity, and Berkeley Nucleonics will provide a formal quotation and lead-time estimate.

Email: info@berkeleynucleonics.com

Phone: 800-234-7858

Online: Use the ScintIQ Configurator

ScintIQ crystals are grown and finished with our long-standing scintillation partner in the Netherlands (Scionix Holland).