new material
L(Y)SO (Lutetium Yttrium Silicate) crystal is a high-performance scintillator material known for its excellent light yield, fast decay time, and superior radiation resistance. Engineered through advanced crystallization techniques, it provides high detection efficiency, strong mechanical stability, and broad spectral response. This material is widely used in medical imaging, radiation detection, high-energy physics experiments, and industrial applications, ensuring reliable performance in advanced detection and optical systems.
Product Overview:
L(Y)SO (Lutetium Yttrium Silicate) crystal is a high-quality scintillator material known for its high density, high light yield, fast decay time, and excellent energy resolution. It has wide application prospects in fields such as nuclear medicine imaging, high-energy physics, and nuclear physics. L(Y)SO crystals are primarily used in the production of γ-ray detectors, especially in Positron Emission Tomography (PET) scanners, where they serve as core detection components. Due to its outstanding performance, L(Y)SO crystal has become a key material in the next generation of nuclear medicine imaging technologies.
Key Features:
- High Energy Resolution:Provides precise energy detection, enhancing imaging and measurement accuracy.
- Fast Decay Time:The crystal has an extremely fast decay response, enabling high-speed data acquisition.
- High Light Yield:Excellent light yield ensures efficient energy conversion in detectors.
- High Light Output:Ensures stronger light signal output, improving detection sensitivity.
Applications:
- Nuclear Medicine Imaging:Widely used in Positron Emission Tomography (PET) scanners, serving as one of the core detection components.
- High-Energy Physics:Used in particle physics experiments for γ-ray detection, providing high-precision data.
- Nuclear Physics:Applied in various nuclear physics research, particularly in nuclear reactions and radiation measurements.
- Other Detection Applications:Can be used in various high-energy detectors, such as γ-ray detectors and particle counters.
| Property | Value |
| Density (g/cm³) | 7.2 |
| Melting Point (°C) | 2050 |
| Hardness (Mohs) | 5.8 |
| Refractive Index | 1.82 |
| Decay Time (ns) | <42 |
| Photon Yield (Photon/MeV) | ≥32000 |
| Radiation Resistance (rad) | >10⁶ |
| Hygroscopicity | No |
| Energy Resolution | 8-10% |
| Peak Emission (nm) | 428 |
| Effective Atomic Number | 66 |
| Irradiation Length (cm) | 1.1 |
