P-Therphenyl
From Detec-Rad.com
(C18H14)
Through the introduction of special dopants into p-terphenyl, light output can be increased by a factor of 4 to 5.
Doped p-terphenyl can be used for the detection and spectroscopy of alpha and beta particles and neutrons. It exhibits a short decay time (τ ≈ 3-4 ns) and a temperature-independent scintillation yield within a wide temperature range (- 80°C +150°C).
Single crystals of p-terphenyl are translucent, knotty over the whole volume, plastic, water-insoluble, and poorly soluble in organic solvents.
Scintillators based on doped p-terphenyl crystals are used in β-radiation spectrometry, where they are the most effective organic scintillators. They are also used in α-radiation spectrometry, as well as for fast neutrons detection in high γ-radiation background in schemes for radiation discrimination by scintillation pulse shape method.
Due to short decay time, p-terphenyl can be used in the spectrometry of high-intensity radiation
- Short decay time
- High light yield
- Lowermost light output anisotropy
- Environment resistant
Applications
- Detection and spectroscopy of α and β radiations
- Fast neutron spectroscopy n/γ
Physical Properties of p-Therphenyl
| Molecular weight (g/mol) | 230 |
| Density (g/cm3) | 1.23 |
| H/C - ratio | 0.778 |
| Melting point (°C) | 214 |
| Wavelength of emission maximum (nm) | 420 |
| Refractive index at emission maximum | 1.65 |
| Light output (104 photons/MeV) | 2.7 |
| Decay time (ns) | 3.7 |
| Ratio of ranges in the crystal and anthracene for: | |
| 0.997 |
| 1.012 |
| Radiation degradation (Mrad) | 4.5 |


