SrI2(Eu) | Scintillation crystal is a new inorganic scintillation crystal that can be used in a variety of medical applications.
SrI2(Eu) | Scintillation Crystal is a new inorganic scintillation crystal. It has excellent performances in light yield, energy resolution, and energy response. In addition, with no background radiation it can be used for element isotope discrimination, medical imaging, and can be used in safety inspection areas.
| Diameter | ~25mm |
|---|---|
| Cylindrical High | ~50mm |
| Density | 4.6cm3 |
| Decay Time | ~1100ns |
| Wavelength of Maximum Emission | 435nm |
| Energy Resolution | <3.0% (Cs-137) |
| Light Output | ~300% (of NaI(Tl) for γ-rays) |
| Non-Proportionality | ~2%(60-1274keV) |
| Capsulation | Seal |
TeO2 | Piezo-Electrical Crystal is an excellent acousto-optic (AO) crystal with high AO figure of merit, birefringence, good optical rotation, and slow propagation velocity along the [110] direction.
TeO2 | Piezo-Electrical Crystal is an excellent acousto-optic (AO) crystal with high AO figure of merit, birefringence, good optical rotation, and slow propagation velocity along the [110] direction. The resolution of AO devices made of TeO2 crystals is several levels greater than others. It consists of yellow and white fine crystalline powder and when heated, it melts to a dark yellow. It is not water soluble, and the melting and boiling point is 733°C and 1260°C, respectively.
MAIN APPLICATIONS
Trans-PET® BioCaliburn® | Small-Animal PET Scanner is a high-sensitivity all-digital PET system that images mice and rats.
| Number of Detectors | 12 |
|---|---|
| Crystal | LYSO |
| Pixel Size | 1.9 x 1.9 x 13 mm³ |
| Number of Crystals | 8112 |
| Photodetector | PSPMT |
| Number of Photodetectors | 48 |
| Ring Diameter | 9.2 cm |
| Transversal FOV | 6.5 cm |
| Axial FOV | 10.6 cm |
| Sensitivity | 8.0% |
| Spatial Resolution | 1.0 mm |
| Timing Resolution | 1.5 ns |
| Energy Resolution | 15% |
| Imaging Subjects | Mouse, Rat |
| Power Supply | 110–220 V |
| Operating Temperature | 50–104 °F (10–40 °C) |
| Relative Humidity | 30–75% |
| Atmospheric Pressure | 700–1060 hPa |
| FCC Compliance | CISPR PUB. 22, FCC Part 15 |
Tubular Digital | Multichannel Pulse Amplitude Analyzer is a set of high-performance tubular digital multichannel pulse amplitude analyzers based on multiple communication interfaces (USB or Ethernet).
Tubular Digital | Multichannel Pulse Amplitude Analyzer is a set of high-performance tubular digital multichannel pulse amplitude analyzers based on multiple communication interfaces (USB or Ethernet). It can match scintillator detectors such as NaI(Tl) and LaBr3(Ce) and connect photomultiplier tubes (PMTs) with commonly used 8 or 10-stage structures.
KEY FEATURES
MAIN APPLICATIONS
| Scope of application | PMT of 8 or 10-stage structures |
|---|---|
| Consumption | <1.5W |
| HV output | 0～±1250V |
| Conversion gain | set to 1k, 2k, and 4k channels |
| ADC resolution | 12 Bit |
| ADC sampling frequency | 20/40/65 MHz |
| Integral nonlinearity | <±0.05% |
| Differential nonlinearity | <±1% |
| Maximum input pulse frequency | 500kcps |
| Maximum channel capacity N_max | N_max= 2^32-1 |
| Working environment temperature | -20～60℃ |
| Storage ambient temperature | -40～70℃ |
| Dimensions | Φ67×110mm |
V3+YAG | Q-Switch Crystal (Crystals of Yttrium-Aluminum Garnet (YAG) doped with three-valence vanadium V3+ in the tetrahedral position) is relatively new material for passive Q-switching.
V3+YAG | Q-Switch Crystal (Crystals of Yttrium-Aluminum Garnet (YAG) doped with three-valence vanadium V3+ in the tetrahedral position) is relatively new material for passive Q-switching. The Q-switching and mode-locking has been obtained with a number of active media such as YAG(Nd), KGW(Nd), and YVO4(Nd) under ash-lamp and laser diode pumping in the past years. YAG(V) has worked as an efficient Q-switch for lasers operating in the 1.0 to 1.5µm region. Additionally, the absorption band between 1.0 to 1.5µm is attributed to the 3A2 →3T2 transition of V3+ ion in the tetrahedral position of the garnet lattice and the concentration of V3+ in tetrahedral position is controlled by growth and annealing conditions.
ADVANTAGES
MAIN APPLICATIONS
XZP06A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 6 GHz.
XZP06A is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 6 GHz. The optical input is supplied through a single-mode fiber. The photodetector is designed to operate over a wide range of wavelengths. The photodetector incorporates an internal bias tee that connects the detector chip to both the bias voltage input and the DC-coupled RF signal output.
| Operating Temperature | -40–185 °F (-40–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Active Diameter | 60 µm |
| Responsivity | 0.85 A/W |
| Optical Return Loss | 30–35 |
| Reverse Breakdown Voltage | 10 V |
| Work Voltage | 3.3/5 V |
| Dark Current | 10 nA |
| 3 dB Bandwidth | 6-6.5 GHz |
| Low Frequency Cutoff | DC kHz |
| Output Resistance | 45–60 Ω |
XZP12A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 12 GHz.
XZP12A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 12 GHz. The optical input is supplied through a single-mode fiber. The photodetector is designed to operate over a wide range of wavelengths. The photodetector incorporates an internal bias tee that connects the detector chip to both the bias voltage input and the DC-coupled RF signal output.
FEATURES
| Operating Temperature | -40–185 °F (-40–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Active Diameter | 50 µm |
| Responsivity | 0.9 A/W |
| Optical Return Loss | 30–35 |
| Reverse Breakdown Voltage | 10 V |
| Work Voltage | 3.3/5 V |
| Dark Current | 10 nA |
| 3 dB Bandwidth | 10–15 GHz |
| Low Frequency Cutoff | DC kHz |
| Output Resistance | 45–60 Ω |
XZP12T | Microwave Photodetector integrates a 12 Gbps PIN photodiode and a low-noise transimpedance amplifier (TIA) into a hermetic box module.
XZP12T | Microwave Photodetector integrates a 12 Gbps PIN photodiode and a low-noise transimpedance amplifier (TIA) into a hermetic box module. The optical input is supplied through a single-mode fiber. The receiver is designed to operate at 14 Gbps optical transmission.
FEATURES
| Operating Temperature | -4–185 °F (-20–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Responsivity | 0.85 A/W |
| Optical Return Loss | 30–35 dB |
| Max. Optical Input Power | 1 mW |
| Supply Current | 28–40 mA |
| Supply Voltage | 3.0–3.6 V |
| Transimpedance Gain | 3.4 kΩ |
| Limited Output Voltage Swing | 140–150 mVₚₚ |
| 3 dB Bandwidth | 10–15 GHz |
| Low Frequency Cutoff | DC kHz |
| Output Resistance | 45–60 Ω |
XZP20A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a bandwidth of 20 GHz.
XZP20A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a bandwidth of 20 GHz. The optical input is supplied through a single-mode fiber. The photodetector is designed to operate over a wide range of wavelengths. The photodetector incorporates an internal bias tee that connects the detector chip to both the bias voltage input and the DC-coupled RF signal output.
FEATURES
| Operating Temperature | -40–185 °F (-40–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Active Diameter | 20 µm |
| Responsivity | 0.8 A/W |
| Optical Return Loss | 30–35 |
| Reverse Breakdown Voltage | 10 V |
| Work Voltage | 3.3/5 V |
| Dark Current | 50 nA |
| 3 dB Bandwidth | 18–20 GHz |
| Low Frequency Cutoff | DC kHz |
| Output Resistance | 40–60 Ω |
XZP25A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 25 GHz.
XZP25A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 25 GHz. The optical input is supplied through a single-mode fiber. The photodetector is designed to operate over a wide range of wavelengths. The photodetector incorporates an internal bias tee that connects the detector chip to both the bias voltage input and the DC-coupled RF signal output.
FEATURES
| Operating Temperature | -40–185 °F (-40–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Active Diameter | 20 µm |
| Responsivity | 0.6 A/W |
| Optical Return Loss | 30–35 |
| Reverse Breakdown Voltage | 10 V |
| Work Voltage | 3.3/5 V |
| Dark Current | 50 nA |
| 3 dB Bandwidth | 25–27 GHz |
| Low Frequency Cutoff | DC kHz |
| Output Resistance | 40–60 Ω |
XZP35A | Microwave Photodetector is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a minimum bandwidth of 35 GHz.
XZP35A is a high-speed microwave photodetector designed for direct optical-to-electrical detection, providing a bandwidth of 35 GHz. The optical input is supplied through a single-mode fiber. The photodetector is designed to operate over a wide range of wavelengths. The photodetector incorporates an internal bias tee that connects the detector chip to both the bias voltage input and the DC-coupled RF signal output.
| Operating Temperature | -40–185 °F (-40–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Active Diameter | 14 µm |
| Responsivity | 0.5 A/W |
| Optical Return Loss | 30–35 |
| Reverse Breakdown Voltage | 10 V |
| Work Voltage | 3.3/5 V |
| Dark Current | 10 nA |
| 3 dB Bandwidth | 32-35 GHz |
| Low Frequency Cutoff | DC kHz |
| Output Resistance | 45-55 Ω |
XZP43T integrates a 30 Gbps PIN photodiode and a low-noise transimpedance amplifier (TIA) into a hermetic box module.
XZP43T integrates a 30 Gbps PIN photodiode and a low-noise transimpedance amplifier (TIA) into a hermetic box module. The optical input is supplied through a single-mode fiber. The receiver is designed to operate up to 43 Gbps optical transmission.
| Operating Temperature | -4–185 °F (-20–85 °C) |
|---|---|
| Response Spectrum | 1100–1650 nm |
| Responsivity | 0.55 A/W |
| Optical Return Loss | 30–35 |
| Sensitivity | -10 dBm |
| Max. Optical Input Power | 1-3 mW |
| Supply Current | 70-100 mA |
| Supply Voltage | 3.0-3.6 V |
| Transimpedance Gain | 2 kΩ |
| Limited Output Voltage Swing | 140-150 mVpp |
| 3 dB Bandwidth | 27 GHz |
| Low Frequency Cutoff | 10-100 MHz |
| Output Resistance | 95–105 Ω |
