品牌 | 西安立鼎光电 | 型号 | 30 |
产品介绍:
si探测器
光谱响应图
硅光电探测器是光电器件重要的的组成部分,是可见光和近红外波段主要的探测器。硅的探测器的工作波长在0.3-1.0微米。在室温的条件下,该产品具有很高的灵敏度,还有一些附件支持,如滤光片(长波滤光片和带通滤光片)、前置放大器、光纤连接器。这些器件可应用在工业的控制系统、气体分析、热传感器以及光纤测试设备中。
技术参数:
1、室温Si探测器
Detector type | Active Dia (mm) | Shunt Resistanve (MΩ) | Shunt Capacitance pF),tpy | OperatingWavelength (nm) | Spectral Responsivity (A/W) | NEP (W/ HZ 1/2 ) @800nm,1KHz |
LD-S-010 | 1.0 | 500 | 25 | 300-1000 | 0.55@850nm | <1.0x10-14 |
LD-UVS-010 | 1.0 | 500 | 50 | 200-1000 | 0.55@800nm | <1.0x10-14 |
LD-S-025 | 2.5 | 500 | 400 | 300-1000 | 0.55@850nm | <1.0x10-14 |
LD-UVS-025 | 2.5 | 200 | 300 | 200-1000 | 0.50@800nm | <1.5x10-14 |
LD-S-050 | 5 | 200 | 1500 | 350-1100 | 0.55@850nm | <1.5x10-14@850nm |
LD-UVS-050 | 5 | 50 | 1000 | 200-1100 | 0.50@800nm | <3.0x10-14@700nm |
LD-S-100 | 10 | 10 | 1000 | 350-1100 | 0.50@850nm | <1.0x10-13@850nm |
LD-UVS-100 | 10 | 50 | 1800 | 200-1000 | 0.50@800nm | <5x10-14@800nm |
LD-S-113 | 11.3 | 200 | 9000 | 300-1100 | 0.55@850nm | <1.5x10-14 |
LD-UVS-113 | 11.3 | 10 | 4000 | 200-1000 | 0.50@800nm | <1.0x10-13 |
2、二级制冷Si探测器
type | OperatingTemperature(℃) | Shunt Resistanve (MΩ) | Shunt Capacitance (pF),tpy | NEP (W/ HZ 1/2 )@800nm | Responsivity@850nm (A/W) | Cooler Current (A) |
LD-S-010-TE2 | 22 | 500 | 25 | —— | 0.55 | 0.00 |
-30 | >1000 | 25 | —— | 0.55 | 0.65 | |
LD-UVS-010-TE2 | 22 | 500 | 50 | —— | 0.55 | 0.00 |
-30 | >1000 | 50 | —— | 0.55 | 0.65 | |
LD-S-025-TE2 | 22 | 100 | 400 | <1.9x10-14 | 0.55 | 0.00 |
-30 | >1000 | 400 | <5x10-15 | 0.55 | 0.65 | |
LD-UVS-025-TE2 | 22 | 200 | 300 | <1.5x10-14 | 0.55 | 0.00 |
-30 | >1000 | 300 | <10-14 | 0.55 | 0.65 | |
LD-S-050-TE2 | 22 | >200 | 1000 | <1.5x10-14 | 0.55 | 0.00 |
-30 | >1000 | 1000 | <10-14 | 0.55 | 0.65 | |
LD-UVS-050-TE2 | 22 | >100 | 1000 | <2x10-14 | 0.55 | 0.00 |
-30 | >1000 | 1000 | <10-14 | 0.55 | 0.65 | |
LD-S-100-TE2 | 22 | 10 | 1000 | <1.0x10-13 | 0.50 | 0.00 |
-30 | 500 | 900 | <1.0x10-14 | 0.50 | 0.70 | |
LD-UVS-100-TE2 | 22 | 50 | 1800 | <5.0x10-14 | 0.50 | 0.00 |
-30 | 1000 | 1600 | <1.0x10-14 | 0.50 | 0.70 |