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光电倍增管单元
H10330C-45
H10330C 系列是一款紧凑型 NIR-PMT 单元（近红外光电倍增管），利用我们先进的光阴极面技术开发。NIR-PMT 包含在一个高真空热绝缘密封外壳中。内部电子制冷器无需液氮和冷却水。这些模块的受光窗使用聚光透镜，可提供更大的受光面，确保能够轻松实现光学耦合。还可提供用于连接光纤和单色仪的适配器选件。
C10330C 系列有三种阵容。（H10330C-45：950 nm 至 1400 nm，H10330C-25：950 nm 至 1200 nm，H10330C-75：950 nm 至 1700 nm）
特点
- 高灵敏度（适用于光子计数）
- 快速响应：上升时间：0.9 ns，T.T.S.：400 ps
- 通过风冷式电子制冷器实现简便操作：无需液氮，无需冷却水
- 可在开机后 20 分钟内操作
- 大检测面：检测平行光时直径达到 18 mm
用途
- 光致发光测量
- 单线态氧测量
- LIDAR
- 拉曼光谱测量
- 阴极射线发光测量
- 荧光、荧光寿命测量
- 光通信设备评估
特性
光谱灵敏度特性
时序属性
波形
渡越时间分散度 (T.T.S.)
详细参数
| 参数 | 说明/值 | 单位 | ||
|---|---|---|---|---|
| 光谱灵敏度特性 | 950 至 1400 | nm | ||
| 光阴极面材料 | InP/InGaAsP | - | ||
| 平行光检测面 | φ18 | mm | ||
| PMT 的有效面积 | φ1.6 | mm | ||
| 最大值 PMT 电源电压 | -900 | V | ||
| PMT 平均阳极电流高达 | 1 | µA | ||
| 阴极 *1 | 量子效率 | 最小 | 1 | % |
| 典型值 | 2 | |||
| 辐射灵敏度 | 典型值 | 21 | mA/W | |
| 阳极 | 辐射灵敏度 *1*2 | 典型值 | 2.1×104 | A/W |
| 增益率 | 典型值 | 1.0×106 | - | |
| 阳极暗电流 *2*3 | 典型值 | 4 | nA | |
| 最大值 | 40 | |||
| 阳极暗计数 *2*3 | 典型值 | 2.5×104 | s-1 | |
| 时间响应 | 上升时间 | 典型值 | 0.9 | ns |
| 下降时间 | 典型值 | 1.7 | ns | |
| 渡越时间分散度 | 典型值 | 0.4 | ns | |
| PMT 工作温度 | -60 | ℃ | ||
| PMT 工作保证电压 | -500 至 -900 | V | ||
| 工作环境温度 | +5 至 +40 | ℃ | ||
| 工作环境湿度 *4 | 低于 80 | % | ||
| 存储温度 | -20 至 +50 | ℃ | ||
| 存储湿度 *4 | 低于 80 | % | ||
*1：在 1300 nm 处
*2：电源电压 = -800 V
*3：避光存储 30 分钟后。
*4：无冷凝。
外形尺寸图（单位：mm）
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