680-2300nm波长可调谐调Q脉冲激光器
波长:680-2300nm
能量:至11mJ,重频至100Hz,10-15 cm-1线宽
应用:
•红外分光光度法
•腔衰荡光谱
•气体光谱
•单分子振动光谱
•扫描近场光学显微镜
•遥感
- 基本信息
- 文档
- 相关产品
1380-4500 nm波长可调谐红外调Q激光器——Q-TUNE-IR
- Seamless laser and Optical Parametric Oscillator (OPO) integration.
- Remote control via PC.
- Turnkey performance due to water-free pump laser design.
- Guaranteed > 2 Gshot pump diode lifetime.
- Microprocessor controlled operation with self-optimization, self-calibration capability.
- Hands-free, automated tuning from 1380 to 4500 nm.
- >17 mJ pulse energy at the peak of tuning curve.
- <10 cm-1 linewidth (broadband ~200 cm-1 version is available).
- Up to 20 Hz pulse repetition rate.
- Internal or external triggering modes.
- Separate output port for access to pump laser beam.
- Low power consumption – from 50 to 100 W depending on model.
- Can be powered from +12 VDC or +28 VDC source.
Q-TUNE-IR——波长可调(1380-4500 nm)
简介
Q-TUNE-IR is a high peak power coherent light source for infrared spectroscopy, infrared spectrophotometry, metrology, single molecule vibrational microscopy, remote sensing.
Q-TUNE-IR employs Optical Parametric Oscillator (OPO) to produce tunable wavelength in 1380-4500 nm range with linewidth of less than 10 cm-1. Broadband version with linewidth up to 200 cm-1 is available by request.
There two types of OPO coatings available. The first one is optimized for maximum transmission in 2.1 µm range (option -TC1). The second one is optimized for maximum transmission in 3.3 – 3.9 µm range (option -TC2). See tuning curves in datasheet for comparison.
QLI breakthrough water-free laser crystal pumping technology allows to produce high quality laser beam with up to 100 mJ pulse energy. There are no chillers or bulky power supplies that one needs fit under the table. All laser electronics are integrated into housing of the Q-TUNE-IR and the only external module is mains adapter that provides 12 or 28 VDC, 50-150 W power (depending on model).
Q-TUNE-IR can be configured with dedicated QLI pump laser for optimal match to your application. If high pulse energy is required, Q-TUNE-IR can be configured for 6 mJ output @ 3300 nm at 10 Hz pulse repetition rate. Cost effective solution is also available, Q-TUNE-IR-C10 can be configured for 10 Hz operation with 2 mJ @ 3300 nm pulse energy.
Both pump laser and OPO are controlled trough single Ethernet port via build-in web-server. There is no need to install control software any computer or even cell phone with modern web-browser will be able to control Q-TUNE-IR. API is also provided for integration with user devices.
In addition to tunable wavelength output, the Q-TUNE-IR provides a extra port for access to the pump laser beam.
Optional extensions available by request:
• Compact spectrometer for OPO wavelength and linewidth monitoring.
• Build-in broadband attenuator for pulse energy control.
• Air purging for removal of water vapor absorption lines and improved lifetime of optics.
应用
• Infrared spectrophotometry
• Cavity ring-down spectroscopy
• Gas spectroscopy
• Single molecule vibrational spectroscopy
• Scanning near-field optical microscopy
• Remote sensing
参数 1)
Model |
Q-TUNE-IR |
||||
-C10 |
-C100 |
-E33 |
-F10 |
-F20 |
|
Wavelength range, nm 2) |
1380-4500 nm |
||||
Pulse repetition rate 3) |
10 Hz |
100 Hz |
33 Hz |
10 Hz |
20 Hz |
Pulse energy 4) |
|||||
-TC1 |
≥1.5 mJ |
≥1 mJ |
≥3 mJ |
≥5 mJ |
≥4 mJ |
-TC2 |
≥2 mJ |
≥1.3 mJ |
≥4 mJ |
≥6 mJ |
≥5 mJ |
Linewidth 5) |
<10 cm-1 |
||||
Pulse duration 6) |
3-4 ns typical |
||||
Pulse-to-pulse stability 7) |
< 4.5 % RMS |
||||
Power drift 8) |
± 3.0 % |
||||
Polarization |
horizontal, linear |
||||
Typical beam diameter 9) |
3 mm |
5 mm |
6 mm |
||
Typical beam divergence 10) |
< 7 mrad |
< 5 mrad |
|||
Jitter 11) |
< 0.5 ns RMS |
||||
Pump laser output |
|||||
Max pulse energy at fundamental wavelength 12) |
20 mJ |
14 mJ |
50 mJ |
80 mJ |
60 mJ |
Dimensions |
|||||
Laser head |
390× 620 × 153 mm3 (W×L×H) |
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Power adapter |
192 × 178 × 46 mm3 (W×L×H) 13) 14) |
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Air purging unit |
422 × 460 × 89 mm3 (W×L×H) 15) |
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Operating requirements |
|||||
Cooling requirements |
Air cooled (water-free) |
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Ambient temperature |
15 – 30 ºC |
||||
Relative humidity (non-condensing) |
10 – 80 % |
||||
Mains voltage |
90-230 VAC, single phase, 47-63 Hz 14) |
||||
Average power consumption |
< 50 W |
<150 W |
<80 W |
< 120 W |
1. Due to continuous improvements all specifications are subject to change. Unless stated otherwise all specifications are measured at 3300 nm and max pulse repetition rate. The parameters marked typical are not specifications. They are indications of typical performance and will vary with each unit we manufacture.
2. There are two wavelengths at the exit port in 1800 – 2500 nm range corresponding to signal and idler of OPO. Configurations for single wavelength output and/or no gap in 2800-2900 nm range are available. Please inquire for details.
3. Factory-set pulse repetition rate in internal triggering mode. Pulse repetition rate can be divided-down to 1 Hz.
4. Pulse energy @3300 nm. See tuning curves for typical pulse energies at other wavelengths.
5. Broadband version is available, with linewidth up to 200 cm-1. Please inquire for details.
6. FWHM level at 1550 nm, measured with 350 ps rise time photodiode.
7. Measured during 30 seconds operation after warm-up.
8. Over 8 hour period after 20 minutes of warm-up, when ambient temperature variation is less than ±2 °C. Power value is calculated every 1 second.
9. Beam diameter is measured 20 cm from laser output at the 1/e2 level at 1550 nm.
10. Full angle measured at 1550 nm at the 1/e2 level.
11. In respect to falling edge of pump diode triggering pulse.
12. Laser pulse energy is optimized for OPO pumping may differ from stand-alone laser specifications indicated here.
13. Power adapter size depends of Q-TUNE-IR model.
14. Laser can be powered from appropriate 12 or 28 VDC power source, depending on model. Please inquire for details.
15. Air purging unit is supplied with integrated power adapter.
Fergie零像差光谱仪
美国Princeton Instruments公司是科学级CCD相机和光谱仪的领先者,经过数十载技术创新,推出首台全焦面零像差成像光谱仪Fergie。它采用内置高灵敏度科学级CCD芯片的全集成式紧凑设计,最简化光谱实验硬件设置。零像差不仅最大化提高了光谱分辨率,也让成像和光谱的切换轻松自如。辅以Fergie CUBEs模块化设计,无论是吸收、透射光谱,或是荧光、拉曼光谱,光路搭建都变得易如反掌。