P R O D U C T S
770nm Narrow linewidth laser
Based on high-power, low-noise Er-doped fiber lasers amplification and frequency doubling technology, Precilasers can provide high-power, narrow linewidth laser output with a wavelength ranging from 765 to 798 nm.
Features
- Narrow Linewidth
- Low RIN
- High Power
- Power Stability:<0.75%rms, 3hrs
- Excellent Beam Quality (M² <1.1)
- Never Mode-hop
- High Temperature And Vibration Resistance
Application
- Rb Atom Cooling
- Magic Optical Lattice
- Atom Interferometry
- Atom Clock
Main parameters
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Specification |
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Partnumber |
FL-SF-XXXX-YY-CW(1) |
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Wavelength Range |
765-770nm |
770-785nm |
785-798nm |
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Typical Wavelength |
767nm、770nm |
780nm |
795nm |
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Seed Laser Type |
Fiber DFB Seed Laser(1530-1596nm) |
Fixed External Cavity Diode Laser(FECL,1530-1596nm) |
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Output Power(2) |
>0.2W/2W/6W |
>0.2W/2W/8W/15W |
>0.2W/2W/4W |
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Thermal Tuning Range |
>0.5nm,Never Mode-hop |
>15GHz, Never Mode-hop |
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Output Mode |
PM Fiber Output,FC/APC(Output Power ≤2W)OR Free Space Output(Compatible with all versions) |
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Beam Diameter(3) |
0.7-1.0mm |
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Power Tuning Range |
5-100% |
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Beam Pointing Stability |
<10μrad |
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Linewidth(4)(100us) |
<2kHz/5kHz |
<10kHz/20kHz |
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PER |
linear,>20dB |
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Power Stability |
<0.75%@3hours, RMS |
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Beam Quality |
TEM00,M2<1.1 |
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Fast Frequency Tuning Range |
>3GHz |
>1GHz |
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Fast Frequency Tuning Bandwidth |
>5kHz,PZT Tuning |
>1MHz,Current Tuning |
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AOM Tuning Range (Optional) |
>±5MHz |
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AOM Tuning Bandwidth (Optional) |
>500kHz |
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RIN |
<0.08%(RMS,10Hz-100MHz) |
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Cooling |
Air Cooling/Water Cooling |
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Operating Environment & Power Supply |
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Temperature |
15-30 ℃(Air Cooling) or 15-35 ℃(Water Cooling) |
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Power Supply |
100V-240V, AC, 50/60Hz |
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Communication |
RS422 |
(1)XXXX is the laser center wavelength,YY is the laser power,for a 6W 770nm laser,the partnumberis FL-SF-770-6-CW
(2)If the laser output power ≤2W, the PM fiber output version can be choosed
(3)Beam diameter is only applicable to free space output mode,For PM fiber output mode,the fiber without collimator
(4)Measured by self-hetrodyne method