Ultra-Low Noise Fiber Laser(1064,532,759,780,813nm)

Single Frequency Fiber laser with low Relative Intensity Noise (RIN) have wide application in quantum optics, pumping lasers, lidar, coherent optical communications, high-precision optical sensing, optical measurement, and precision spectroscopy. For example, the laser for trapping atoms in optical lattice demands not only high output power, but also low RIN to reduce the resonance between the lattice and atoms and low frequency noise (FN) to reduce the spatial vibration, which is quite important for the atoms lifetime in the lattice. In the atomic interferometer and atomic clock application, high power laser could lead to more atoms, uniform interaction area and high measurement SNR.

    Main Specification

    Ultra-Low Noise Fiber Laser

    Single Frequency Fiber laser with low Relative Intensity Noise (RIN) have wide application in quantum optics, pumping lasers, lidar, coherent optical communications, high-precision optical sensing, optical measurement, and precision spectroscopy. For example, the laser for trapping atoms in optical lattice demands not only high output power, but also low RIN to reduce the resonance between the lattice and atoms and low frequency noise (FN) to reduce the spatial vibration, which is quite important for the atoms lifetime in the lattice. In the atomic interferometer and atomic clock application, high power laser could lead to more atoms, uniform interaction area and high measurement SNR.

    Fig. 1, Schematic of the low noise fiber laser.
    *The doubler module is equipped with SHG model

     

     

    PreciLasers offers high power low noise 1064 nm and 1550 nm fiber laser with low FN and low RIN seed + low noise fiber amplifier shown in Fig. 1. In Fig. 2, the amplifier will not introduce the extra frequency noise and the linewidth broadening is measured to be less than 1 Hz. The RIN of the amplifier is ultra-low(RIN<-140 dBc/Hz (>5 kHz), RIN integration from 10 Hz-10 MHz <0.03% ). Also, the wavelength could extend to be 1020-1120 nm for Ytterbium-doped fiber amplifier and 1530-1596 nm for Er-doped fiber amplifier. With stable single pass frequency doubling module, the low noise fiber laser wavelength could extend to be 510-556 nm and 765-798 nm . In the process of frequency doubling, the linewidth of the laser is doubled, and the intensity noise (RIN) is only increased by 6 dB, thus inheriting the low noise characteristics of the fundamental frequency light.

     

    Fig. 2, Linewidth broadening test and result

    PreciLasers offers a high-power (up to 130 W), low intensity noise, narrow linewidth highly-reliable 1064 nm fiber laser solution for the optical lattice application.

    Typical relative intensity noise power density spectrum (RIN) * of 90 W FL-SF-1064

    Model FL-SF-1064-130 FL-SF-1064-100 FL-SF-1064-50
    Central Wavelength1 , nm 1064 1064 1064
    Linewidth, kHz < 10 < 10 < 10
    Tuning Range, GHz 10 10 10
    Power after ISO, W >130 >100 >50
    RIN RIN:  -140 dBc/Hz (100 kHz)
    RMS Integration: <0.05% (10Hz-10 MHz)
    RIN:  -140 dBc/Hz (100 kHz)
    RMS Integration: <0.05% (10Hz-10 MHz)
    RIN : -140 dBc/Hz (100 kHz)
    RMS Integration: <0.05% (10Hz-10 MHz)
    Beam Quality TEM00 , M2<1.15 TEM00 , M2<1.15 TEM00 , M2<1.15
    Polarization Linearly Polarized , > 300: 1 Linearly Polarized , > 300: 1 Linearly Polarized , > 300: 1
    P-P, RMS Power Stability <0.5 %@3hrs <0.5 %@3hrs <0.5 %@3hrs
    Cooling Water Cooling Water Cooling Air Cooling/Water Cooling
    Output Connector Space (300*240 mm2) Space (300*240 mm2) Fiber

     

    1: Wavelength could be selected from 1020-1112nm

     

    Key Features:

    • Low Intensity Noise (-140 dBc/Hz @100 kHz)
    • Narrow Linewidth(<10 kHz)
    • Good Beam quality (M² <1.2)
    • High Output Power (up to 100 W)
    • Operation in harsh conditions
    • Full Protection System

    Applications:

    • Optica Lattice
    • Optical Tweezers
    • Optical Traps
    • Pump laser for OPO

     

    With single pass and resonant cavity SHG module, low noise 532 nm laser could be generated with output power up to 30 W, which has been applied in optical lattice application.

    Typical 10 W 532 nm laser RIN spectrum

    Model
    FL-SF-532-10(Single Pass SHG)
    FL-SF-532-30(Resonant Cavity SHG)
    Central Wavelength1 , nm
    532
    532
    Linewidth, kHz
    < 20
    < 20
    Tuning Range, GHz
    20
    20
    Output Power, W
    10
    30
    RIN
    RIN:  -130 dBc/Hz (100 kHz)
    RMS Integration: <0.05%(10Hz-10 MHz)
    RIN:  -130 dBc/Hz (100 kHz)
    RMS Integration: <0.05% (10Hz-10 MHz)
    Beam Quality
    TEM00 , M2<1.2
    TEM00 , M2<1.1
    Polarization
    Linearly Polarized , > 100: 1
    Linearly Polarized , > 100: 1
     Power Stability
    <0.5 %@3hrs
    <0.5 %@3hrs
    Cooling
    Air Cooling/Water Cooling
    Air Cooling/Water Cooling

     

    1 Central Wavelength could be selected from 510-540 nm  

     

    Key Features:

    • Narrow Linewidth<20 kHz
    • Low Intensity Noise (-130 dBc/Hz @ 100 kHz)
    • High Power (up to 30W @ LN-YFA-SHG)
    • Good Beam Quality (M² <1.2)
    • Linearly Polarize
    • Active Power Stability

     

    759/813nm Ultra-Noise Single Frequency Laser

    FL-SF-759-XX-CW FL-SF-813-XX-CW

     

    PreciLasers offers a high-power, low intensity noise, narrow linewidth highly reliable 759/813nm fiber laser solution (FL-SF-759-2-CW, FL-SF-813-4-CW) for the magic-wavelength optical for Yb/Sr atomic clock.

     

    • Narrow Linewidth<20 kHz
    • Low intensity Noise (RIN -140 dBc/Hz @ 100 kHz)
    • High output power (2W@759nm 10W@ 813nm)
    • Excellent beam quality (M2 <1.1)
    • Wavelength Tunable and high feedback bandwidth


     

    Model FL-SF-759-XX-CW  
    FL-SF-813-XX-CW
    Central Wavelength1,nm 759 813
    Linewidth(100us integration),kHz < 50 < 20
    Output Power,W >2 >10
    Feedback Bandwidth,MHz >1MHz
    Tuning Range,GHz >80GHz
    RIN RMS Integration:<0.05% (10Hz-10 MHz)
    Beam Quality TEM00,M2<1.1
    Polarization Linearly Polarized,> 300:1
    RMS Power Stability <0.2%@8h
    Cooling Air Cooling/Water Cooling

    1:Wavelength could be selected from 614-1000nm

    PreciLasers offers a high-power (up to 15 W), low intensity noise, narrow linewidth highly-reliable 1550 nm fiber laser solution for the coherent detecting, precision measurement physics application.

    Model
    FL-SF-1550-15
    Central Wavelength1 , nm
    1550
    Linewidth, kHz (250us)
    < 10
    Tuning Range, GHz
    >10 
    Output Power, W
    >15
    RIN
    RIN: < -140 dBc/Hz (100 kHz)
    RMS Integration: <0.05% (10Hz-10 MHz)
    Beam Quality
    TEM00 , M2<1.2
    Polarization
    Linearly Polarization , > 100: 1
    RMS Power Stability
    <0.5 %@2hrs
    Cooling
    Air Cooling/Water Cooling

     

     

    1: Central Wavelength could be selected from1530-1580 nm

    Key Features:

    • Low Intensity Noise (-140 dBc/Hz @100 kHz)
    • Narrow Linewidth(<2 kHz)
    • Good Beam quality (M² <1.1)
    • High Power (up to 15 W)
    • Operation in harsh conditions
    • Full Protection System

    Applications:

    • Precision Measurement
    • Coherent Detecting
    • Fundamental Light for Atom Cooling

     

    In order to satisfy the Rb atomic interferometer and other applications, PreciLasers have developed 780 nm laser with the maximum power of 10 W by utilizing the frequency doubling technology for Rb atom cooling / detection, magic wavelength optical lattice and so on. Due to its excellent environmental adaptability such as portability, low drift and anti-vibration, FL-SF-780 nm has been used in the field experiment of Rb atomic interferometer and has completed the several months’ operation for the frequency stabilization of saturated absorption spectrum.

     

     

    Model
    FL-SF-780-5
    FL-SF-780-2.5
    Central Wavelength1 , nm
    780
    780
    Linewidth   ,  kHz 
    < 20
    <20
    Tuning Range, GHz
    20
    20
    Output Power
    >7
    >2.5
    RIN
    RMS Integration: <0.05% (10Hz-10 MHz)
    RMSIntegration: <0.05% (10Hz-10 MHz)
    Beam Quality
    TEM00 , M2<1.1
    TEM00 , M2<1.1
    Polarization
    Linearly Polarized , > 100: 1
    Linearly Polarized , > 100: 1
     RMS Power Stability
    <0.5 %@3hrs
    <0.5 %@3hrs
    Cooling
    Air Cooling/Water Cooling
    Air Cooling/Water Cooling

     

     

    1: Central Wavelength could be selected from 765-795 nm

    Key Features:

    • Narrow Linewidth <200 Hz
    • Low RIN (RIN <-130 dBc/Hz @ 100 kHz)
    • High Output Power (10 W)
    • Good Beam Quality (M²  <1.1)
    • Tunable Wavelength
    • Active Power Stability

    Applications:

    • Rb atom cooling
    • Optical Lattice
    • Rb atom interferometry

     

    Applications

    Key Features:

    • Low Intensity Noise (-140 dBc/Hz @100 kHz)
    • Narrow Linewidth(<10 kHz)
    • Good Beam quality (M² <1.2)
    • High Output Power (up to 100 W)
    • Operation in harsh conditions
    • Full Protection System 

    Applications:

    • Optica Lattice
    • Optical Tweezers
    • Optical Traps
    • Pump laser for OPO 

    Size

    1064nm 50w Ultra-Low Noise Fiber Laser-Air Cooling 1064nm 50w Ultra-Low Noise Fiber Laser-Air Cooling
    1064nm 50w Ultra-Low Noise Fiber Laser-Water Cooling 1064nm 50w Ultra-Low Noise Fiber Laser-Water Cooling
    1064nm 100W Ultra-Low Noise Fiber Laser 1064nm 100W Ultra-Low Noise Fiber Laser
    532nm 10w Ultra-Low Noise Fiber Laser-Air Cooling 532nm 10w Ultra-Low Noise Fiber Laser-Air Cooling
    532nm 10w Ultra-Low Noise Fiber Laser-Water Cooling 532nm 10w Ultra-Low Noise Fiber Laser-Water Cooling
    532nm 35w Ultra-Low Noise Fiber Laser 532nm 35w Ultra-Low Noise Fiber Laser
    532nm 35w Ultra-Low Noise Fiber Laser 532nm 35w Ultra-Low Noise Fiber Laser
    1550nm 15w Ultra-Low Noise Fiber Laser 1550nm 15w Ultra-Low Noise Fiber Laser