Ultra-Low Noise Fiber Laser

Short Description:

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.


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The product description

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.

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Erbium group 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. 

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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.

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

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

Technical indicators

Model

LN-YFA-1064-130

LN-YFA-1064-100

LN-YFA-1064-50

Central Wavelength¹, nm

1064

1064

1064

Linewidth, kHz

< 10

< 10

< 10

Tuning Range,GHz

10

10

                 10

Power afterISO, W

>130

>100

>50

RIN

RIN: -140 dBc/Hz (100 kHz)

RMS Integration: <0.0(10Hz-10 MHz)

RIN: -140 dBc/Hz (100 kHz)

RMS Integration: <0.0(10Hz-10 MHz)

RIN: -140 dBc/Hz (100 kHz)

RMS Integration: <0.0(10Hz-10 MHz)

Beam Quality

TEMₒₒ , M² <1.15

TEMₒₒ , M² <1.15

TEMₒₒ , 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

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.

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Typical 10 W 532 nm laser RIN spectrum

Key Features

● Narrow Linewidth<20 kHz

● Low Intensity Noise (-130 dBc/ Hz @ 100 kHz)

● High Power (up to 30W @ LNYFA-SHG)

● Good Beam Quality (M² <1.2)

● Linearly Polarize

● Active Power Stability 

Applications

● Optica Lattice

● Optical Tweezers

● Pump laser for Ti: Sapphir laser

Technical indicators

Model

LN-YFA-D-532-10(Single Pass SHG)

LN-YFA-D-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

TEMₒₒ , M² <1.2

TEMₒₒ , M² <1.1

Polarization

Linearly Polarized , > 100: 1

Linearly Polarized , > 100: 1

P-P, 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 510-540 nm


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