CW Fiber Lasers

This advanced fiber laser module is designed for ultra-narrow linewidth single-frequency laser output with extraordinary noise control. It employs patented technology to eliminate standing wave space hole burning, ensuring ultra-stable and ultra-narrow linewidth performance. The all-fiber design, coupled with polarization control ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 0.1 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.1
Spectral Linewidth: -- nm
Connet CoSF-R optimized traveling wave cavity ultra-narrow linewidth single-frequency fiber laser is a low-noise ultra-narrow linewidth fiber laser independently developed by patented technology. CoSF-R single-frequency fiber laser uses a unique \"optimized traveling wave cavity\" The design eliminates the standing wave space hole ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 10 W
Output Mode: N/A
Beam Quality (M^2): 1.1
Spectral Linewidth: nm
Connet CoSF-R optimized traveling wave cavity ultra-narrow linewidth single-frequency fiber laser is a low-noise ultra-narrow linewidth fiber laser independently developed by patented technology. CoSF-R single-frequency fiber laser uses a unique "optimized traveling wave cavity" The design eliminates the standing wave space hole ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 0.1 W
Output Mode: Continuous Wave (CW)
Beam Quality (M^2): 1.1
Spectral Linewidth: -- nm
The CoSF-R-YB-B-HP Ultra-narrow Linewidth Single Frequency Fiber Laser by Connet is a low-noise, ultra-narrow linewidth fiber laser designed using patented technology. It features the optimized traveling wave cavity design, which eliminates standing wave space hole burning and ensures single longitudinal mode output. With ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 100 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.3
Spectral Linewidth: -- nm
This remarkable fiber laser, independently developed using patented technology, boasts an ultra-narrow linewidth, making it ideal for demanding applications in scientific research and beyond. The CoSF-R-TM-B-LP utilizes an innovative "optimized traveling wave cavity" design, eliminating the standing wave space hole burning ...

Specifications

Center Wavelength: 1900-2090 nm
Output Power: 0.1 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.1
Spectral Linewidth: -- nm
The CoSF-R-TM-B-MP Ultra-narrow Linewidth Single Frequency Fiber Laser by Connet is a high-performance fiber laser designed for applications requiring ultra-narrow linewidth and low noise. With its stable single-frequency, single-polarization output and benchtop all-in-one package, it provides exceptional performance in various ...

Specifications

Center Wavelength: 1900-2090 nm
Output Power: 5 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.1
Spectral Linewidth: -- nm
Introducing the Connet CoSF-R: Optimized Traveling Wave Cavity Ultra-Narrow Linewidth Single-Frequency Fiber Laser. This cutting-edge fiber laser represents a breakthrough in low-noise technology, delivering exceptional performance and reliability, thanks to our patented innovations. At the heart of the CoSF-R single-frequency fiber ...

Specifications

Center Wavelength: 1090-2090 nm
Output Power: 50 W
Output Mode: Continuous Wave (CW), Modulated, Single Longitudinal Mode
Beam Quality (M^2): 1.3
Spectral Linewidth: -- nm
Connet CoSF-R optimized traveling wave cavity ultra-narrow linewidth single-frequency fiber laser is a low-noise ultra-narrow linewidth fiber laser independently developed by patented technology. CoSF-R single-frequency fiber laser uses a unique "optimized traveling wave cavity". The design eliminates the standing wave space hole ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 0.1 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: -- nm
Connet CoSF-R optimized traveling wave cavity ultra-narrow linewidth single-frequency fiber laser is a low-noise ultra-narrow linewidth fiber laser independently developed by patented technology. CoSF-R single frequency fiber laser uses a unique "optimized traveling wave cavity". The design eliminates the standing wave space hole ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 0.1 W
Output Mode: Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.1
Spectral Linewidth: -- nm
Connet CoSF-R optimized traveling wave cavity ultra-narrow linewidth single-frequency fiber laser is a low-noise ultra-narrow linewidth fiber laser independently developed by patented technology. CoSF-R single-frequency fiber laser uses a unique "optimized traveling wave cavity". The design eliminates the standing wave space hole ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 5 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.1
Spectral Linewidth: -- nm
Connet CoSF-R optimized traveling wave cavity ultra-narrow linewidth single-frequency fiber laser is a low-noise ultra-narrow linewidth fiber laser independently developed by patented technology. CoSF-R single frequency fiber laser uses a unique "optimized traveling wave cavity". The design eliminates the standing wave space hole ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 20 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.3
Spectral Linewidth: -- nm
The Connet CoSF-D-YB-M Single Frequency Fiber Laser Module represents a breakthrough in laser technology, harnessing the power of Distributed Feedback Bragg Grating (DFB) to deliver a low-noise, stable single-frequency laser output. Boasting independent intellectual property rights, this module guarantees single longitudinal mode, ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 50 W
Output Mode: Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: 0.01 nm
Introducing the Connet CoSF-D, an advanced, low-noise, Single Frequency Fiber Laser engineered with state-of-the-art Distributed Feedback Bragg Grating (DFB) technology. This device is not only a product of independent intellectual property rights, but it also delivers an impeccably stable, single-frequency laser output characterized ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 0.02 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: -- nm
Connet CoSF-D is a low-noise Single Frequency Fiber Laser based on Distributed Feedback Bragg Grating (DFB) technology. It has independent intellectual property rights and achieves a stable single frequency laser output with single longitudinal mode, linear polarization, and narrow linewidth. CoSF-D has very low phase ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 10 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: -- nm
Connet CoSF-D is a low-noise Single Frequency Fiber Laser based on Distributed Feedback Bragg Grating (DFB) technology. It has independent intellectual property rights and achieves a stable single frequency laser output with single longitudinal mode, linear polarization, and narrow linewidth. CoSF-D has very low phase ...

Specifications

Center Wavelength: 1010-1120 nm
Output Power: 100 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.2
Spectral Linewidth: -- nm
This cutting-edge fiber laser module, built upon Distributed Feedback Bragg Grating (DFB) technology, delivers exceptional performance with an emphasis on stability and low noise. Ideal for scientific research and advanced optical systems, it provides a stable single-frequency laser output with single longitudinal mode, linear ...

Specifications

Center Wavelength: 1015 nm
Output Power: 0.01 W
Output Mode: Continuous Wave (CW), Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: -- nm
The CoSF-D-RS-ER-M is a low-noise Single Frequency fiber laser module based on Distributed Feedback Bragg Grating (DFB) technology. It delivers a stable single-frequency laser output with single longitudinal mode, linear polarization, and narrow linewidth. With very low phase and frequency noise, as well as low relative intensity ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 0.05 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: nm
The CoSF-D-RS-EY-M Low RIN Single Frequency Fiber Laser Module by Connet is a high-performance laser module based on Distributed Feedback Bragg Grating (DFB) technology. It offers stable single-frequency, single-polarization output with low phase noise, frequency noise, and relative intensity noise (RIN). With its narrow linewidth ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 0.1 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: -- nm
The Connet CoSF-D-ER-M is an exceptional Single Frequency Fiber Laser Module built upon Distributed Feedback Bragg Grating (DFB) technology, showcasing independent intellectual property rights. This module produces a stable single-frequency laser output with single longitudinal mode, linear polarization, and an ultra-narrow ...

Specifications

Center Wavelength: 1530-1572 nm
Output Power: 0.1 W
Output Mode: Continuous Wave (CW), Single Frequency, Single Longitudinal Mode
Beam Quality (M^2): 1.05
Spectral Linewidth: 0.01 nm

Frequently Asked Questions

In fiber lasers the active gain medium is an optical fiber doped with rare elements. A pump source, typically a laser diode is coupled into the core of a doped optical fiber where stimulated emission occurs. Doping the optical fiber with rare earth element such as ytterbium, erbium, holmium, etc. creates the medium where population inversion is enabled and where light amplification by stimulated emission occurs. The light generated is then amplified upon thousands of reflections off the nodes of a fiber Bragg grating which acts as the “cavity mirrors” similar to that of a traditional free-space laser. Fiber Bragg grating acts as the optical filter allowing reflection of only specific modes in the laser cavity.

Fiber Bragg grating (FBG) is a periodic structure (segment of periodic variation of optical index) created inside the fiber core that causes the light to diffract, reflect or transmit based on the phase and wavelength. These periodic structures applied to the core of the optical fibers are typically a few millimeters or centimeters long with a period that is on the order of a wavelength or hundreds of nanometers. FBG acts as an effective optical filter in fiber optic devices including fiber lasers.

Single-mode and multimode fibers are both used in designing and producing fiber lasers. However, single-mode fiber lasers tend to be more efficient and have a higher beam quality. Not to mention that single-mode fiber lasers do not suffer from mode hopping. In particular, ultra-narrow linewidth fiber lasers are constructed of single mode fibers doped with rare elements.

Supercontinuum generation exploits the nonlinear effects of certain optical media. Therefore, the fibers used in supercontinuum lasers are made of strongly nonlinear materials. These fibers will also need to provide good transmission throughout the entire amplification bandwidth. Fluoride based optical fibers are often used in supercontinuum fiber lasers.

While free-space lasers can last up to 15 years, fiber lasers enjoy a much longer lifespan which could reach 45 years or the equivalent of 100,000 hours of operation. This longevity is thanks to the compact sealed design that has fully integrated cavity without any free space intracavity optics that exists in other DPSS lasers.

Owing to their strong power output, CW fiber lasers are widely used in laser machining applications such as laser cutting, drilling, marking, and welding. They are also used in many research areas to perform precision measurements, spectroscopy, laser pumping, and optical testing.

You are probably referring to the external fiber that couples the laser output to other devices. Typically, the fiber length ranges between 0.5 and 1m in fiber lasers. However, the fiber end is attached to a connector which makes it very easy and simple to connect to other fibers if needed. The length of the optical fiber inside the cavity is fixed and determines the amplification gain.

Some units offer a tunable wavelength feature which allows the user to select a wavelength out of a few options. Supercontinuum fiber lasers can be used along with a bandpass filter to filter out the desired wavelength as well.

Many suppliers of CW fiber lasers offer models with both linear and random polarization. Less frequently, circular polarization is also an available option on market from many suppliers.

There are 248 different CW Fiber Lasers from suppliers and manufacturers listed in this category. In just a few clicks you can compare different CW Fiber Lasers with each other and get an accurate quote based on your needs and specifications. Please note that the prices of CW Fiber Lasers vary significantly for different products based on various factors including technical parameters, features, brand name, etc. Please contact suppliers directly to inquire about the details and accurate pricing information for any product model. Simply navigate to the product page of interest and use the orange button to directly reach out to the respective supplier with one click.

Did You know?

The first fiber laser was operated in a Nd-doped glass fiber and was transversely pumped by coiling the fiber around a flash lamp. It consisted of a diode pump laser, and a wavelength selective coupler that allowed the pump wavelength to enter the fiber transmission system without disturbing the signal. Fiber lasers have potential applications in production of ultra-short pulses as well as in distance communications where optically transmitted signal can obtain a direct optical "boost" or amplification as it travels from one continent to another. This supersedes the earlier technique of converting the optical signal to an electrical one, amplifying it, and then re-inserting it into the fiber for further optical transmission.