Fiber Amplifiers
Posted on 2007-07-30 as part of the Photonics Spotlight (available as e-mail newsletter!)
Permanent link: https://www.rp-photonics.com/spotlight_2007_07_30.html
Author: Dr. Rüdiger Paschotta, RP Photonics AG, RP Photonics AG
Abstract: Amplified spontaneous emission in a fiber amplifier is often stronger in backward direction, compared to the forward direction. The article explains why that is.
Ref.: encyclopedia articles on amplified spontaneous emission and fiber amplifiers
It is often found that the power carried away by amplified spontaneous emission (ASE) in a fiber amplifier is substantially (often several times) larger for the backward direction (i.e., the direction opposite to that of the pump light) than for the forward direction. This may seem surprising, as the gain (amplification factor) is of course the same for both directions: we are not dealing with a non-reciprocal device.
To clarify this issue, we can begin with locating the asymmetry which is behind the asymmetry of ASE powers. It is of course not the pump propagation direction as such – how should that matter? – but rather the higher excitation density on the side from where the pump light comes.
Now consider the simple example of two subsequent pieces of rare-earth-doped fiber, where the dopant ions (e.g. Er3+) have a quasi-three-level system. The first piece of fiber is strongly pumped so as to exhibit positive net gain, while the second piece is only weakly pumped so that it just reaches the transparency level, i.e., zero net gain. Now see what happens to the ASE:
- Consider first the forward direction, with ASE coming from the first fiber and then going into the second one. As the second fiber has no net gain, it will only weakly increase the ASE power by adding some spontaneous emission.
- For the backward direction, the situation is different: the weakly pumped fiber provides some level of spontaneous emission, which acts as a seed for the more strongly pumped fiber. Here, the contribution of spontaneous emission in the weakly pumped fiber is stronger, since it has to be compared with the weak ASE at the input end, rather than the strong ASE at the output end of the strongly pumped fiber.
In a real fiber amplifier, we of course have a gradual decrease of excitation density, but this will obviously not change the situation altogether.
Even for a four-level fiber amplifier, based e.g. on neodymium, there could be somewhat stronger ASE in backward direction, if the fiber has significant parasitic losses: backward ASE has to travel a shorter distance before being detected. Such effects, however, are usually much less pronounced than the above-mentioned ones in quasi-three-level amplifiers.
This issue alone would suggest that backward pumping is always preferable, and that would be underlined by the remark that the power efficiency (even without ASE) is often better that way (for other reasons). However, the noise figure is usually lower for forward propagation. A good compromise (if that is required) may be bidirectional pumping.
Suppliers
The RP Photonics Buyer's Guide contains 65 suppliers for fiber amplifiers. Among them:
Cycle
Based on Cycle's own femtosecond fiber lasers, the company also offers fiber-based amplifiers (EDFA) with a center wavelength of 1550 nm to 1700 nm. This variant of the SOPRANO-15 is a very attractive solution to amplify the output of beam arrival monitors in synchrotron or FEL facilities, for example. Other custom-made fiber amplifiers are available upon request.
Lumibird
Lumibird manufactures an extensive range of mature and custom-designed optical fiber amplifiers and fiber lasers. High output powers are achieved through the use of double cladding fibers pumped by broad stripe diodes. Several varieties of pumping techniques are used each optimized for specific applications. Lumibird also develops key components for producing unique and innovative light sources.
RPMC Lasers
Serving North America, RPMC offers a wide range of Telcordia grade erbium and ytterbium fiber lasers and amplifiers that are deployed in a wide range of applications, including LIDAR, mapping, 3D scanning and telecommunications. The BKtel suite of lasers and amplifiers are available in a range of wavelengths from 1030 nm to 2054 nm, with average powers up to 40 W, pulsed and CW capabilities, and numerous features, including low noise, compact package size, and a digital control system. Standard and custom solutions available. Let RPMC help you find the right laser today!
AdValue Photonics
AdValue Photonics offers fiber amplifiers for wavelength around 1 μm, 1.5 μm or 2 μm. They are suitable for pulsed or continuous-operation, narrow linewidth or broadband light.
For the 1-μm region, we have compact and yet powerful large mode area fiber amplifier modules, which can deliver more than 120 W average output power.
Active Fiber Systems
AFS’s customized kW average power and multi-mJ pulse energy ultrafast laser systems are based on AFS leading-edge fiber technology. They unite multiple main-amplifier channels using coherent combination, a technology which AFS has matured to an industrial grade. All essential parameters are software-controlled and can be tuned over a wide range, making them an extremely valuable tool for numerous application.
DK Photonics
DK Photonics offers various erbium-doped fiber amplifiers for telecom applications, including compact amplifier modules as well as bench-top instruments with controls and displays.
Ytterbium-doped amplifiers for the 1-μm wavelength region are also available.
TOPTICA Photonics
Our new highly reliable Raman fiber amplifiers (RFA) are based on patented technology. With their high power of up to 30 W, the amplifiers cover the wavelength range from 1120 to 1370 nm that is not accessible by Yb or Er fiber amplifiers. For wavelengths outside this range, please enquire for a custom system.
The RFA is designed using TOPTICA’s high quality engineering excellence and utilizing a stable European & North American supply chain. The all fiber design requires no re-alignment and provides a high degree of stability. The RFA offers a wide tuning range of up to 10 nm, a relative intensity noise <1% r.m.s. (10 Hz – 10 MHz) and excellent long term RMS power stability of less than 0.5% over 100 hours (with a TA pro seed laser).
AMS Technologies
For both C- and L-band operation, AMS Technologies provides a selection of CW and pulsed erbium-(Er-)doped fiber amplifiers (EDFAs) as well as Yb/Er co-doped fiber amplifiers (YEDFAs) in a wide range of configurations and gains:
- 20 and 15 dB miniature size EDFA modules
- high-power, ?27 dBm EDFA modules
- high-speed, pulsed EDFA modules, SM and PM
- single- or multi-port high-power YEDFA modules
- PM YEDFA modules
- 19”, 1U EDFA racks, also PM
- 19”, 1U YEDFA racks, also PM
- 19”, 2U multiport high-power EDFA racks
- Raman fiber amplifier module
MPB Communications
In 1995, MPB Communications provided its first generation of high-power boosters and quantum-limited noise-figure EDFAs for long-haul, unrepeatered telecom systems. MPBC amplification solutions have been adopted by system integrators in the terrestrial, submarine and utilities markets and continue to offer exceptional reliability which power communication backbones worldwide.
Today, our fiber amplifier technology can be found in our line of network-ready telecom solutions, as well as in our extensive portfolio of gain modules, and in our single-frequency Raman fiber amplifiers.
Thorlabs
Thorlabs manufactures erbium (Er)-, ytterbium (Yb)-, and praseodymium (Pr)-doped fiber amplifiers for applications from ultrafast pulse amplification to datacom. Along with these stand-alone benchtop amplifiers, Thorlabs has developed a family of femtosecond lasers utilizing oscillator-amplifier architectures.
Le Verre Fluore
Thanks to their high rare-earth solubility (up to 100,000 ppm) and low phonon energy, LVF fluoride fibers offer dozens of active transitions, enabling a broad range of applications from visible to the mid-infrared, one of which is amplification. For example, LVF praseodymium and thulium doped fibers are used for amplification at 1.3 µm and 1.47 µm respectively. LVF doped fibers for amplification are available as single-mode fiber or double cladding fiber.
Le Verre Fluoré will soon offer laser and amplifier fiber modules. The required fiber will be integrated in a robust housing and connectorized with FC/PC, FC/APC, SMA or custom connectors depending on customer need: this is a plug-and-play module.
Depending on specific needs, modules might include single-mode or multimode splices between fluoride fibers or between silica and fluoride fibers.
This article is a posting of the Photonics Spotlight, authored by Dr. Rüdiger Paschotta. You may link to this page and cite it, because its location is permanent. See also the RP Photonics Encyclopedia.
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