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Double-clad Fibers

Author: the photonics expert

Definition: optical fibers with different waveguide structures for pump and signal light

Alternative terms: double cladding fibers, cladding-pumped fibers

More general term: rare-earth-doped fibers

Category: article belongs to category fiber optics and waveguides fiber optics and waveguides

DOI: 10.61835/tl9   Cite the article: BibTex plain textHTML

The technology of double-clad fibers is important in the area of active fiber optics, particularly for high-power fiber lasers and amplifiers. Only with double-clad fibers, very high output powers of fiber-based amplifiers and lasers are possible.

For the invention of double-clad fiber designs, one only had a choice between the following two approaches:

  • One could realize fiber lasers or amplifiers based on an active single-mode fiber. That way, one can generate a diffraction-limited output, but it restricts the pump sources to those with diffraction-limited beam quality and thus normally to those with low power.
  • When using a highly multimode fiber, one can easily launch much higher pump power and consequently achieve much higher output powers. However, with a multimode core one usually obtains a quite poor beam quality. A high beam quality, however, is highly desirable for many applications.

That dilemma has been resolved with the invention of double-clad fiber designs, which allow cladding pumping of fiber devices. Here, the laser light propagates in a single-mode (or multimode) core, which is surrounded by an inner cladding in which the pump light propagates. Only the core (or sometimes a ring around the core [4]) is rare-earth-doped. The pump light is restricted to the inner cladding (called pump cladding) by an outer cladding with lower refractive index, and also partly propagates in the single-mode core, where it can be absorbed by the laser-active ions. The pump cladding has a significantly larger area (compared with that of the core) and typically a much higher numerical aperture, so that it can support a large number of propagation modes, allowing the efficient launching of pump light from high-power laser diodes (e.g. beam-shaped high-power diode bars), despite their poor beam quality. Fig. 1 shows the example of a simple high-power fiber amplifier.

cladding-pumped fiber amplifier
Figure 1: Cladding-pumped fiber amplifier based on a double-clad fiber with free-space coupling.

The signal light is launched into the doped core, while the pump light is launched into the inner cladding. The core is D-shaped for more efficient pump absorption. Industrial devices typically contain fiber-optic pump combiners for better robustness and stability.

The pump light does not necessarily need to be injected into the fiber ends, as shown in Figure 1. It is also possible to use side pumping techniques, where access to the fiber ends is not required for pumping. For example, coated V grooves cut into the inner cladding can be used to reflect pump light into the inner cladding. In other cases, one exploits coupling of pump light from additional pump fibers wound around the active fiber.

Double-clad Fiber Designs

There are various different designs of double-clad fibers. Figure 2 shows the fiber cross-sections for the most important design types.

double-clad fiber designs
Figure 2: Various designs of double-clad fibers. The fiber core is shown in blue, the inner cladding in light gray, and the outer cladding in dark gray. An additional polymer coating, as often used, is not shown.

The simplest kind of design has a circular pump cladding and a centered core (first design in Figure 2). The actual glass fiber may not differ at all from a normal core-pumped fiber, except that one uses a suitable coating with sufficiently low refractive index (e.g. fluorinated acrylate) to obtain a sufficiently large numerical aperture of the pump cladding. This kind of double-clad fiber is thus easy to make and use. However, but such fibers with a radially symmetric design there are propagation modes of the inner cladding (related to helical rays) which have hardly any overlap with the core, so that some significant part of the pump light exhibits incomplete absorption. Figure 3 shows an example case with a numerical simulation, done with the software RP Fiber Power. This shows that the pump intensity distribution develops a “hole” in the core region. The remaining pump light exhibits quite incomplete absorption, even over longer distances. As a result, the gain and power efficiency are compromised. Only to a limited extent, this problem can be solved by strongly coiling the fiber.

amplitude distribution along the fiber
Figure 3: Amplitude distribution of pump light along a double-clad fiber with a circular pump cladding. The granular structure results from simulating with a monochromatic source; in reality, the structure is washed out by the polychromatic nature of the pump light.

The problem of strongly mode-dependent pump absorption can be mitigated by using a modified fiber design with a lower symmetry. Examples are designs with an off-centered core or a non-circular (e.g. elliptical, D-shaped or rectangular) inner cladding. Such pump claddings are also often better matching the properties of pump sources such as beam-shaped diode bars. However, if the overall fiber (not only the cladding) has a non-circular shape, this may cause problems when splicing the fibers. Splicing is also more difficult if the fibers have off-centered cores, since those then need to be properly aligned.

air-clad photonic crystal fiber
Figure 4: Structure of a photonic crystal fiber with an air cladding.

In some cases, there is another undoped cladding of relatively small diameter around the fiber core [13] which is used to optimize the guided mode properties.

Double-clad fibers can also be made as photonic crystal fibers as shown in Figure 4. Here, the multimode pump core is suspended by very thin struts in the air cladding, through which the pump light cannot escape. (Note that pump leakage resulting from an imperfect air cladding may damage the fiber coating.) Such a structure can have a very high numerical aperture of at least 0.6 for the pump light, which further reduces the requirements concerning the brightness of the pump source. The thickness of the struts can be chosen such that at the same time one achieves good mechanical stability, high thermal conductivity (resulting in a not dramatically increased temperature of the fiber core during high power operation), and minimal pump losses. Another advantage of this type of fiber is that pump light is kept away from the protective polymer coating, avoiding any damage by absorbed pump light. The guidance of light in the core is achieved as in other photonic crystal fibers.

Triple-clad Fibers

There are triple-clad fibers, having one more undoped cladding around the pump cladding. While such fibers overall behave similar to double-clad fibers, that refinement can bring some advantages. In particular, one may achieve a smaller area ratio between pump cladding and core, which is desirable in some cases.

It is possible to have an all-glass double-clad waveguide structure, plus a polymeric coating which then has no optical function. It is then also more easily possible to use a pump cladding of modified shape, for example a rectangular or octagonal shape, while keeping the overall cross-section circular.

For more details, see the article on triple-clad fibers.

Fabrication Methods and Parameters of Double-clad Fibers

In many cases, a double-clad fiber is basically made in the same way as an ordinary core-pumped fiber, except that one uses a polymer coating which is suitable for minimizing light losses and handling high optical powers. In addition, one may modify the shape of the pump cladding, for example using a D shape where

In many cases, the core and inner cladding of a double-clad fiber are similar to those of a normal core-pumped fiber, except that in addition there is the lower-index outer cladding. If the inner cladding is made of silica, the outer cladding may consist of fluorine-doped silica. The numerical aperture for the inner cladding can then be e.g. ≈ 0.28, which is sufficient in many cases but not ideal. Larger values are possible with polymer outer claddings, but these cannot tolerate very high temperatures and may introduce higher propagation losses for the pump light. Therefore, all-glass designs are often preferred for high output powers.

One may use triple-clad designs, but photonic crystal fiber designs such as that shown in Figures 4 and 5 also provide all-glass solutions, and that with very high NA of the inner cladding.

rod fiber
Figure 5: Microscope picture of the end of a photonic crystal rod fiber. The design is similar to that shown in Figure 4, but the core is rather large and polarization-maintaining guidance is achieved with two stress rods. The photograph has been kindly provided by NKT Photonics.

Besides the properties of the fiber core, the ratio of the areas of inner cladding and core is an important parameter. That area ratio should not be too large – for too reasons:

  • The pump absorption becomes weak, so that one requires a longer length of fiber. That is particularly problematic 11 runs into problems with fibers nonlinearities, e.g. when amplifying intense signal pulses.
  • The pump intensity in the core gets smaller, resulting in low excitation levels which can also compromise the power efficiency.

Area ratios of the order of 100–1000 are common. Pump sources with improved brightness allow the use of fibers with a smaller area ratio (possibly made a triple-clad fibers), and thus also with a smaller length, which also reduces the impact of various types of nonlinearities.

A smaller area ratio may often be advantageous. For achieving this, one can either increase the core size or decrease the size of the pump cladding. While the former method is limited by the demand of single-mode performance, the latter is not easy to realize:

  • One may simply draw the whole glass fiber to a smaller diameter, but working with non-standard diameters causes issues like reduced mechanical stability and compatibility with other fiber-optic components such as fiber-optic pump combiners.
  • One may keep the overall fiber diameter but introduce an additional glass cladding around the pump cladding. That is the previously mentioned triple-clad method. Here, the numerical aperture of the pump cladding is more limited, since the refractive index contrast between two glass compositions is smaller than that between glass and a polymer.

For those reasons, it is common to use either a double-fiber with standard cladding diameter of 125 μm or (less frequently) a triple-clad design, where the pump cladding may be smaller.

Erbium-doped double-clad fibers would normally be difficult to use, since the low absorption cross-section combined with the limited realistic doping concentration of erbium in silicate glasses would lead to quite poor pump absorption. A good solution is ytterbium co-doping – see the article on erbium-ytterbium-doped laser gain media.

Coupling Light into Double-clad Fibers

In research setups, light is often coupled from free space into a double-clad fiber, as shown in Figure 1. For industrial lasers, however, this approach is not sufficient stable and robust. They should be based on an all-fiber setup e.g. as shown in Figure 6, where fiber-coupled pump laser diodes are directly connected to the active fiber via some passive transport fibers, avoiding any air spaces in the beam path. One then requires fiber-optic pump combiners (or pump couplers), i.e., special types of fiber couplers used for interfacing to the active fiber.

all-fiber setup of high-power fiber laser
Figure 6: Set up of a high-power fiber laser. Light from eight fiber-coupled pump diodes is combined with two pump fiber combiners and sent into the active fiber from both directions. Fiber Bragg gratings are used to form the laser resonator.

Various designs of high-power pump combiners have been developed. They are partly offered by the manufacturers of double-clad fibers, and partly by other more specialized manufacturers. The advances in the development of fiber pump combiners with high power handling capability, preservation of radiance, compatibility to certain double-clad fibers etc. have been an important contribution to the progress on high-power fiber devices.


Double-clad fibers are extensively used for cladding-pumped high-power fiber lasers and amplifiers. Such devices can have a fairly high power conversion efficiency (sometimes above 80%) combined with a high beam quality. As the beam quality of the output can be diffraction-limited whereas that of the pump can be poor, the brightness of the laser or amplifier output can be much higher than that of the pump source. Particularly if this increase in brightness is essential for an application, the cladding-pumped fiber laser may be called a brightness converter.

Typical Problems with Double-clad Fibers

It has already been mentioned above that rather incomplete pump absorption can result from cladding modes with weak core overlap. Even if strong mode mixing is ensured with a suitable design, the pump absorption is reduced according to the limited overlap of pump light with the doped fiber core. Therefore, one typically requires an accordingly longer length of active fiber. That can be detrimental e.g. in terms of fiber nonlinearities. Also, the larger total amount of dopant ions can make it more difficult to achieve laser or amplifier operation with short signal wavelengths, and the increased amount of fluorescent light can decrease the power conversion efficiency.

Some of the signal light may be coupled out of the core into the pump cladding, e.g. as a result of bending or by a fiber Bragg grating. That light will then remain in the pump cladding and will not (as for other fibers) get lost via the coating. One may need some type of cladding light stripper (cladding mode stripper) to remove such light, if it would be disturbing in the device output. That may also be the case for residual pump light.


tutorial fiber amplifiers

Fiber Amplifiers | rare earth ions, gain and pump absorption, ASE, pumping, double-clad fibers, pulse amplification, noise
Part 6: High-power Fiber Amplifiers With Double-clad Fibers | ASE

We discuss high-power fiber amplifiers with double-clad fibers. With double-clad devices one encounters various additional difficulties, e.g. related to reduced pump absorption and increased ASE problems.

case study double-clad fiber amplifier

Case Studies

Case Study: Designing a Double-clad Fiber Amplifier

We develop a double-clad fiber amplifier with high gain, where we have to care about limiting losses by ASE.

More to Learn


Case studies:

Encyclopedia articles:


The RP Photonics Buyer's Guide contains 17 suppliers for double-clad fibers. Among them:


[1]E. Snitzer et al., “Double-clad, offset-core Nd fiber laser” (first report of cladding pumping), Proc. Conf. Optical Fiber Sensors, postdeadline paper PD5 (1988)
[2]E. Snitzer et al. “Optical fiber lasers and amplifiers”, US Patent 4,815,079A (1989)
[3]D. J. Ripin et al., “High efficiency side-coupling of light into optical fibres using embedded v-grooves”, Electron. Lett. 31, 2204 (1995); https://doi.org/10.1049/el:19951429
[4]J. Nilsson et al., “Ring-doped cladding-pumped single-mode three-level fiber laser”, Opt. Lett. 23 (5), 355 (1998); https://doi.org/10.1364/OL.23.000355
[5]V. Dominic et al., “110 W fibre laser”, Electron. Lett. 35, 1158 (1999); https://doi.org/10.1049/el:19990792
[6]G. C. Valley, “Modeling cladding-pumped Er/Yb fiber amplifiers”, Opt. Fiber Technol. 7, 21 (2001); https://doi.org/10.1006/ofte.2000.0351
[7]F. Hakimi and H. Hakimi, “Side-pumped optical amplifiers and lasers”, US Patent 6,370,297B1 (2002)
[8]D. Kouznetsov and J. V. Moloney, “Efficiency of pump absorption in double-clad fiber amplifiers. II. Broken circular symmetry”, J. Opt. Soc. Am. B 19 (6), 1259 (2002); https://doi.org/10.1364/JOSAB.19.001259
[9]D. Kouznetsov and J. V. Moloney, “Efficiency of pump absorption in double-clad fiber amplifiers. III: Calculation of modes”, J. Opt. Soc. Am. B 19 (6), 1304 (2003); https://doi.org/10.1364/JOSAB.19.001304
[10]J. Limpert et al., “Thermo-optical properties of air-clad photonic crystal fiber lasers in high power operation”, Opt. Express 11 (22), 2982 (2003); https://doi.org/10.1364/OE.11.002982
[11]Y. Jeong et al., “Ytterbium-doped large-core fiber laser with 1.36 kW continuous-wave output power”, Opt. Express 12 (25), 6088 (2004); https://doi.org/10.1364/OPEX.12.006088
[12]L. J. Cooper et al., “High-power Yb-doped multicore ribbon fiber laser”, Opt. Lett. 30 (21), 2906 (2005); https://doi.org/10.1364/OL.30.002906
[13]A. Croteau et al., “Bending-insensitive, highly Yb-doped LMA triple clad fiber for nearly diffraction-limited laser output”, Proc. SPIE 6101, 61010G-1 (2006); https://doi.org/10.1117/12.674317
[14]V. Filippov et al., “Double clad tapered fiber for high power applications”, Opt. Express 16 (3), 1929 (2008); https://doi.org/10.1364/OE.16.001929
[15]Y. Shamir et al., “250 W clad pumped Raman all-fiber laser with brightness enhancement”, Opt. Lett. 43 (4), 711 (2018); https://doi.org/10.1364/OL.43.000711
[16]Y. Feng et al., “Pump absorption, laser amplification, and effective length in double-clad ytterbium-doped fibers with small area ratio”, Opt. Express 27 (19), 26821 (2019); https://doi.org/10.1364/OE.27.026821
[17]J. Kafka, US patent 4,829,529 “Laser diode pumped fiber laser with pump cavity” (1989)
[18]R. Paschotta, case study on pump absorption in a double-clad fiber

(Suggest additional literature!)

Questions and Comments from Users


Isn't figure 1 labeled wrongly? I believe the label of the dark gray should be “outer cladding” rather than “polymer coating”.

The author's answer:

Well, both is correct: the polymer coating functions as the outer cladding in this case.


Does the NA of the inner cladding have an influence on pump absorption?

The author's answer:

In principle, that could be the case, since a higher NA means more high-order modes, which could exhibit weaker pump absorption. In practice, however, I think that such effects should be weak.

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