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Large Mode Area Fibers

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Acronym: LMA fiber

Definition: optical fibers with relatively large mode areas and a single transverse mode or only a few modes

German: Fasern mit großer Modenfläche

Category: fiber optics and waveguides

How to cite the article; suggest additional literature

For some applications, it is desirable to use optical fibers with particularly large effective mode areas (LMA fibers) – often still with single-mode guidance. Due to the reduced optical intensities, such fibers effectively have lower nonlinearities and a higher damage threshold, which makes them suitable for, e.g., the amplification of intense pulses or single-frequency signals in fiber amplifiers, or in the case of passive fibers for delivery of such light. Whereas standard single-mode fibers have an effective mode area below 100 μm2, large mode area fibers reach values of hundreds or even thousands of μm2.

For a large mode area, one requires a large fiber core. However, large-core fibers do not necessarily have large modes, if they are strongly multimode; at least the fundamental mode may then be much smaller than the core.

Note that waveguide dispersion becomes weak for large mode areas. Therefore, there is limited scope for tailoring the chromatic dispersion of large mode area fibers.

standard and large mode area fiber

Figure 1: Comparison of bare (uncoated) fibers with a standard core size (e.g. 8 μm diameter) and a large core (50 μm diameter).

Design Approaches and Limiting Factors

A straightforward design approach to obtain large mode areas is to decrease the numerical aperture (NA), i.e., to decrease the refractive index difference between the core and the cladding, for a step-index fiber design (see Figure 2). However, there are severe limitations: the guidance (waveguiding) then becomes weak, and significant losses can arise from small imperfections of the fiber or from bending (→ bend losses). Therefore, the numerical aperture should normally not be made smaller than approximately 0.06, although in extreme cases values as low as 0.04 have been used [38].

parameters of step-index LMA fibers

Figure 2: Effective mode area of a step-index fiber as a function of numerical aperture (NA) for different values of the V number. Large mode areas can in principle be achieved even with V = 2, i.e., with strictly single-mode guidance, but this requires the use of a very small numerical aperture, which implies a critical dependence on refractive index inhomogeneities and bending.

There are additional difficulties in applying this concept to rare-earth-doped fibers. Relatively high concentrations of additional dopants are often required, e.g. for reducing certain quenching effects, and these dopants often increase the numerical aperture. Even if the refractive index contrast can be reduced in some way, the precision of refractive index control may be decreased, and this affects the ability to realize very large mode areas.

Somewhat larger mode areas can be achieved with fiber designs supporting a few propagation modes (→ multimode fibers). It may then still be possible to guide light dominantly in the fundamental mode, so that the output e.g. of a fiber amplifier is close to diffraction-limited [1, 2, 5]. Stringent limitations arise from the more critical launch conditions and from mode mixing in the fiber, which can spoil the beam quality and lead to beam pointing fluctuations [16].

Various more sophisticated fiber designs (partly based on photonic crystal fibers) and techniques have been developed for addressing these challenges. In many cases, one attempts to introduce substantial propagation losses for any higher-order modes, making it more easy to maintain robust single-mode propagation in a multimode fiber. Another important aspect is to minimize unwanted mode coupling. Some examples for possible strategies are:

The best fiber designs reach an effective mode area of several thousand μm2. There is not a strict limit, but designs with larger mode areas exhibit less robust single-mode propagation and often can tolerate only very slight bending. It appears that no kind of design can offer a further substantial expansion of the mode area with robust single-mode propagation. The reason for this is essentially that a mode involves some balance of diffraction and waveguiding, and as diffraction inevitably becomes weaker at larger mode areas, this balance becomes more and more sensitive to any disturbances.

In high-power fiber lasers and amplifiers based on large mode area fibers, thermal lensing can lead to changes of mode properties, in particular to a reduction in effective mode area [31].

The problem of refractive index control can in some situations be mitigated by using a multifilament core, where the fiber core is realized as a two-dimensional array of filaments [19]. As each single filament exhibits only weak guidance, the overall structure can exhibit single-mode guidance. This concept is particularly interesting for erbium-ytterbium-doped fibers.

A relatively novel concept is that of the gain-guided, index-antiguided single-mode fiber [6, 14, 22, 26], which is a type of active fiber. Here, the unpumped fiber is not guiding (even antiguiding), as the refractive index of its core is lower than that of the cladding. For sufficiently strong pumping, however, gain guiding can stabilize a leaky mode with high beam quality. As the losses of such a mode rapidly decrease for increasing core size, a fairly moderate laser gain can be sufficient to achieve propagation with positive net gain if the core is large. Higher-order modes also exist, but would require a significantly higher gain. That level of gain is not reached when the lower-order mode saturates the gain, as it easily happens in a laser, but not necessarily in a high-gain amplifier. The greatest challenge of this concept is efficient pumping. Note that the pump light is not guided and even expelled from the doped core by the index structure and the absorption. A diode-pumped fiber laser has been demonstrated with this concept [22], but novel pump arrangements will have to be developed to allow for efficient operation.

A General Difficulty

A general problem with the use of large mode are fibers is that these fibers are not compatible with standard fiber components. (Many fiber-optic components are only available with standard mode sizes.) When a large mode area fiber is fusion spliced to a standard fiber, the large mismatch in mode areas leads to an excessive power loss at the joint (see the article on fiber joints). There are two solutions to this problem, which however are both not fully satisfying:

Possible Alternative Solution: Using Higher-order Modes

Normally, a large mode area fiber is understood to be a fiber which has a single guided mode for polarization direction or only very few modes. However, one can also obtain a large mode area by utilizing a high-order mode of a multimode fiber [10, 20, 34]. In practice, one can first couple light from the fundamental mode to a particular higher-order mode, using a long-period fiber Bragg grating. Thereafter, light can propagate in that mode e.g. in an amplifying fiber, and finally it can be converted back to the fundamental mode with another fiber Bragg grating. The advantage of using a higher-order mode is twofold: such modes have larger effective mode areas, and they exhibit a weaker coupling to other modes. The power losses associated with coupling to and from this higher-order mode can be small, and the fiber design can be optimized for a broad bandwidth for this coupling.

However, difficulties with that HOM fiber technique might arise from the very uneven intensity distribution. This can lead to fiber damage even in a regime where the overall nonlinearity is moderately strong, so the approach may solve problems with nonlinearities but not those with damage. Also, the mode field significantly extends into the cladding (the inner cladding in the case of a double-clad fiber), which is not ideal for amplification.

Bibliography

[1]M. E. Fermann, “Single-mode excitation of multimode fibers with ultrashort pulses”, Opt. Lett. 23 (1), 52 (1998)
[2]H. L. Offerhaus et al., “High-energy single-transverse-mode Q-switched fiber laser based on a multimode large-mode-area erbium-doped fiber”, Opt. Lett. 23 (21), 1683 (1998)
[3]J. C. Knight et al., “Large mode area photonic crystal fibre”, Electron. Lett. 34, 1347 (1998)
[4]N. G. R. Broderick et al., “Large mode area fibers for high power applications”, Opt. Fiber Technol. 5, 185 (1999)
[5]J. P. Koplow et al., “Single-mode operation of a coiled multimode fiber amplifier”, Opt. Lett. 25 (7), 442 (2000)
[6]A. E. Siegman, “Propagating modes in gain-guided optical fibers”, J. Opt. Soc. Am. A 20 (8), 1617 (2003)
[7]W. S. Wong et al., “Breaking the limit of maximum effective area for robust single-mode propagation in optical fibers”, Opt. Lett. 30 (21), 2855 (2005)
[8]J. M. Fini, “Bend-resistant design of conventional and microstructure fibers with very large mode area”, Opt. Express 14 (1), 69 (2006)
[9]J. M. Fini, “Bend-compensated design of large-mode-area fibers”, Opt. Lett. 31 (13), 1963 (2006)
[10]S. Ramachandran et al., “Light propagation with ultralarge modal areas in optical fibers”, Opt. Lett. 31 (12), 1797 (2006)
[11]L. Dong et al., “Bend-resistant fundamental mode operation in ytterbium-doped leakage channel fibers with effective areas up to 3160 μm2”, Opt. Express 14 (24), 11512 (2006)
[12]C. Liu et al., “Effectively single-mode chirally-coupled core fiber”, in Advanced Solid-State Photonics, OSA Technical Digest Series (CD), paper ME2 (2007)
[13]Y. Tsuchida et al., “Design of single-moded holey fibers with large-mode-area and low bending losses: the significance of the ring-core region”, Opt. Express 15 (4), 1794 (2007)
[14]Y. Chen et al., “Lasing in a gain-guided index antiguided fiber”, J. Opt. Soc. Am. B 24 (8), 1683 (2007)
[15]L. Dong et al., “Leakage channel optical fibers with large effective area”, J. Opt. Soc. Am. B 24 (8), 1689 (2007)
[16]S. Wielandy, “Implications of higher-order mode content in large mode area fibers with good beam quality”, Opt. Express 15 (23), 15402 (2007)
[17]O. Schmidt et al., “Single-polarization ultra-large-mode-area Yb-doped photonic crystal fiber”, Opt. Express 16 (6), 3918 (2008)
[18]X. Feng et al., “Single-mode tellurite glass holey fiber with extremely large mode area for infrared nonlinear applications”, Opt. Express 16 (18), 13651 (2008)
[19]G. Canat et al., “Multifilament-core fibers for high energy pulse amplification at 1.5 μm with excellent beam quality”, Opt. Lett. 33 (22), 2701 (2008)
[20]S. Ramachandran et al., “Ultra-large effective-area, higher-order mode fibers: a new strategy for high-power lasers”, Laser & Photon. Rev. 2 (6), 429 (2008)
[21]A. Galvanauskas et al., “Effectively single-mode large core passive and active fibers with chirally coupled-core structures”, paper CMB1 at CLEO/QELS 2008, May 4–9, San Jose, CA
[22]V. Sudesh et al., “Diode-pumped 200 μm diameter core, gain-guided, index-antiguided single mode fiber laser”, Appl. Phys. B 90, 369 (2008)
[23]L. Dong et al., “All-glass large-core leakage channel fibers”, IEEE Sel. Top. Quantum Electron. 15 (1), 47 (2009)
[24]L. Fu et al., “Extremely large mode area optical fibers formed by thermal stress”, Opt. Express 17 (14), 11782 (2009)
[25]X. Ao, T. Her and L. W. Casperson, “Gain guiding in large-core Bragg fibers”, Opt. Express 17 (25), 22666 (2009)
[26]W. Hageman et al., “Scalable side-pumped, gain-guided index-antiguided fiber laser”, J. Opt. Soc. Am. B 27 (12), 2451 (2010)
[27]F. Stutzki et al., “High average power large-pitch fiber amplifier with robust single-mode operation”, Opt. Lett. 36 (5), 689 (2011)
[28]J. M. Fini, “Large mode area fibers with asymmetric bend compensation”, Opt. Express 19 (22), 21866 (2011)
[29]K. R. Hansen et al., “Thermo-optical effects in high-power ytterbium-doped fiber amplifiers”, Opt. Express 19 (24), 23965 (2011)
[30]J. Limpert et al., “Yb-doped large-pitch fibres: effective single-mode operation based on higher-order mode delocalisation”, Light Sci. Appl. 1 (4), e8 (2012)
[31]F. Jansen et al., “Thermally induced waveguide changes in active fibers”, Opt. Express 20 (4), 3997 (2012)
[32]W. Ke et al., “Thermally induced mode distortion and its limit to power scaling of fiber lasers”, Opt. Express 21 (12), 14272 (2013)
[33]S. Lefrancois et al., “High-energy similariton fiber laser using chirally-coupled core fiber”, Opt. Lett. 38 (1), 43 (2013)
[34]X. Peng et al., “Higher-order mode fiber enables high energy chirped-pulse amplification”, Opt. Express 21 (26), 32411 (2013)
[35]J. Yehouessi et al., “Design and realization of flexible very large mode area pixelated Bragg fibers”, Opt. Lett. 40 (3), 363 (2015)
[36]D. Jain et al., “Demonstration of ultra-low NA rare-earth doped step index fiber for applications in high power fiber lasers”, Opt. Express 23 (6), 7407 (2015)
[37]J. Yehouessi et al., “Extreme large mode area in single-mode pixelated Bragg fiber”, Opt. Express 24 (5), 4761 (2016)
[38]F. Beier et al., “Narrow linewidth, single mode 3 kW average power from a directly diode pumped ytterbium-doped low NA fiber amplifier”, Opt. Express 24 (6), 6011 (2016)

(Suggest additional literature!)

See also: large-core fibers, effective mode area, fibers, bend losses, numerical aperture, fiber core, leaky modes, fiber amplifiers, photonic crystal fibers, Spotlight article 2006-08-10, Spotlight article 2006-10-04, Spotlight article 2006-12-03, Spotlight article 2006-12-03, Spotlight article 2007-02-04, Spotlight article 2007-04-28
and other articles in the category fiber optics and waveguides

In the RP Photonics Buyer's Guide, 7 suppliers for large mode area fibers are listed.

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