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Optics Express

  • Editor: Andrew M. Weiner
  • Vol. 21, Iss. 22 — Nov. 4, 2013
  • pp: 26663–26670
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Bending performance of large mode area multi-trench fibers

Deepak Jain, Catherine Baskiotis, and Jayanta Kumar Sahu  »View Author Affiliations


Optics Express, Vol. 21, Issue 22, pp. 26663-26670 (2013)
http://dx.doi.org/10.1364/OE.21.026663


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Abstract

Bending performance of the Multi-trench Fibers (MTFs) has been investigated using the Finite Element Method. Numerical investigations show that MTFs can provide low-loss effective single mode operation under bent configuration, thanks to the resonant coupling of the Higher order Modes (HOMs). Large ratio between the HOMs and the Fundamental Mode (FM) losses can be ensured, although the ratio drops with increasing Effective Area (Aeff) of the FM. MTFs provide better losses ratio between the HOMs and the FM in comparison with other fibers like step-index, W-type, and parabolic fibers.

© 2013 Optical Society of America

1. Introduction

High power fiber lasers have realized their potential over the last decade. Power level of fiber lasers has already crossed the 10kW level [1

1. V. Gapontsev, V. Fomin, A. Ferin, and M. Abramov, “Diffraction limited ultra-high-power fiber lasers,” ASSP Paper AWA1 (2010).

]. However, non-linear effects impose serious constraints on power scaling. One way to mitigate these effects is to increase the Effective Area (Aeff) of the fundamental core mode and reduce the length of the fiber laser, which increases the threshold power level for stimulated non-linear effects.

Low-NA SIFs, which work on elimination of the HOMs by bend-induced filtering, have shown good potential for mode area scaling [5

5. J. P. Koplow, D. A. V. Kliner, and L. Goldberg, “Single-mode operation of a coiled multimode fiber amplifier,” Opt. Lett. 25(7), 442–444 (2000). [CrossRef] [PubMed]

, 6

6. M.-J. Li, X. Chen, A. Liu, S. Gray, J. Wang, D. T. Walton, and L. A. Zenteno, “Limit of effective area for single-mode operation in step-index large mode area laser fibers,” J. Lightwave Technol. 27(15), 3010–3016 (2009). [CrossRef]

]. Their performances are limited by the decreasing losses ratio between the HOMs and the FM with increasing area [6

6. M.-J. Li, X. Chen, A. Liu, S. Gray, J. Wang, D. T. Walton, and L. A. Zenteno, “Limit of effective area for single-mode operation in step-index large mode area laser fibers,” J. Lightwave Technol. 27(15), 3010–3016 (2009). [CrossRef]

]. PCFs are also a new approach of large mode area scaling [7

7. J. Limpert, A. Liem, M. Reich, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermann, J. Broeng, A. Petersson, and C. Jakobsen, “Low-nonlinearity single-transverse-mode ytterbium-doped photonic crystal fiber amplifier,” Opt. Express 12(7), 1313–1319 (2004). [CrossRef] [PubMed]

]. However, they require complex fabrication process like stack and draw technique. Moreover, the presence of air-holes leads to numerous practical difficulties. LCFs, which are a modified form of the PCFs, offer better mode area scaling than PCFs but have poor losses ratio between the HOMs and the FM [3

3. J. M. Fini, “Bend-resistant design of conventional and microstructure fibers with very large mode area,” Opt. Express 14(1), 69–81 (2006). [CrossRef] [PubMed]

, 8

8. L. Dong, H. A. McKay, L. Fu, M. Ohta, A. Marcinkevicius, S. Suzuki, and M. E. Fermann, “Ytterbium-doped all glass leakage channel fibers with highly fluorine-doped silica pump cladding,” Opt. Express 17(11), 8962–8969 (2009). [CrossRef] [PubMed]

]. Recently, mode-area scaling of 2-D ASPBGFs has been proposed [9

9. F. Kong, K. Saitoh, D. Mcclane, T. Hawkins, P. Foy, G. Gu, and L. Dong, “Mode area scaling with all-solid photonic bandgap fiber,” Opt. Express 20(24), 26363–26372 (2012). [CrossRef]

]. However, their fabrication is complex and expensive. Moreover, these fibers suffer from reduced cladding-pumping efficiency due to the presence of high index rods in the cladding. Fibers having tailored cladding for HOMs suppression are also limited in mode area scaling [11

11. A. Kumar and V. Rastogi, “Design and analysis of a multilayer cladding large-mode-area optical fiber,” J. Opt. A, Pure Appl. Opt. 10(1), 015303 (2008). [CrossRef]

].

Bragg fibers have shown large mode area scaling capability and offer the advantages of good bend-robustness and easy fabrication process [10

10. E. M. Dianov, M. E. Likhachev, and S. Fevrier, “Solid-core photonic bandgap fibers for high-power fiber lasers,” IEEE J. Sel. Top. Quantum Electron. 15(1), 20–29 (2009). [CrossRef]

, 12

12. C. Baskiotis, D. Molin, G. Bouwmans, F. Gooijer, P. Sillard, Y. Quiquempois, and M. Douay, “Bending behaviours of all-solid silica large mode area Bragg fibers,” Proc. SPIE 7195, 719520 (2009). [CrossRef]

, 13

13. C. Baskiotis, Y. Quiquempois, M. Douay, and P. Sillard, “Extending the effective area of coiled all-solid silica single-mode Bragg fibers,” ECOC, Geneva, Switzerland, paper We.10.P1.02, (2011).

]. However, the presence of the high-index rings in the Bragg fiber can cause unwanted couplings between the core and the high-index ring modes due to slight imperfections in the realized fibers [14

14. S. S. Aleshkina, M. E. Likhachev, A. D. Pryamikov, D. A. Gaponov, A. N. Denisov, M. M. Bubnov, M. Y. Salganskii, A. Y. Laptev, A. N. Guryanov, Y. A. Uspenskii, N. L. Popov, and S. Février, “Very-large-mode-area photonic bandgap Bragg fiber polarizing in a wide spectral range,” Opt. Lett. 36(18), 3566–3568 (2011). [CrossRef] [PubMed]

]. Moreover, these high-index rings do not allow the Stress Applying Parts (SAPs) to be put outside of the core region, which makes the realization of a polarization maintaining Bragg fiber difficult. On the other hand, by placing the SAPs inside the core of the Bragg fiber, a single-polarization Bragg fiber has been demonstrated. However, this dramatically reduces the Aeff of the FM [14

14. S. S. Aleshkina, M. E. Likhachev, A. D. Pryamikov, D. A. Gaponov, A. N. Denisov, M. M. Bubnov, M. Y. Salganskii, A. Y. Laptev, A. N. Guryanov, Y. A. Uspenskii, N. L. Popov, and S. Février, “Very-large-mode-area photonic bandgap Bragg fiber polarizing in a wide spectral range,” Opt. Lett. 36(18), 3566–3568 (2011). [CrossRef] [PubMed]

].

Recently, we proposed a new structure, the Multi-trench fibers (MTFs), for mode area scaling of rod-type fibers [15

15. D. Jain, C. Baskiotis, and J. K. Sahu, “Mode area scaling with Multi-trench rod-type fibers,” Opt. Express 21(2), 1448–1455 (2013). [CrossRef] [PubMed]

]. Thanks to their cylindrical symmetry, these fibers offer advantages such as easy fabrication and preservation of beam quality in the presence of small core index-depression (better than in the case of large-pitch PCFs (LPFs)) [15

15. D. Jain, C. Baskiotis, and J. K. Sahu, “Mode area scaling with Multi-trench rod-type fibers,” Opt. Express 21(2), 1448–1455 (2013). [CrossRef] [PubMed]

]. Moreover, there are no high-index rings in the MTFs, so it should be free from any unwanted couplings due to imperfections in the realized fibers. In this paper, we investigate the potential of MTFs for compact fiber lasers and beam delivery applications.

2. Multi-trench fiber

Figure 1(a)
Fig. 1 (a) Schematic cross-section of the MTF. Blue and white colours represent high and low-refractive index regions respectively. (b) Schematic of refractive index profile of the MTF.
shows the schematic cross section of the MTF structure. Figure 1(b) shows the schematic of refractive index profile of the MTF and also presents the notations used in this paper: rc is the core radius, t is the thickness of all the low-index rings (trenches), d1 and d2 are the thicknesses of the first and the second high-index rings (resonant rings), and Δn is the refractive index difference between the core and the trenches.

Numerical simulations on MTFs have been performed with a full-vectorial Finite Element Method (FEM), in which the domain truncation has been ensured by using the circular anisotropic Perfectly Matched Layer (PML). All the calculations presented in this paper are at 1.06µm wavelength.

3. Design of 30µm core MTF in straight and bent condition

The leakage losses of the FM and the first four HOMs of a 30µm diameter core fiber, with t = 2µm and Δn = 0.006, as a function of thickness of the resonant ring (assuming both resonant rings thicknesses to be the same, i.e. d1 = d2 = d) are shown in Fig. 2(a)
Fig. 2 Losses of the FM and the few HOMs in (a) unbent (b) bent fiber at 15cm bend radius as a function of the resonant ring thickness of the fiber having rc = 15µm, t = 2µm, and Δn = 0.006.
. All the modes of the core are leaky due to their resonance coupling with the resonant rings modes. In order to ensure, a single-mode operation of the core, we need to ensure high losses for the HOMs of the core by resonant couplings to the resonant rings modes as compared to the FM modes. It is well known that for a complete resonant coupling to take place between two leaky modes, there are two basic conditions to satisfy. First one is the phase matching and second one is the loss matching of two leaky modes under coupling [16

16. Z. Zhang, Y. Shi, B. Bian, and J. Lu, “Dependence of leaky mode coupling on loss in photonic crystal fiber with hybrid cladding,” Opt. Express 16(3), 1915–1922 (2008). [CrossRef] [PubMed]

].

It is worth noting that the effective indices of the HOMs of the core are different, so it is impossible to fulfill both of these conditions completely for all the relevant HOMs of the core at a single thickness of the resonant ring. However, the thickness of the resonant ring can be chosen in such a way that all the relevant HOMs sustain sufficient leakage losses for effective single mode operation as shown in Fig. 2(a). The leakage losses of the FM are smaller than 0.0045dB/m for all the studied resonant ring thicknesses (5μm to 10μm) and the LP11 leakage losses remain larger than 1dB/m for resonant ring thickness from 8.5µm to 10.0μm. The leakage losses of all the other HOMs of the core (we have considered all the possible HOMs of the core, although the losses of only few of them have been shown in Fig. 2(a)) are larger than 1.5dB/m for all the studied resonant ring thicknesses. The leakage losses of the HOMs can be increased by decreasing the trench thickness (t), or the refractive index difference of trench (Δn) as observed in the design of the 100μm and 140µm diameter core MTFs [15

15. D. Jain, C. Baskiotis, and J. K. Sahu, “Mode area scaling with Multi-trench rod-type fibers,” Opt. Express 21(2), 1448–1455 (2013). [CrossRef] [PubMed]

].

Bending losses of the MTF can be analyzed using standard conformal mapping [17

17. D. Marcuse, “Influence of curvature on the losses of doubly clad fibers,” Appl. Opt. 21(23), 4208–4213 (1982). [CrossRef] [PubMed]

] with additional stress perturbations [18

18. K. Nagano, S. Kawakami, and S. Nishida, “Change of the refractive index in an optical fiber due to external forces,” Appl. Opt. 17(13), 2080–2085 (1978). [CrossRef] [PubMed]

] by following the standard equation:
    n2eq(r,φ)=n2(r)*(1+2rρRcosφ),
(1)
where n(r) is the index profile of the unbent fiber, R is the bend radius, φ is the azimuthal angle, and ρ (here fixed to 1.25) has been included to take account of the stress factor. Inset of Fig. 2(b) shows the obtained equivalent refractive index profile of the MTF shown in Fig. 1(b) for d = 8µm, Δn = 0.006, t = 2μm, at a bend radius of 15cm using the above equation. It is clear from the equivalent profile of the fiber that, under the bent case the effective indices of the core and the ring modes change, and in turn the conditions of phase matching for resonance coupling also change. Figure 2(b) shows the bending losses of the LP01 and the LP11 modes (including both polarizations of the LP11 mode) of the core as a function of the resonant ring thickness. The losses in the bent case are large compared to the unbent case due to the bend-induced coupling with the resonant rings. Figure 2(b) shows the large losses for the LP11 mode (from 4dB/m to 14dB/m) for the resonant ring thickness from 8.0 to 8.5µm.

From a perspective of fabrication, we studied the unitless ratio of lowest losses level of the HOMs, expressed in dB/m, (considering all the HOMs and their polarizations as well) to the FM losses, expressed in dB/m, as a function of the resonant ring thickness. We have considered the mismatch of both the resonant rings thicknesses since it is unlikely to obtain exactly the same thickness of both the resonant rings in a fabricated fiber. Figure 3(a)
Fig. 3 Ratio of the HOMs lowest losses level to the FM losses for different combinations of the first and the second resonant rings thicknesses for 30µm diameter core fiber with t = 2µm (a) Δn = 0.006 (b) Δn = 0.005. (c) and (d) shows the respective FM losses for these fiber parameters. X-axis presents thickness of the first resonant ring (d1) and Y-axis presents a parameter Y, where thickness of the second resonant ring is equal to d2 = 2*Y-d1. All Figs. has its own color scale.
shows the ratio of lowest losses level of the HOMs to the FM losses for different thicknesses of the resonant rings of the fiber with rc = 15μm, t = 2µm, and Δn = 0.006 at 15cm bend radius. X-axis shows the thickness of the first resonant ring (d1). Y-axis shows the relative thickness of the second resonant ring (Y), whereas absolute thickness of the second resonant ring is d2 = 2*Y-d1. For example in Fig. 3(a), for a first resonant ring thickness (d1) of 8µm, Y varies from 8µm to 8.5µm, so the absolute thickness of the second resonant ring (d2) varies from 8μm to 9μm. Similarly for d1 = 8.5μm, Y varies from 8μm to 8.5μm which corresponds to second ring thickness (d2) from 8μm to 8.5μm. Figure 3(b) shows the losses ratio for the similar fiber as in Fig. 3(a) but for a different Δn = 0.005. Figures 3(c) and 3(d) show the corresponding losses of the FM. It can be observed that for Δn = 0.006, the FM losses vary from 0.014dB/m to 0.022dB/m, the losses ratio varies from 168 to 394, and the HOMs lowest losses vary from 2.35dB/m to 7dB/m. Similarly for Δn = 0.005, the FM losses vary from 0.06dB/m to 0.1dB/m, the losses ratio varies from 162 to 317, and the HOMs lowest losses vary from 12dB/m to 22dB/m. From Figs. 3(c) and 3(d), we can conclude that slight variations of the refractive-index have stronger impact on the FM and the HOMs losses than their losses ratio. This result is in good agreement with those of the earlier study of the rod-type MTFs [15

15. D. Jain, C. Baskiotis, and J. K. Sahu, “Mode area scaling with Multi-trench rod-type fibers,” Opt. Express 21(2), 1448–1455 (2013). [CrossRef] [PubMed]

]. Similarly, we have observed that a slight increase and decrease of the trench thickness has stronger impact on the FM and the HOMs losses than their losses ratio. We have omitted, here, the details of these results (impact of trench thickness on the losses of the core modes), due to their similarity with those obtained in the unbent case [15

15. D. Jain, C. Baskiotis, and J. K. Sahu, “Mode area scaling with Multi-trench rod-type fibers,” Opt. Express 21(2), 1448–1455 (2013). [CrossRef] [PubMed]

]. We can see from these calculations that a good losses ratio between the HOMs and the FM, which is an important property for the fiber lasers and for beam-delivery applications, can be obtained from a 30µm diameter core MTF. Moreover, this high ratio can be obtained for a wide range of bend radius, which is also a desired feature for numerous applications.

4. Mode area scaling to 40μm and 46µm diameter core

To scale up the mode area further, we studied 40µm and 46µm diameter core MTFs with t = 1.6µm and Δn = 0.006 at 20cm bend radius. Figures 5(a)
Fig. 5 (a) and (c) Ratio of the HOMs lowest losses level to the FM losses for different combinations of the first and the second resonant rings thicknesses for 40µm and 46µm diameter core fibers respectively with t = 1.6µm and Δn = 0.006 at 20cm bend radius (b) and (d) shows the respective FM losses for these fiber parameters. X-axis presents the thickness of the first resonant ring (d1) and Y-axis presents a parameter Y, where the thickness of the second resonant ring is equal to d2 = 2*Y-d1. All Figs. has its own color scale.
and 5(b) show the ratio of the HOMs lowest losses level to the FM losses and the losses of the FM respectively, for different combinations of the first and second resonant ring thicknesses of 40μm diameter core fiber. For large numbers of combinations of the resonant ring thicknesses shown in Figs. 5(a) and 5(b), the FM losses vary from 0.033dB/m to 0.099dB/m, while the losses ratio varies from 49 to 203. Figure 5(a) also shows a region covered by the dashed white line, which corresponds to the thicknesses of both the resonant rings varying from 10µm to 11µm. For these combinations of the thicknesses, the FM losses vary from 0.034dB/m to 0.075dB/m, while the losses ratio varies from 49 to 130, and the Aeff is larger than 650µm2. On the other hand, for certain combinations of ring thicknesses (shown in dark blue in Fig. 5(a)), the FM losses goes high up to 0.21dB/m and the losses ratio drops below 30. For these combinations, the second resonator thickness is large enough (from 12.5µm to 13µm) to induce the coupling between the FM and the second resonant ring modes, which in turn induces high losses to the FM. Figure 5(c) shows the ratio of the HOMs lowest losses level to the FM losses for 46µm diameter core. Over the large numbers of combinations of the resonant ring thicknesses, the FM losses remain smaller than 0.12dB/m (shown in Fig. 5(d)), while the losses ratio varies from 30 to 131, and the Aeff exceeds 790µm2.

Fini et al. have reported a comparative analysis of the losses ratio between the FM and the HOMs lowest losses for a fixed FM losses of 0.1dB/m, for four different fiber design parabolic fibers, SIFs, W-type, and LCFs [3

3. J. M. Fini, “Bend-resistant design of conventional and microstructure fibers with very large mode area,” Opt. Express 14(1), 69–81 (2006). [CrossRef] [PubMed]

]. Analysis shows that the parabolic fibers offer best leakage losses ratio, which is smaller than 200 for Aeff 400µm2and 20 for Aeff 700µm2. Our study in section 3 and 4 shows that the MTFs can offer better leakage losses ratio (i.e. 162 to 317 for Aeff 400μm2 and larger than 30 for Aeff 790um2 for a fixed FM losses of 0.1dB/m) compared to the parabolic fibers. On the other hand, MTFs show significantly larger bend radius range, which is difficult to achieve in case of the SIFs and the parabolic fibers.

5. MTF in double clad configuration

It is worth noting that, in a double clad configuration, the lower power fraction of the HOMs in the core region (assuming the entire core is doped with rare-earth ions) as compared to the power fraction of the FM in the core region can also be another useful criterion for single mode operation. We calculated the power fraction of the HOMs and the FM in the core for different parameters of MTF, assuming a polymer coating of refractive index 1.35. MTF offers reduced overlap of the HOMs with the core region as compared to the FM. For example, for rc = 15μm, t = 2μm, and d = 8µm at 15cm bend radius, for different refractive index difference between the core and the trench: Δn = 0.005, 0.0045, and 0.004, the power fraction of the HOMs in the core is smaller than 0.86, 0.82, and 0.67 respectively, while the power fraction of the FM remains larger than 0.98.

6. Conclusion

We theoretically investigated the bending behavior of the MTFs at 1.06µm. MTFs with a core diameter of 30µm ensuring HOMs losses larger than 10dB/m and 1dB/m and the FM losses smaller than 0.1dB/m and 0.01dB/m respectively, over wide range of bend radius have been achieved. The Aeff of the FM remains larger than 380μm2. Furthermore, the mode area scaling to 790μm2 for a 46µm core diameter at 20cm bend radius has been achieved but at the expense of reduced losses ratio between HOMs and FM. MTFs ensure better HOMs suppression than other fiber structures like Parabolic, SIFs, and W-type fibers.

Acknowledgments

The work is supported by the EPSRC Centre for the Innovative Manufacturing in Photonics EP/HO2607X/1.

References and links

1.

V. Gapontsev, V. Fomin, A. Ferin, and M. Abramov, “Diffraction limited ultra-high-power fiber lasers,” ASSP Paper AWA1 (2010).

2.

T. Eidam, C. Wirth, C. Jauregui, F. Stutzki, F. Jansen, H.-J. Otto, O. Schmidt, T. Schreiber, J. Limpert, and A. Tünnermann, “Experimental observations of the threshold-like onset of mode instabilities in high power fiber amplifiers,” Opt. Express 19(14), 13218–13224 (2011). [CrossRef] [PubMed]

3.

J. M. Fini, “Bend-resistant design of conventional and microstructure fibers with very large mode area,” Opt. Express 14(1), 69–81 (2006). [CrossRef] [PubMed]

4.

J. Limpert, N. Deguil-Robin, I. Manek-Hönninger, F. Salin, F. Röser, A. Liem, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermann, J. Broeng, A. Petersson, and C. Jakobsen, “High-power rod-type photonic crystal fiber laser,” Opt. Express 13(4), 1055–1058 (2005). [CrossRef] [PubMed]

5.

J. P. Koplow, D. A. V. Kliner, and L. Goldberg, “Single-mode operation of a coiled multimode fiber amplifier,” Opt. Lett. 25(7), 442–444 (2000). [CrossRef] [PubMed]

6.

M.-J. Li, X. Chen, A. Liu, S. Gray, J. Wang, D. T. Walton, and L. A. Zenteno, “Limit of effective area for single-mode operation in step-index large mode area laser fibers,” J. Lightwave Technol. 27(15), 3010–3016 (2009). [CrossRef]

7.

J. Limpert, A. Liem, M. Reich, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermann, J. Broeng, A. Petersson, and C. Jakobsen, “Low-nonlinearity single-transverse-mode ytterbium-doped photonic crystal fiber amplifier,” Opt. Express 12(7), 1313–1319 (2004). [CrossRef] [PubMed]

8.

L. Dong, H. A. McKay, L. Fu, M. Ohta, A. Marcinkevicius, S. Suzuki, and M. E. Fermann, “Ytterbium-doped all glass leakage channel fibers with highly fluorine-doped silica pump cladding,” Opt. Express 17(11), 8962–8969 (2009). [CrossRef] [PubMed]

9.

F. Kong, K. Saitoh, D. Mcclane, T. Hawkins, P. Foy, G. Gu, and L. Dong, “Mode area scaling with all-solid photonic bandgap fiber,” Opt. Express 20(24), 26363–26372 (2012). [CrossRef]

10.

E. M. Dianov, M. E. Likhachev, and S. Fevrier, “Solid-core photonic bandgap fibers for high-power fiber lasers,” IEEE J. Sel. Top. Quantum Electron. 15(1), 20–29 (2009). [CrossRef]

11.

A. Kumar and V. Rastogi, “Design and analysis of a multilayer cladding large-mode-area optical fiber,” J. Opt. A, Pure Appl. Opt. 10(1), 015303 (2008). [CrossRef]

12.

C. Baskiotis, D. Molin, G. Bouwmans, F. Gooijer, P. Sillard, Y. Quiquempois, and M. Douay, “Bending behaviours of all-solid silica large mode area Bragg fibers,” Proc. SPIE 7195, 719520 (2009). [CrossRef]

13.

C. Baskiotis, Y. Quiquempois, M. Douay, and P. Sillard, “Extending the effective area of coiled all-solid silica single-mode Bragg fibers,” ECOC, Geneva, Switzerland, paper We.10.P1.02, (2011).

14.

S. S. Aleshkina, M. E. Likhachev, A. D. Pryamikov, D. A. Gaponov, A. N. Denisov, M. M. Bubnov, M. Y. Salganskii, A. Y. Laptev, A. N. Guryanov, Y. A. Uspenskii, N. L. Popov, and S. Février, “Very-large-mode-area photonic bandgap Bragg fiber polarizing in a wide spectral range,” Opt. Lett. 36(18), 3566–3568 (2011). [CrossRef] [PubMed]

15.

D. Jain, C. Baskiotis, and J. K. Sahu, “Mode area scaling with Multi-trench rod-type fibers,” Opt. Express 21(2), 1448–1455 (2013). [CrossRef] [PubMed]

16.

Z. Zhang, Y. Shi, B. Bian, and J. Lu, “Dependence of leaky mode coupling on loss in photonic crystal fiber with hybrid cladding,” Opt. Express 16(3), 1915–1922 (2008). [CrossRef] [PubMed]

17.

D. Marcuse, “Influence of curvature on the losses of doubly clad fibers,” Appl. Opt. 21(23), 4208–4213 (1982). [CrossRef] [PubMed]

18.

K. Nagano, S. Kawakami, and S. Nishida, “Change of the refractive index in an optical fiber due to external forces,” Appl. Opt. 17(13), 2080–2085 (1978). [CrossRef] [PubMed]

19.

G. Gu, F. Kong, T. W. Hawkins, P. Foy, K. Wei, B. Samson, and L. Dong, “Impact of fiber outer boundaries on leaky mode losses in leakage channel fibers,” Opt. Express 21(20), 24039–24048 (2013). [CrossRef] [PubMed]

OCIS Codes
(060.2280) Fiber optics and optical communications : Fiber design and fabrication
(140.3510) Lasers and laser optics : Lasers, fiber

ToC Category:
Fiber Optics and Optical Communications

History
Original Manuscript: July 29, 2013
Revised Manuscript: October 18, 2013
Manuscript Accepted: October 22, 2013
Published: October 29, 2013

Citation
Deepak Jain, Catherine Baskiotis, and Jayanta Kumar Sahu, "Bending performance of large mode area multi-trench fibers," Opt. Express 21, 26663-26670 (2013)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-21-22-26663


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References

  1. V. Gapontsev, V. Fomin, A. Ferin, and M. Abramov, “Diffraction limited ultra-high-power fiber lasers,” ASSP Paper AWA1 (2010).
  2. T. Eidam, C. Wirth, C. Jauregui, F. Stutzki, F. Jansen, H.-J. Otto, O. Schmidt, T. Schreiber, J. Limpert, and A. Tünnermann, “Experimental observations of the threshold-like onset of mode instabilities in high power fiber amplifiers,” Opt. Express19(14), 13218–13224 (2011). [CrossRef] [PubMed]
  3. J. M. Fini, “Bend-resistant design of conventional and microstructure fibers with very large mode area,” Opt. Express14(1), 69–81 (2006). [CrossRef] [PubMed]
  4. J. Limpert, N. Deguil-Robin, I. Manek-Hönninger, F. Salin, F. Röser, A. Liem, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermann, J. Broeng, A. Petersson, and C. Jakobsen, “High-power rod-type photonic crystal fiber laser,” Opt. Express13(4), 1055–1058 (2005). [CrossRef] [PubMed]
  5. J. P. Koplow, D. A. V. Kliner, and L. Goldberg, “Single-mode operation of a coiled multimode fiber amplifier,” Opt. Lett.25(7), 442–444 (2000). [CrossRef] [PubMed]
  6. M.-J. Li, X. Chen, A. Liu, S. Gray, J. Wang, D. T. Walton, and L. A. Zenteno, “Limit of effective area for single-mode operation in step-index large mode area laser fibers,” J. Lightwave Technol.27(15), 3010–3016 (2009). [CrossRef]
  7. J. Limpert, A. Liem, M. Reich, T. Schreiber, S. Nolte, H. Zellmer, A. Tünnermann, J. Broeng, A. Petersson, and C. Jakobsen, “Low-nonlinearity single-transverse-mode ytterbium-doped photonic crystal fiber amplifier,” Opt. Express12(7), 1313–1319 (2004). [CrossRef] [PubMed]
  8. L. Dong, H. A. McKay, L. Fu, M. Ohta, A. Marcinkevicius, S. Suzuki, and M. E. Fermann, “Ytterbium-doped all glass leakage channel fibers with highly fluorine-doped silica pump cladding,” Opt. Express17(11), 8962–8969 (2009). [CrossRef] [PubMed]
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