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  • Editor: Alan E. Willner
  • Vol. 34, Iss. 10 — May. 15, 2009
  • pp: 1507–1509
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Highly scalable, resonantly cladding-pumped, Er-doped fiber laser with record efficiency

M. Dubinskii, J. Zhang, and V. Ter-Mikirtychev  »View Author Affiliations


Optics Letters, Vol. 34, Issue 10, pp. 1507-1509 (2009)
http://dx.doi.org/10.1364/OL.34.001507


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Abstract

We report the performance of a resonantly cladding-pumped, Yb-free, Er-doped fiber laser. We believe this is the first reported resonantly cladding-pumped fiber-Bragg-grating-based, Er-doped, large-mode-area (LMA) fiber laser. The laser, pumped by fiber-coupled In Ga As P In P laser diode modules at 1532.5 nm , delivers 48 W of cw output at 1590 nm . It is believed to be the highest power ever reported from a Yb-free Er-doped LMA fiber. This fully integrated laser also has the optical-to-optical efficiency of 57 % , to the best of our knowledge, the highest efficiency reported for cladding-pumped unidirectionally emitting Er-doped laser.

© 2009 Optical Society of America

Major power scaling results in the eye-safe 1.5μm fiber lasers were reported with the cladding pumped Yb-Er codoped fibers pumped at 915980nm into Yb-absorption band [1

1. D. Y. Shen, J. K. Sahu, and W. A. Clarkson, Opt. Express 13, 4916 (2005). [CrossRef] [PubMed]

]. Owing to inefficiencies associated with very large (40%) quantum defect pertinent to this approach, scalability of these devices suffers from and is limited by enormous heat deposition inconsistent with major power scaling toward multikilowatt power levels. Besides, scaling beyond the current eye-safe power record of 300W [1

1. D. Y. Shen, J. K. Sahu, and W. A. Clarkson, Opt. Express 13, 4916 (2005). [CrossRef] [PubMed]

] is impossible with the Yb-Er codoping approach, because multihundred-watt Yb-Er fiber lasers typically carry in their output a significant fraction of competing 1 μm Yb emission [either narrowband or amplified spontaneous emission (ASE)], thus significantly compromising an eye-safe application itself. This, combined with the fact that power conversion efficiency of the Er-Yb laser systems is limited by inefficiency of Yb-Er energy transfer on top of quantum defect of Er-doped fiber pumped at 9XX nm, provides significant motivation for going back to resonantly pumped Yb-free Er-doped fiber lasers quite successfully used in telecom applications. With the resonant pumping approach Er-doped fibers should poten tially behave no different from resonantly pumped Yb-doped fibers known to be able to deliver up to 90% optical-to-optical efficiency [2

2. H. M. Pask, R. J. Chapman, D. C. Hanna, A. C. Tropper, C. J. Mackechnie, P. R. Barber, and J. M. Dawes, IEEE J. Sel. Top. Quantum Electron. 1, 2 (1995). [CrossRef]

]. In support of that statement we have recently achieved over 85% optical-to-optical efficiency from a resonantly pumped, Yb-free, Er-doped, single-mode fiber amplifier based on commercial off-the-shelf (COTS) fiber [3

3. M. Dubinskii, J. Zhang, and V. Ter-Mikirtychev, Electron. Lett. 45, 400 (2009). [CrossRef]

]. In this case pump-induced heat deposition would predominantly be associated with low quantum defect (5% and less) of a resonantly pumped Er-doped fiber laser, which opens up significant space for fiber laser power scaling suffering no thermal management complications. As opposed to single-mode fiber lasers (only scalable toward telecom power goals), an important step toward a highly scalable resonantly pumped Er fiber laser is cladding pumping, which would accommodate highly multimode fiber-coupled 14XX–15XX nm InGaAsPInP high power diodes and bars for pumping. The latter is supported by recent dramatic efficiency and power strides in the quantum-well separate confinement heterostructure lasers based on InGaAsPInP systems (e.g., [4

4. M. L. Osowski, W. Hu, R. M. Lammert, S. W. Oh, P. T. Rudy, T. Stakelon, L. Vaissie, and J. E. Ungar, Proc. SPIE 6952, 695208 (2008). [CrossRef]

]).

So far only very few efforts were reported on resonantly cladding-pumped Yb-free Er fiber lasers [5

5. D. T. Walton, L. A. Zenteno, A. Ellison, J. Anderson, X. Liu, L. Hughes, C. Caneau, and C. E. Zah, in Conference on Lasers and Electro-Optics/International Quantum Electronics Conference and Photonic Applications Systems Technologies, Technical Digest (CD) (Optical Society of America, 2004), paper CMK5.

, 6

6. J. D. Minelly, V. Stasyuk, J. P. de Sandro, E. Gagnon, and S. Chatigny, presented at Optical Amplifiers and their Applications (OAA 2004), San Francisco, Calif., June 27–30 2004, postdeadline paper PD4-1.

, 7

7. M. Dubinskii, J. Zhang, and I. Kudryashov, Appl. Phys. Lett. 93, 031111 (2008). [CrossRef]

]. In [5

5. D. T. Walton, L. A. Zenteno, A. Ellison, J. Anderson, X. Liu, L. Hughes, C. Caneau, and C. E. Zah, in Conference on Lasers and Electro-Optics/International Quantum Electronics Conference and Photonic Applications Systems Technologies, Technical Digest (CD) (Optical Society of America, 2004), paper CMK5.

, 6

6. J. D. Minelly, V. Stasyuk, J. P. de Sandro, E. Gagnon, and S. Chatigny, presented at Optical Amplifiers and their Applications (OAA 2004), San Francisco, Calif., June 27–30 2004, postdeadline paper PD4-1.

] output power of 1W was achieved (in [5

5. D. T. Walton, L. A. Zenteno, A. Ellison, J. Anderson, X. Liu, L. Hughes, C. Caneau, and C. E. Zah, in Conference on Lasers and Electro-Optics/International Quantum Electronics Conference and Photonic Applications Systems Technologies, Technical Digest (CD) (Optical Society of America, 2004), paper CMK5.

] by summing up the power emitted from both fiber ends). The work of [6

6. J. D. Minelly, V. Stasyuk, J. P. de Sandro, E. Gagnon, and S. Chatigny, presented at Optical Amplifiers and their Applications (OAA 2004), San Francisco, Calif., June 27–30 2004, postdeadline paper PD4-1.

] was actually the first effort of successfully getting to the most scalable large-mode-area (LMA) fiber approach. The work of Dubinskii et al.[7

7. M. Dubinskii, J. Zhang, and I. Kudryashov, Appl. Phys. Lett. 93, 031111 (2008). [CrossRef]

] was the first effort to scale significantly beyond the 1W power level. Single-frequency output power of 9.3W was obtained in master-oscillator power-amplifier configuration from resonantly cladding-pumped Yb-free EDFA with the slope efficiency of 46% with respect to absorbed pump power [7

7. M. Dubinskii, J. Zhang, and I. Kudryashov, Appl. Phys. Lett. 93, 031111 (2008). [CrossRef]

]. Presented here are characterization results of a resonantly cladding-pumped fiber Bragg grating (FBG) laser based on Yb-free Er-doped COTS LMA fiber. To our knowledge this is the first reported resonantly cladding-pumped FBG-based Er-doped LMA fiber laser. Obtained narrowband output of 47.6W is believed to be the highest power ever reported from a Yb-free Er-doped fiber laser. This fully integrated laser also has the optical-to-optical efficiency of 56.7%, which we believe is the highest efficiency ever reported for a cladding-pumped unidirectionally emitting Er-doped laser. No indication of power saturation effects was observed; i.e., achieved power is strictly pump limited and can be further scaled significantly.

In this work no special effort was made on laser fiber composition and design: A commercially available Liekki Er60-20/125DC double-clad (DC), Yb-free, Er-doped LMA fiber was efficiency and power tested in a simple FBG-based laser configuration for power scaling potential evaluation.

Figure 1 depicts the optical layout of the fully integrated Er fiber laser based on COTS Liekki Er60-20/125 DC fiber pumped through the FBG which was used in a function of a dichroic (WDM) pump mirror. The FBG, matching the 20125 DC fiber format, was manufactured by IPG Photonics Corp. and has the 93.5% reflectivity centered at 1589.4nm with the 2.58nm bandwidth (FWHM). The fiber laser was copumped by six fiber-coupled (into a 105125μm, NA 0.15 fiber) spectrally narrowed (bandwidth of 0.5nm FWHM), InGaAsPInP laser diode modules. The custom-made modules, spectrally narrowed by volume Bragg gratings, delivered an average of 18.5W of fiber-coupled power each, centered at 1532.5nm. This wavelength was chosen to fit the peak of the Er60-20/125DC fiber absorption spectrum in order to minimize the required fiber length. Copumping was realized through the SIFAM six-port pump combiner matching the Er60-20/125DC active fiber. The output end of the 15-m-long fiber (the length was chosen to maximize optical-to-optical efficiency versus absorbed pump power) had a straight cleave used as an outcoupling Fresnel mirror. With this fiber length maximum of 101W of launched power at 1532.5nm (after the coupler and FBG) resulted in a maximum of 84.1W of power absorbed in the fiber.

In this FBG laser experiment the 1590nm output was spectrally pure. It was obtained with the ASE level never exceeding the 35dB below the signal level (see Fig. 3 ) and up to the maximum output power.

Typical FBG fiber laser output with a loosely coiled LMA fiber was multimode (two to three lower-order modes were most often seen) and unstable in time (transverse mode hopping was dynamically observed). Stable nearly diffraction-limited operation was achieved, with the penalty in efficiency of less than 5%, by partial coiling of the Er60-20/125 DC LMA fiber to a diameter of 810cm. The far-field pattern of the fiber laser output in this case is shown in Fig. 4 .

In conclusion, we demonstrated highly scalable, efficient, ultralow quantum defect (3.75%) operation of the resonantly cladding-pumped, Yb-free, Er-doped FBG laser based on a COTS LMA fiber. We believe this is the first reported resonantly cladding-pumped, FBG-based, Er-doped LMA fiber laser. Obtained narrowband output of 47.6W at 1590nm is believed to be the highest power ever reported from a Yb-free Er-doped fiber laser. The laser operating with no power saturation effects is assumed to be strictly pump limited and can be further scaled significantly. Currently achieved optical-to-optical efficiency of 56.7%, to the best of our knowledge, is the highest efficiency reported for a cladding-pumped unidirectionally emitting Er-doped laser. This efficiency is clearly far from QD-limited operation, which indicates that there are other efficiency-limiting factors likely associated with upconversion, nonradiative losses due to Er ion clustering, as well as the presence of trace water amounts in this particular COTS fiber. Yb-free Er-doped DC fibers for clad pumping are currently grossly underdeveloped. With specialty Er fibers developed specifically for the power scaling conversion efficiency can be increased to a QD-limited level, very similar to Yb-doped fiber lasers.

This work was partially supported by the High Energy Laser Joint Technology Office.

Fig. 1 Optical layout of the resonantly cladding-pumped, Yb-free, Er-doped fiber laser based on a COTS Liekki Er60-20/125DC fiber pumped at 1532.5nm. Laser cavity consists of the high-reflectivity FBG mirror and the straight cleave at the output fiber end.
Fig. 2 Output versus absorbed pump-power dependence obtained for the resonantly cladding-pumped Er-doped FBG laser shown in Fig. 1. The line is the linear regression of the data points presented by open circles.
Fig. 3 Spectral output of the FBG laser shown in Fig. 1 (ANDO AQ6370 optical spectrum analyzer, resolution 0.05nm). Indicated in Fig. 3 are: residual pump, the leaked unabsorbed pump power at 1532.5nm; ASE, amplified spontaneous emission; lasing, the underresolved (on the scale shown in Fig. 3) FBG-controlled fiber laser emission at 1590nm.
Fig. 4 Far-field pattern of the laser output beam for the resonantly cladding-pumped, Yb-free, Er-doped FBG laser after stripping the higher-order modes by proper fiber coiling.
1.

D. Y. Shen, J. K. Sahu, and W. A. Clarkson, Opt. Express 13, 4916 (2005). [CrossRef] [PubMed]

2.

H. M. Pask, R. J. Chapman, D. C. Hanna, A. C. Tropper, C. J. Mackechnie, P. R. Barber, and J. M. Dawes, IEEE J. Sel. Top. Quantum Electron. 1, 2 (1995). [CrossRef]

3.

M. Dubinskii, J. Zhang, and V. Ter-Mikirtychev, Electron. Lett. 45, 400 (2009). [CrossRef]

4.

M. L. Osowski, W. Hu, R. M. Lammert, S. W. Oh, P. T. Rudy, T. Stakelon, L. Vaissie, and J. E. Ungar, Proc. SPIE 6952, 695208 (2008). [CrossRef]

5.

D. T. Walton, L. A. Zenteno, A. Ellison, J. Anderson, X. Liu, L. Hughes, C. Caneau, and C. E. Zah, in Conference on Lasers and Electro-Optics/International Quantum Electronics Conference and Photonic Applications Systems Technologies, Technical Digest (CD) (Optical Society of America, 2004), paper CMK5.

6.

J. D. Minelly, V. Stasyuk, J. P. de Sandro, E. Gagnon, and S. Chatigny, presented at Optical Amplifiers and their Applications (OAA 2004), San Francisco, Calif., June 27–30 2004, postdeadline paper PD4-1.

7.

M. Dubinskii, J. Zhang, and I. Kudryashov, Appl. Phys. Lett. 93, 031111 (2008). [CrossRef]

OCIS Codes
(140.3480) Lasers and laser optics : Lasers, diode-pumped
(140.3500) Lasers and laser optics : Lasers, erbium
(140.3510) Lasers and laser optics : Lasers, fiber

ToC Category:
Lasers and Laser Optics

History
Original Manuscript: February 17, 2009
Revised Manuscript: April 7, 2009
Manuscript Accepted: April 10, 2009
Published: May 5, 2009

Citation
M. Dubinskii, J. Zhang, and V. Ter-Mikirtychev, "Highly scalable, resonantly cladding-pumped, Er-doped fiber laser with record efficiency," Opt. Lett. 34, 1507-1509 (2009)
http://www.opticsinfobase.org/ol/abstract.cfm?URI=ol-34-10-1507


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References

  1. D. Y. Shen, J. K. Sahu, and W. A. Clarkson, Opt. Express 13, 4916 (2005). [CrossRef] [PubMed]
  2. H. M. Pask, R. J. Chapman, D. C. Hanna, A. C. Tropper, C. J. Mackechnie, P. R. Barber, and J. M. Dawes, IEEE J. Sel. Top. Quantum Electron. 1, 2 (1995). [CrossRef]
  3. M. Dubinskii, J. Zhang, and V. Ter-Mikirtychev, Electron. Lett. 45, 400 (2009). [CrossRef]
  4. M. L. Osowski, W. Hu, R. M. Lammert, S. W. Oh, P. T. Rudy, T. Stakelon, L. Vaissie, and J. E. Ungar, Proc. SPIE 6952, 695208 (2008). [CrossRef]
  5. D. T. Walton, L. A. Zenteno, A. Ellison, J. Anderson, X. Liu, L. Hughes, C. Caneau, and C. E. Zah, in Conference on Lasers and Electro-Optics/International Quantum Electronics Conference and Photonic Applications Systems Technologies, Technical Digest (CD) (Optical Society of America, 2004), paper CMK5.
  6. J. D. Minelly, V. Stasyuk, J. P. de Sandro, E. Gagnon, and S. Chatigny, presented at Optical Amplifiers and their Applications (OAA 2004), San Francisco, Calif., June 27-30 2004, postdeadline paper PD4-1.
  7. M. Dubinskii, J. Zhang, and I. Kudryashov, Appl. Phys. Lett. 93, 031111 (2008). [CrossRef]

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