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Optics Express

Optics Express

  • Editor: C. Martijn de Sterke
  • Vol. 20, Iss. 9 — Apr. 23, 2012
  • pp: 9940–9947
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Passively Q-switched 1.5-1.6 μm Er:Yb:LuAl3(BO3)4 laser with Co2+:Mg0.4Al2.4O4 saturable absorber

Yujin Chen, Yanfu Lin, Yuqi Zou, Zundu Luo, and Yidong Huang  »View Author Affiliations


Optics Express, Vol. 20, Issue 9, pp. 9940-9947 (2012)
http://dx.doi.org/10.1364/OE.20.009940


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Abstract

Using a Co2+:Mg0.4Al2.4O4 spinel crystal as saturable absorber, efficient passively Q-switched pulse laser operating at 1.5-1.6 μm was realized in an Er:Yb:LuAl3(BO3)4 crystal end-pumped by a 970 nm diode laser. At absorbed pump power of 15.7 W, 1540 nm laser with 28.6 μJ energy, 40 ns duration and 22 kHz repetition rate, and 1520 nm laser with 9.9 μJ energy, 37 ns duration and 63 kHz repetition rate were obtained in a plano-concave cavity, respectively. For a plano-plano cavity, corresponding values of 1520 nm laser were 16.3 μJ, 14 ns and 41 kHz, respectively, and the maximum output peak power was about 1.16 kW.

© 2012 OSA

1. Introduction

Eye-safe 1.5-1.6 μm pulse lasers emitted from a compact source are of potential interest in some areas, such as sensing of gases and contamination in air, medicine, laser-range-finding, and lidar [1

1. P. Laporta, S. Taccheo, S. Longhi, O. Svelto, and C. Svelto, “Erbium-ytterbium microlasers: optical properties and lasing characteristics,” Opt. Mater. 11(2-3), 269–288 (1999). [CrossRef]

, 2

2. R. Häring, R. Paschotta, R. Fluck, E. Gini, H. Melchior, and U. Keller, “Passively Q-switched microchip laser at 1.5 μm,” J. Opt. Soc. Am. B 18(12), 1805–1812 (2001). [CrossRef]

]. Passive Q-switching of Er-Yb solid-state laser is an attractive technique developed for these applications, because it makes1.5-1.6 μm pulse laser device with kilowatt-level peak power and nanosecond duration compact and low-cost [2

2. R. Häring, R. Paschotta, R. Fluck, E. Gini, H. Melchior, and U. Keller, “Passively Q-switched microchip laser at 1.5 μm,” J. Opt. Soc. Am. B 18(12), 1805–1812 (2001). [CrossRef]

, 3

3. S. A. Zolotovskaya, K. V. Yumashev, N. V. Kuleshov, and A. V. Sandulenko, “Diode-pumped Yb,Er:glass laser passively Q switched with a V3+:YAG crystal,” Appl. Opt. 44(9), 1704–1708 (2005). [CrossRef] [PubMed]

].

For Er-Yb codoped crystals, few investigations of passively Q-switched 1.5-1.6 μm laser operation have been reported till now [4

4. J. E. Hellström, G. Karlsson, V. Pasiskevicius, F. Laurell, B. Denker, S. Sverchkov, B. Galagan, and L. Ivleva, “Passive Q-switching at 1.54 μm of an Er-Yb:GdCa4O(BO3)3 laser with a Co2+:MgAl2O4 saturable absorber,” Appl. Phys. B 81(1), 49–52 (2005). [CrossRef]

, 5

5. N. A. Tolstik, A. E. Troshin, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. N. Matrosov, T. A. Matrosova, and M. I. Kupchenko, “Spectroscopy, continuous-wave and Q-switched diode pumped laser operation of Er3+, Yb3+:YVO4 crystal,” Appl. Phys. B 86(2), 275–278 (2007). [CrossRef]

]. With a Co2+:MgAl2O4 crystal as saturable absorber, 1540 nm pulse laser with energy of about 2.8 μJ and duration of 5-6 ns, and 1604 nm pulse laser with energy of 4.3 μJ and duration of 150 ns have been realized in Er:Yb:GdCa4O(BO3)3 and Er:Yb:YVO4 crystals, respectively [4

4. J. E. Hellström, G. Karlsson, V. Pasiskevicius, F. Laurell, B. Denker, S. Sverchkov, B. Galagan, and L. Ivleva, “Passive Q-switching at 1.54 μm of an Er-Yb:GdCa4O(BO3)3 laser with a Co2+:MgAl2O4 saturable absorber,” Appl. Phys. B 81(1), 49–52 (2005). [CrossRef]

, 5

5. N. A. Tolstik, A. E. Troshin, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. N. Matrosov, T. A. Matrosova, and M. I. Kupchenko, “Spectroscopy, continuous-wave and Q-switched diode pumped laser operation of Er3+, Yb3+:YVO4 crystal,” Appl. Phys. B 86(2), 275–278 (2007). [CrossRef]

]. The obtained maximum output peak powers are only about 0.5 kW and 0.03 kW, respectively. Among Er-Yb codoped crystals, Er:Yb:YAl3(BO3)4 (Er:Yb:YAB) crystal has been considered as the best 1.5-1.6 μm laser crystal for continuous-wave (cw) 970 nm diode pumping [6

6. N. A. Tolstik, V. E. Kisel, N. V. Kuleshov, V. V. Maltsev, and N. I. Leonyuk, “Er,Yb:YAl3(BO3)4-efficient 1.5 μm laser crystal,” Appl. Phys. B 97(2), 357–362 (2009). [CrossRef]

]. 1.5-1.6 μm cw laser with output power of 1 W and slope efficiency of 35%, and passively mode-locked 1530 nm pulse laser with duration of 4.8 ps and average output power of 280 mW have been realized in Er:Yb:YAB crystal [7

7. N. A. Tolstik, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. V. Maltsev, O. V. Pilipenko, E. V. Koporulina, and N. I. Leonyuk, “Efficient 1 W continuous-wave diode-pumped Er,Yb:YAl3(BO3)4 laser,” Opt. Lett. 32(22), 3233–3235 (2007). [CrossRef] [PubMed]

, 8

8. A. A. Lagatsky, V. E. Kisel, A. E. Troshin, N. A. Tolstik, N. V. Kuleshov, N. I. Leonyuk, A. E. Zhukov, E. U. Rafailov, and W. Sibbett, “Diode-pumped passively mode-locked Er,Yb:YAl3(BO3)4 laser at 1.5-1.6 microm,” Opt. Lett. 33(1), 83–85 (2008). [CrossRef] [PubMed]

], which show that the crystal has better laser performance than that of the commercially available Er:Yb:phosphate glasses. Therefore, as a member of the same family, Er:Yb:LuAl3(BO3)4 (Er:Yb:LuAB) crystal should also be an interesting and valuable 1.5-1.6 μm laser crystal [9

9. Y. J. Chen, Y. F. Lin, J. H. Huang, X. H. Gong, Z. D. Luo, and Y. D. Huang, “Spectroscopic and laser properties of Er(3+):Yb(3+):LuAl(3)(BO(3))(4) crystal at 1.5-1.6 microm,” Opt. Express 18(13), 13700–13707 (2010), http://www.opticsinfobase.org/abstract.cfm?uri=oe-18-13-13700. [CrossRef] [PubMed]

].

Similar to the Co2+:MgAl2O4 crystal, Co2+-doped alumina-rich Mg0.4Al2.4O4 spinel crystal is a novel saturable absorber for Q-switching of 1.5-1.6 μm lasers [10

10. D. P. Jiang, Y. Q. Zhou, L. B. Su, H. L. Tang, F. Wu, L. H. Zheng, H. J. Li, and J. Xu, “A Co2+-doped alumina-rich Mg0.4Al2.4O4 spinel crystal as saturable absorber for a LD pumped Er:glass microchip laser at 1535nm,” Laser Phys. Lett. 8(5), 343–348 (2011). [CrossRef]

]. Its ground-state absorption cross-section at 1535 nm is about 2.54 × 10−19 cm2. Using a Co2+:Mg0.4Al2.4O4 crystal as saturable absorber, 1535 nm pulse laser with energy of 4.8 μJ and duration of 3.5 ns has been realized in Er:Yb:glass [10

10. D. P. Jiang, Y. Q. Zhou, L. B. Su, H. L. Tang, F. Wu, L. H. Zheng, H. J. Li, and J. Xu, “A Co2+-doped alumina-rich Mg0.4Al2.4O4 spinel crystal as saturable absorber for a LD pumped Er:glass microchip laser at 1535nm,” Laser Phys. Lett. 8(5), 343–348 (2011). [CrossRef]

]. In this work, using an Er:Yb:LuAB crystal as gain medium and a Co2+:Mg0.4Al2.4O4 as saturable absorber, efficient passively Q-switched 1.5-1.6 μm pulse laser with kilowatt-level peak power and ten-odd nanosecond duration is demonstrated when the gain medium is end-pumped by a 970 nm diode laser.

2. Laser experimental arrangement

End-pumped linear resonators were adopted in the experiment and the schematic of experimental setups are depicted in Fig. 1
Fig. 1 Experimental setups of the quasi-cw 970 nm diode-pumped passively Q-switched Er:Yb:LuAB lasers at 1.5–1.6 μm: (a) plano-concave cavity; (b) plano-plano cavity.
. A 0.7-mm-thick and c-cut Er(1.1 at.%):Yb(24.1 at.%):LuAB crystal chip was used as gain medium. A 970 nm fiber-coupled diode laser (800 μm diameter core) from Coherent Inc. was used as pump source. After passing a simple telescopic lens system (TLS), the pump beam was focused to a spot with waist radius of about 220 µm in the crystal chip. The uncoated crystal chip was attached on an aluminum slab with heat-conducting adhesive and there is a hole in the center of the slab to permit the passing of the pump and fundamental laser beams. For making the laser more compact, no other device was used to control the temperature of the chip, which was only cooled by the natural air. In order to reduce the influence of pump-induced thermal load on laser performance and avoid the fracture of the chip at high pump power, the diode laser was operated in quasi-cw mode. Pump pulse width was 2 ms and pulse period was 100 ms. Because the duty cycle of the used diode laser was 2%, average power mentioned hereinafter was the measured average power multiplied by fifty. About 85% of the incident pump power was absorbed by the crystal chip. A 1-mm-thick Co2+:Mg0.4Al2.4O4 crystal with Co2+ concentration of 0.02 at.% was used as saturable absorber and placed as close as possible to the Er:Yb:LuAB crystal. The saturable absorber wafer was antireflection coated and had an initial transmission of about 97% around 1530 nm. The flat input mirror (IM) of the laser resonator had 90% transmission at 970 nm and 99.8% reflectivity around 1530 nm. For the plano-concave cavity, two output mirrors (OMs) with a fixed 30 mm radius of curvature (RoC) and different transmissions (1.5% and 2.4%) around 1530 nm were used. In order to reduce the cavity loss, the length of the plano-concave cavity was set close to the RoC of OMs. For the plano-plano cavity, one flat OM with transmission of 4.6% around 1530 nm was used. The cavity length was kept at about 7 mm. Spectrum of the passively Q-switched Er:Yb:LuAB laser was recorded with a monochromator (Triax550, Jobin-Yvon) associated with a TE-cooled Ge detector (DSS-G025T, Jobin-Yvon). Pulse profile was measured by a 2 GHz InGaAs photodiode connected to a digital oscilloscope with bandwidths of 1 GHz (DSO6102A, Agilent).

3. Results and discussion

Figure 3
Fig. 3 Average output power of the passively Q-switched Er:Yb:LuAB laser as a function of absorbed pump power at 970 nm in plano-concave cavities.
shows average output power of the passively Q-switched Er:Yb:LuAB laser as a function of absorbed pump power in the plano-concave cavities. At absorbed pump power of 15.7 W, 1540 nm pulse laser with the maximum average output power of 0.63 W and slope efficiency of 8.1%, and 1520 nm pulse laser with the maximum average output power of 0.62 W and slope efficiency of 9.2% were achieved for the OMs with transmissions of 1.5% and 2.4%, respectively. The absorbed pump thresholds of the 1540 and 1520 nm lasers were about 8.0 and 9.0 W, respectively.

Figure 6
Fig. 6 Pulse repetition rate of the passively Q-switched Er:Yb:LuAB laser as a function of absorbed pump power at 970 nm in plano-concave cavities.
shows pulse repetition rate of the passively Q-switched Er:Yb:LuAB laser as a function of absorbed pump power in the plano-concave cavities. For the OM transmissions of 1.5% and 2.4%, pulse repetition rates increase from 8 to 22 kHz and from 15 to 63 kHz, respectively, when absorbed pump power is changed from 10 to 15.7 W. Furthermore, pulse durations of both lasers are almost kept invariant at various pump powers [12

12. J. J. Degnan, “Optimization of passively Q-switched lasers,” IEEE J. Quantum Electron. 31(11), 1890–1901 (1995). [CrossRef]

]. At absorbed pump power of 15.7 W, pulse energy and peak power of the 1540 nm laser were estimated to be about 28.6 μJ and 0.72 kW, respectively, for the OM transmission of 1.5%. For the OM transmission of 2.4%, the corresponding values of the 1520 nm laser decreased to be about 9.9 μJ and 0.27 kW, respectively.

Because laser pulse with higher peak power and shorter pulse duration can be obtained in a shorter resonator [12

12. J. J. Degnan, “Optimization of passively Q-switched lasers,” IEEE J. Quantum Electron. 31(11), 1890–1901 (1995). [CrossRef]

], the passively Q-switched Er:Yb:LuAB laser in a plano-plano cavity with 7 mm length was also investigated. Figure 7
Fig. 7 Average output power of the passively Q-switched Er:Yb:LuAB laser as a function of absorbed pump power at 970 nm in a plano-plano cavity. The inset shows the spectrum at absorbed pump power of 15.7 W.
shows average output power of the laser as a function of absorbed pump power at 970 nm. At absorbed pump power of 15.7 W, the maximum average output power and slope efficiency were 0.65 W and 10.5%, respectively, for the OM transmission of 4.6%. The absorbed pump threshold was about 9.5 W. Spectra were similar at various pump powers and laser wavelength was centered at 1520 nm, as shown in the inset of Fig. 7.

Pulse profile of the passively Q-switched Er:Yb:LuAB laser at absorbed pump power of 15.7 W in the plano-plano cavity is shown in Fig. 8
Fig. 8 Pulse train (a) and oscilloscope trace (b) of the passively Q-switched Er:Yb:LuAB laser at absorbed pump power of 15.7 W in a plano-plano cavity. Pulse repetition rate and duration are about 41 kHz and 14 ns, respectively.
. Pulse repetition rate is about 41 kHz and pulse duration is about 14 ns. When the OM transmission increases from 2.4% to 4.6%, laser wavelength is kept at 1520 nm and the influence of the increment of OM transmission on pulse repetition rate may be stronger than that of the reduction of reabsorption loss. Therefore, the pulse repetition rate obtained in the plano-plano cavity with OM transmission of 4.6% is lower than that n the plano-concave cavity with OM transmission of 2.4%. The pulse-to-pulse amplitude fluctuation and interpulse time jittering are about 13% and 7%, respectively. When absorbed pump power was reduced to 10 W, pulse repetition rate decreased to about 10 kHz and pulse duration was still kept at about 14 ns. The maximum pulse energy and output peak power of 1520 nm in the plano-plano cavity were estimated to be about 16.3 μJ and 1.16 kW, respectively. The obtained energy and peak power in this work are higher than those realized in the diode-pumped passively Q-switched Er:Yb:GdCa4O(BO3)3 (about 2.8 μJ and 0.5 kW) and Er:Yb:YVO4 (about 4.3 μJ and 0.03 kW) lasers [4

4. J. E. Hellström, G. Karlsson, V. Pasiskevicius, F. Laurell, B. Denker, S. Sverchkov, B. Galagan, and L. Ivleva, “Passive Q-switching at 1.54 μm of an Er-Yb:GdCa4O(BO3)3 laser with a Co2+:MgAl2O4 saturable absorber,” Appl. Phys. B 81(1), 49–52 (2005). [CrossRef]

, 5

5. N. A. Tolstik, A. E. Troshin, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. N. Matrosov, T. A. Matrosova, and M. I. Kupchenko, “Spectroscopy, continuous-wave and Q-switched diode pumped laser operation of Er3+, Yb3+:YVO4 crystal,” Appl. Phys. B 86(2), 275–278 (2007). [CrossRef]

]. When the resonator is further shortened in the future, the pulse duration can become shorter and the output peak power of the passively Q-switched Er:Yb:LuAB laser can be enhanced.

4. Conclusion

End-pumped by a 970 nm diode laser with 2% duty cycle, efficient passively Q-switched Er:Yb:LuAB pulse laser at 1.5-1.6 μm was realized when a Co2+:Mg0.4Al2.4O4 spinel crystal was used as saturable absorber. When the absorbed pump power was 15.7 W and the OM transmission increased from 1.5% to 2.4% in plano-concave cavities, wavelength of output laser was blue-shifted from 1540 to 1520 nm and pulse repetition rate was rapidly changed from 22 to 63 kHz, while pulse duration was kept at about 40 ns. For a plano-plano cavity, 1520 nm pulse laser with 16.3 μJ energy, 14 ns duration, 41 kHz repetition rate, and 1.16 kW peak power was obtained at absorbed pump power of 15.7 W.

Acknowledgments

This work has been supported by the National Natural Science Foundation of China (grants 91122033), the Natural Science Foundation of Fujian Province (grant 2011J01375), and the Knowledge Innovation Program of the Chinese Academy of Sciences (grant KJCX2-EW-H03-01).

References and links

1.

P. Laporta, S. Taccheo, S. Longhi, O. Svelto, and C. Svelto, “Erbium-ytterbium microlasers: optical properties and lasing characteristics,” Opt. Mater. 11(2-3), 269–288 (1999). [CrossRef]

2.

R. Häring, R. Paschotta, R. Fluck, E. Gini, H. Melchior, and U. Keller, “Passively Q-switched microchip laser at 1.5 μm,” J. Opt. Soc. Am. B 18(12), 1805–1812 (2001). [CrossRef]

3.

S. A. Zolotovskaya, K. V. Yumashev, N. V. Kuleshov, and A. V. Sandulenko, “Diode-pumped Yb,Er:glass laser passively Q switched with a V3+:YAG crystal,” Appl. Opt. 44(9), 1704–1708 (2005). [CrossRef] [PubMed]

4.

J. E. Hellström, G. Karlsson, V. Pasiskevicius, F. Laurell, B. Denker, S. Sverchkov, B. Galagan, and L. Ivleva, “Passive Q-switching at 1.54 μm of an Er-Yb:GdCa4O(BO3)3 laser with a Co2+:MgAl2O4 saturable absorber,” Appl. Phys. B 81(1), 49–52 (2005). [CrossRef]

5.

N. A. Tolstik, A. E. Troshin, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. N. Matrosov, T. A. Matrosova, and M. I. Kupchenko, “Spectroscopy, continuous-wave and Q-switched diode pumped laser operation of Er3+, Yb3+:YVO4 crystal,” Appl. Phys. B 86(2), 275–278 (2007). [CrossRef]

6.

N. A. Tolstik, V. E. Kisel, N. V. Kuleshov, V. V. Maltsev, and N. I. Leonyuk, “Er,Yb:YAl3(BO3)4-efficient 1.5 μm laser crystal,” Appl. Phys. B 97(2), 357–362 (2009). [CrossRef]

7.

N. A. Tolstik, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. V. Maltsev, O. V. Pilipenko, E. V. Koporulina, and N. I. Leonyuk, “Efficient 1 W continuous-wave diode-pumped Er,Yb:YAl3(BO3)4 laser,” Opt. Lett. 32(22), 3233–3235 (2007). [CrossRef] [PubMed]

8.

A. A. Lagatsky, V. E. Kisel, A. E. Troshin, N. A. Tolstik, N. V. Kuleshov, N. I. Leonyuk, A. E. Zhukov, E. U. Rafailov, and W. Sibbett, “Diode-pumped passively mode-locked Er,Yb:YAl3(BO3)4 laser at 1.5-1.6 microm,” Opt. Lett. 33(1), 83–85 (2008). [CrossRef] [PubMed]

9.

Y. J. Chen, Y. F. Lin, J. H. Huang, X. H. Gong, Z. D. Luo, and Y. D. Huang, “Spectroscopic and laser properties of Er(3+):Yb(3+):LuAl(3)(BO(3))(4) crystal at 1.5-1.6 microm,” Opt. Express 18(13), 13700–13707 (2010), http://www.opticsinfobase.org/abstract.cfm?uri=oe-18-13-13700. [CrossRef] [PubMed]

10.

D. P. Jiang, Y. Q. Zhou, L. B. Su, H. L. Tang, F. Wu, L. H. Zheng, H. J. Li, and J. Xu, “A Co2+-doped alumina-rich Mg0.4Al2.4O4 spinel crystal as saturable absorber for a LD pumped Er:glass microchip laser at 1535nm,” Laser Phys. Lett. 8(5), 343–348 (2011). [CrossRef]

11.

P. Burns, J. M. Dawes, P. Dekker, J. A. Piper, H. Zhang, and J. Wang, “CW diode-pumped microlaser operation at 1.5-1.6 μm in Er, Yb:YCOB,” IEEE Photon. Technol. Lett. 14(12), 1677–1679 (2002). [CrossRef]

12.

J. J. Degnan, “Optimization of passively Q-switched lasers,” IEEE J. Quantum Electron. 31(11), 1890–1901 (1995). [CrossRef]

13.

X. Zhang, A. Brenier, Q. Wang, Zh. Wang, J. Chang, P. Li, Sh. Zhang, Sh. Ding, and Sh. Li, “Passive Q-switching characteristics of Yb3+:Gd3Ga5O12 crystal,” Opt. Express 13(19), 7708–7719 (2005). [CrossRef] [PubMed]

OCIS Codes
(140.3380) Lasers and laser optics : Laser materials
(140.3500) Lasers and laser optics : Lasers, erbium
(140.3540) Lasers and laser optics : Lasers, Q-switched

ToC Category:
Lasers and Laser Optics

History
Original Manuscript: March 8, 2012
Revised Manuscript: April 6, 2012
Manuscript Accepted: April 10, 2012
Published: April 17, 2012

Citation
Yujin Chen, Yanfu Lin, Yuqi Zou, Zundu Luo, and Yidong Huang, "Passively Q-switched 1.5-1.6 μm Er:Yb:LuAl3(BO3)4 laser with Co2+:Mg0.4Al2.4O4 saturable absorber," Opt. Express 20, 9940-9947 (2012)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-20-9-9940


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References

  1. P. Laporta, S. Taccheo, S. Longhi, O. Svelto, and C. Svelto, “Erbium-ytterbium microlasers: optical properties and lasing characteristics,” Opt. Mater.11(2-3), 269–288 (1999). [CrossRef]
  2. R. Häring, R. Paschotta, R. Fluck, E. Gini, H. Melchior, and U. Keller, “Passively Q-switched microchip laser at 1.5 μm,” J. Opt. Soc. Am. B18(12), 1805–1812 (2001). [CrossRef]
  3. S. A. Zolotovskaya, K. V. Yumashev, N. V. Kuleshov, and A. V. Sandulenko, “Diode-pumped Yb,Er:glass laser passively Q switched with a V3+:YAG crystal,” Appl. Opt.44(9), 1704–1708 (2005). [CrossRef] [PubMed]
  4. J. E. Hellström, G. Karlsson, V. Pasiskevicius, F. Laurell, B. Denker, S. Sverchkov, B. Galagan, and L. Ivleva, “Passive Q-switching at 1.54 μm of an Er-Yb:GdCa4O(BO3)3 laser with a Co2+:MgAl2O4 saturable absorber,” Appl. Phys. B81(1), 49–52 (2005). [CrossRef]
  5. N. A. Tolstik, A. E. Troshin, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. N. Matrosov, T. A. Matrosova, and M. I. Kupchenko, “Spectroscopy, continuous-wave and Q-switched diode pumped laser operation of Er3+, Yb3+:YVO4 crystal,” Appl. Phys. B86(2), 275–278 (2007). [CrossRef]
  6. N. A. Tolstik, V. E. Kisel, N. V. Kuleshov, V. V. Maltsev, and N. I. Leonyuk, “Er,Yb:YAl3(BO3)4-efficient 1.5 μm laser crystal,” Appl. Phys. B97(2), 357–362 (2009). [CrossRef]
  7. N. A. Tolstik, S. V. Kurilchik, V. E. Kisel, N. V. Kuleshov, V. V. Maltsev, O. V. Pilipenko, E. V. Koporulina, and N. I. Leonyuk, “Efficient 1 W continuous-wave diode-pumped Er,Yb:YAl3(BO3)4 laser,” Opt. Lett.32(22), 3233–3235 (2007). [CrossRef] [PubMed]
  8. A. A. Lagatsky, V. E. Kisel, A. E. Troshin, N. A. Tolstik, N. V. Kuleshov, N. I. Leonyuk, A. E. Zhukov, E. U. Rafailov, and W. Sibbett, “Diode-pumped passively mode-locked Er,Yb:YAl3(BO3)4 laser at 1.5-1.6 microm,” Opt. Lett.33(1), 83–85 (2008). [CrossRef] [PubMed]
  9. Y. J. Chen, Y. F. Lin, J. H. Huang, X. H. Gong, Z. D. Luo, and Y. D. Huang, “Spectroscopic and laser properties of Er(3+):Yb(3+):LuAl(3)(BO(3))(4) crystal at 1.5-1.6 microm,” Opt. Express18(13), 13700–13707 (2010), http://www.opticsinfobase.org/abstract.cfm?uri=oe-18-13-13700 . [CrossRef] [PubMed]
  10. D. P. Jiang, Y. Q. Zhou, L. B. Su, H. L. Tang, F. Wu, L. H. Zheng, H. J. Li, and J. Xu, “A Co2+-doped alumina-rich Mg0.4Al2.4O4 spinel crystal as saturable absorber for a LD pumped Er:glass microchip laser at 1535nm,” Laser Phys. Lett.8(5), 343–348 (2011). [CrossRef]
  11. P. Burns, J. M. Dawes, P. Dekker, J. A. Piper, H. Zhang, and J. Wang, “CW diode-pumped microlaser operation at 1.5-1.6 μm in Er, Yb:YCOB,” IEEE Photon. Technol. Lett.14(12), 1677–1679 (2002). [CrossRef]
  12. J. J. Degnan, “Optimization of passively Q-switched lasers,” IEEE J. Quantum Electron.31(11), 1890–1901 (1995). [CrossRef]
  13. X. Zhang, A. Brenier, Q. Wang, Zh. Wang, J. Chang, P. Li, Sh. Zhang, Sh. Ding, and Sh. Li, “Passive Q-switching characteristics of Yb3+:Gd3Ga5O12 crystal,” Opt. Express13(19), 7708–7719 (2005). [CrossRef] [PubMed]

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