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Optics Express

Optics Express

  • Editor: Michael Duncan
  • Vol. 14, Iss. 25 — Dec. 11, 2006
  • pp: 12183–12187
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Optical bistability in the operation of a continuous-wave diode-pumped Yb:LuVO4 laser

Junhai Liu, Valentin Petrov, Uwe Griebner, Frank Noack, Huaijin Zhang, Jiyang Wang, and Minhua Jiang  »View Author Affiliations


Optics Express, Vol. 14, Issue 25, pp. 12183-12187 (2006)
http://dx.doi.org/10.1364/OE.14.012183


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Abstract

We report on sizable optical bistability in the operation of a continuous-wave diode-pumped Yb:LuVO4 laser, as a result of the resonant reabsorption losses in the laser crystal which increase with the temperature. Significant intensity fluctuations have been observed in a small operational region near the critical point.

© 2006 Optical Society of America

1. Introduction

Since its first discovery in late 1907’s, optical bistability has been found existing in many different optical systems. Generally, these optical systems fall into two categories: passive cavities containing either a saturable absorbing or a nonlinear dispersive medium, and laser systems with intracavity saturable absorbers [1

1. A. E. Siegman, Lasers (University Science, Mill Valley, Calif., 1986), Chap. 13.7.

, 2

2. R. W. Boyd, Nonlinear Optics (Academic Press, Inc., San Diego, Calif., 1992), Chap. 6.3.

]. Recently, a different kind of so-called intrinsic optical bistability was discovered in some active optical materials such as Yb:Cs3Lu2Br9 and Yb:YCa4O(BO3)3, in which the intensity of cooperative luminescence exhibits bistable behavior [3

3. D. R. Gamelin, S. R. Lüthi, and H. U. Güdel, “The role of laser heating in the intrinsic optical bistability of Yb3+-doped bromide lattices,” J. Phys. Chem. B 104, 11045–11057 (2000). [CrossRef]

,4

4. Ph. Goldner, O. Guillot-Noël, and P. Higel, “Optical bistability in Yb3+:YCa4O(BO3)3 crystal,” Opt. Mater. 26, 281–286 (2004). [CrossRef]

].

The first clear demonstration of optical bistability in lasers was reported nearly three decades ago using a CO2 laser with a SF6 cell serving as the saturable absorber [5

5. S. Ruschin and S. H. Bauer, “Bistability, hysteresis and critical behavior of a CO2 laser, with SF6 intracavity as a saturable absorber,” Chem. Phys. Lett. 66, 100–103 (1979). [CrossRef]

]. Since then it has been observed in many types of lasers, such as the semiconductor laser with a split resonator [6

6. T. G. Dziura, “Beyond mean field and plane wave theories of bistable semiconductor lasers,” IEEE J. Quantum Electron. 22, 651–654 (1986). [CrossRef]

], the two-section InAs quantum dot laser [7

7. X. Huang, A. Stintz, H. Li, A. Rice, G. T. Liu, L. F. Lester, J. Cheng, and K. J. Malloy, “Bistable operation of a two-section 1.3-µm InAs quantum dot laser—absorption saturation and the quantum confined Stark effect,” IEEE J. Quantum Electron. 37, 414–417 (2001). [CrossRef]

], the Er-doped fiber ring laser [8

8. J. M. Oh and D. Lee, “Strong optical bistability in a simple L-band tunable erbium-doped fiber ring laser,” IEEE J. Quantum Electron. , 40, 374–377 (2004). [CrossRef]

], and the twin-microdisk laser developed very recently [9

9. S. Ishii and T. Baba, “Bistable lasing in twin microdisk photonic molecules,” Appl. Phys. Lett. 87, 181102-1–3 (2005). [CrossRef]

]. So far, however, such optical bistability has not been observed in solid-state lasers.

One common feature of the different lasers mentioned above is the presence of an effective intracavity saturable absorber which is responsible for the occurrence of the optical bistability. In this respect, the trivalent Yb ion is of particular interest, it has a [Xe]4f13 electronic configuration, giving rise to two spin-orbit split terms 2F7/2 and 2F5/2. In the crystal field of the host, each term will further split, forming a ground state manifold (2F7/2) and an excited state manifold (2F5/2). Therefore, an Yb-laser operating at room temperature will always suffer inevitable resonant losses arising from the thermal population of the terminal level which depend on the ground state splitting for the given host. However, such resonant losses, in principle, can simultaneously act as an inherent effective saturable absorber, and result, under certain circumstances, in optical bistability. Here, we report our observation of optical bistability in the operation of a continuous-wave (cw) Yb:LuVO4 laser end-pumped by a high-power laser diode.

2. Experimental results and discussion

For the present experiment, a 2-mm-thick a-cut Yb:LuVO4 crystal with an aperture of 4×4 mm2 was used. It was coated for high transmission at both the expected laser (~1040 nm) and the pump (985 nm) wavelength. The Yb concentration was 1.56 at. % which results in a small signal absorption of ~70% for the π- and ~36% for the σ-polarization at pumping wavelengths near 980 nm. The crystal was placed inside a compact plano-concave cavity, very close to the flat mirror through which the focused pump beam with NA=0.2 was coupled into the cavity. The pump spot radius in the position of the crystal was ~100 µm. The pump light was unpolarized. The temperature of the copper holder in which the crystal was fixed was maintained at 15°C by use of a water-cooling system. Several 25-mm radius-ofcurvature concave mirrors with transmission ranging from T=0.5% to 2% were used as output couplers. The physical cavity length was 22 mm.

Fig. 1. Dependence of the output power of the Yb:LuVO4 laser on the absorbed pump power, showing a sizable hysteresis loop.

The hysteresis loop itself can be qualitatively explained by continuous heating of the crystal followed by stronger reabsorption, which increases the threshold and makes it necessary to further increase the pump level which in turn produces even more heat. In the absence of lasing (below the up-threshold), when increasing the pump power, nonradiative relaxation processes play an important role. In contrast, when starting from the lasing condition and decreasing the pump power, the stimulated emission increases the part of the radiative relaxation suppressing the nonradiative part which leads to less heat production and reduced down-threshold. The real situation is much more complicated because in the threshold regions both the wavelength and the polarization might change during the transition between the two states. The above explanation based on the role of the thermal effects is consistent with the observed narrowing of the hysteresis region to 0.7 and 0.3 W in terms of Pabs when the output coupler transmission was increased to T = 1% and 2%, respectively. Nevertheless, the fact that the hysteresis loop was observed also with the chopper means that the physical effect behind the bistability is strongly affected by the temperature but heating is not solely responsible for it.

Fig. 2. Oscilloscope traces of the laser output showing the intensity fluctuations near the upthreshold. The traces from (a) to (e) were recorded when the pump power was decreased through the up-threshold point. The horizontal time scale is 0.1 ms/div.

Bistable operation was clearly predicted within the theoretical model used by Lugiato et al. [11

11. L. A. Lugiato, P. Mandel, S. T. Dembinski, and A. Kossakowski, “Semiclassical and quantum theories of bistability in lasers containing saturable absorbers,” Phys. Rev. A 18, 238–254 (1978). [CrossRef]

] for a laser having an absorbing medium inside its resonator. Another interesting effect accompanying the bistability are the significant intensity fluctuations expected to occur in the transition region near the critical point (up-threshold) [11

11. L. A. Lugiato, P. Mandel, S. T. Dembinski, and A. Kossakowski, “Semiclassical and quantum theories of bistability in lasers containing saturable absorbers,” Phys. Rev. A 18, 238–254 (1978). [CrossRef]

]. Indeed, such fluctuations were observed in the present Yb:LuVO4 laser on sub-millisecond time scale when passing this region starting from the lasing state. Figure 2 shows a series of oscilloscope traces of the laser output recorded while the pump power was decreased through the up-threshold point (from (a) to (e)). Near the critical point, the region in which the fluctuations were observed covered a pump power range corresponding to ΔPabs = 0.6 W, the most significant fluctuations occurring close to the up-threshold point.

Table 1. Absorbed pump power at threshold for different Yb-doped crystals (for vanadates, PthPth, up)*

table-icon
View This Table

We have observed bistable laser operation under similar experimental conditions also in other Yb-doped vanadates including Yb:YVO4, Yb:GdVO4, and Yb:LuxGd1-xVO4. We studied several other different Yb-doped crystals, such as KLu(WO4)2, NaGd(WO4)2, YAl3(BO3)4, GdCa4O(BO3)3, Ca3(NbGa)2-xGa3O12, etc., searching for bistable laser operation, but with none of them was it possible to observe a hysteresis loop in the input-output characteristics. Thus optical bistability seems to be a common feature only of the Yb-doped vanadate lasers. What distinguish the Yb-doped vanadates studied by us from other Yb-doped crystals are the higher pump levels required to reach the laser threshold under identical resonator conditions (Table 1). As can be seen from the table, the laser thresholds of the Ybdoped vanadates were roughly 3–5 times higher than those of the other crystals. The (resonant) losses which are responsible for the increased thresholds of the Yb-doped vanadates lasers might be strongly dependent on the crystal temperature and the same holds for the magnitude of the observed bistability effect. Given the strong effect of temperature one can expect that the bistable behavior will depend on the thermal conductivity. It is known that tungstates have lower thermal conductivity than vanadates but no reliable data exist in the literature on the influence of Yb-doping on the thermal conductivity of the different vanadates and tungstates and this influence can be strong and dependent on the passive ion (Y, Gd, or Lu) that is substituted in the host. While the spectroscopic features of Yb seem similar in the different hosts, at present one cannot rule out the possibility that some additional heating (also below the laser threshold) is caused by existing or induced absorbing defect centers, which even do not affect the measured fluorescence lifetime and the estimated quantum efficiency, because all Yb-doped vanadates are still in the initial stage of their development.

3. Conclusion

In summary, we have observed, for the first time to our knowledge, sizable optical bistability in the operation of a diode-pumped Yb:LuVO4 laser, which is attributed to resonant absorption losses in the active medium affected by the thermal load. Significant output fluctuations occur in the transition region near the up-threshold, which is in agreement with theoretical predictions. Such optical bistability seems common to all Yb-doped vanadate lasers.

Acknowledgments

This work was supported by the EU project DT-CRYS, NMP3-CT-2003-505580, the National Natural Science Foundation of China (No. 50572054), the Excellent Young Teachers Program of MOE, China, and the Grant for State Key Program of China (2004CB619002).

References and links

1.

A. E. Siegman, Lasers (University Science, Mill Valley, Calif., 1986), Chap. 13.7.

2.

R. W. Boyd, Nonlinear Optics (Academic Press, Inc., San Diego, Calif., 1992), Chap. 6.3.

3.

D. R. Gamelin, S. R. Lüthi, and H. U. Güdel, “The role of laser heating in the intrinsic optical bistability of Yb3+-doped bromide lattices,” J. Phys. Chem. B 104, 11045–11057 (2000). [CrossRef]

4.

Ph. Goldner, O. Guillot-Noël, and P. Higel, “Optical bistability in Yb3+:YCa4O(BO3)3 crystal,” Opt. Mater. 26, 281–286 (2004). [CrossRef]

5.

S. Ruschin and S. H. Bauer, “Bistability, hysteresis and critical behavior of a CO2 laser, with SF6 intracavity as a saturable absorber,” Chem. Phys. Lett. 66, 100–103 (1979). [CrossRef]

6.

T. G. Dziura, “Beyond mean field and plane wave theories of bistable semiconductor lasers,” IEEE J. Quantum Electron. 22, 651–654 (1986). [CrossRef]

7.

X. Huang, A. Stintz, H. Li, A. Rice, G. T. Liu, L. F. Lester, J. Cheng, and K. J. Malloy, “Bistable operation of a two-section 1.3-µm InAs quantum dot laser—absorption saturation and the quantum confined Stark effect,” IEEE J. Quantum Electron. 37, 414–417 (2001). [CrossRef]

8.

J. M. Oh and D. Lee, “Strong optical bistability in a simple L-band tunable erbium-doped fiber ring laser,” IEEE J. Quantum Electron. , 40, 374–377 (2004). [CrossRef]

9.

S. Ishii and T. Baba, “Bistable lasing in twin microdisk photonic molecules,” Appl. Phys. Lett. 87, 181102-1–3 (2005). [CrossRef]

10.

J. Liu, X. Mateos, H. Zhang, J. Wang, M. Jiang, U. Griebner, and V. Petrov, “Continuous-wave laser operation of Yb:LuVO4,” Opt. Lett. 30, 3162–3164 (2005). [CrossRef] [PubMed]

11.

L. A. Lugiato, P. Mandel, S. T. Dembinski, and A. Kossakowski, “Semiclassical and quantum theories of bistability in lasers containing saturable absorbers,” Phys. Rev. A 18, 238–254 (1978). [CrossRef]

OCIS Codes
(140.3480) Lasers and laser optics : Lasers, diode-pumped
(140.3580) Lasers and laser optics : Lasers, solid-state
(140.5680) Lasers and laser optics : Rare earth and transition metal solid-state lasers

ToC Category:
Lasers and Laser Optics

History
Original Manuscript: October 16, 2006
Revised Manuscript: November 23, 2006
Manuscript Accepted: November 26, 2006
Published: December 11, 2006

Citation
Junhai Liu, Valentin Petrov, Uwe Griebner, Frank Noack, Huaijin Zhang, Jiyang Wang, and Minhua Jiang, "Optical bistability in the operation of a continuous-wave diode-pumped Yb:LuVO4 laser," Opt. Express 14, 12183-12187 (2006)
http://www.opticsinfobase.org/oe/abstract.cfm?URI=oe-14-25-12183


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References

  1. A. E. Siegman, Lasers (University Science, Mill Valley, Calif., 1986), Chap. 13.7.
  2. R. W. Boyd, Nonlinear Optics (Academic Press, Inc., San Diego, Calif., 1992), Chap. 6.3.
  3. D. R. Gamelin, S. R. Lüthi, and H. U. Güdel, "The role of laser heating in the intrinsic optical bistability of Yb3+-doped bromide lattices," J. Phys. Chem. B 104, 11045-11057 (2000). [CrossRef]
  4. Ph. Goldner, O. Guillot-Noël, and P. Higel, "Optical bistability in Yb3+:YCa4O(BO3)3 crystal," Opt. Mater. 26, 281-286 (2004). [CrossRef]
  5. S. Ruschin and S. H. Bauer, "Bistability, hysteresis and critical behavior of a CO2 laser, with SF6 intracavity as a saturable absorber," Chem. Phys. Lett. 66, 100-103 (1979). [CrossRef]
  6. T. G. Dziura, "Beyond mean field and plane wave theories of bistable semiconductor lasers," IEEE J. Quantum Electron. 22, 651-654 (1986). [CrossRef]
  7. X. Huang, A. Stintz, H. Li, A. Rice, G. T. Liu, L. F. Lester, J. Cheng, and K. J. Malloy, "Bistable operation of a two-section 1.3-μm InAs quantum dot laser—absorption saturation and the quantum confined Stark effect," IEEE J. Quantum Electron. 37, 414-417 (2001). [CrossRef]
  8. J. M. Oh and D. Lee, "Strong optical bistability in a simple L-band tunable erbium-doped fiber ring laser," IEEE J. Quantum Electron.,  40, 374-377 (2004). [CrossRef]
  9. S. Ishii and T. Baba, "Bistable lasing in twin microdisk photonic molecules," Appl. Phys. Lett . 87, 181102-1-3 (2005). [CrossRef]
  10. J. Liu, X. Mateos, H. Zhang, J. Wang, M. Jiang, U. Griebner, and V. Petrov, "Continuous-wave laser operation of Yb:LuVO4," Opt. Lett. 30, 3162-3164 (2005). [CrossRef] [PubMed]
  11. L. A. Lugiato, P. Mandel, S. T. Dembinski, and A. Kossakowski, "Semiclassical and quantum theories of bistability in lasers containing saturable absorbers," Phys. Rev. A 18, 238-254 (1978). [CrossRef]

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