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High optical gain in KGdxLuyEr1-x-y(WO4)2 waveguide amplifiers despite energy-transfer upconversion

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18th International Conference on Luminescence – ICL 2017, from August 27th to September 1st 2017, João Pessoa, Paraíba, Brazil.

High optical gain in KGd

x

Lu

y

Er

1-x-y

(WO

4

)

2

waveguide amplifiers

despite energy-transfer upconversion

S. A. Vázquez-Córdova1,*, S. Aravazhi2, C. Grivas3, Y. S. Yong1,

S. M. García-Blanco1, J. L. Herek1, M. Pollnau2,4

1 Optical Sciences, MESA+ Institute, University of Twente, Enschede, The Netherlands 2 Integrated Optical Microsystems, MESA+ Institute, University of Twente, Enschede, The Netherlands

3 School of Physics and Astronomy, University of Southampton, United Kingdom

4 Department of Materials and Nano Physics, KTH – Royal Institute of Technology, Kista, Sweden

* Corresponding author: s.a.vazquezcordova-1@utwente.nl

A crucial enabling function in integrated optics is amplification of optical signals at 1.5 µm. Whereas rare-earth-doped amplifiers allow for high-speed signal transmission at THz bit rates, typically they deliver an internal net gain per unit length of only a few dB/cm [1]. The rare-earth-doped potassium double tungstates KY(WO4)2, KGd(WO4)2, and KLu(WO4)2

[2] are especially suited for optical amplification due to the high transition cross-sections of rare-earth ions in these materials [3]. Recently an internal net gain of ~1000 dB/cm has been demonstrated in ytterbium-doped thin films [1].

Here we report optical gain at 1.53 µm in KGdxLuyEr1-x-y(WO4)2 channel waveguides

doped with five different Er3+ concentrations of 0.75, 1.5, 3, 6, and 10 at.%, grown by liquid-phase epitaxy (LPE) onto undoped KY(WO4)2 substrates [4] and microstructured by Ar+

etching. When pumping at 980 nm, a very high internal net gain of 13 dB/cm is experimentally demonstrated, despite the fact that the intrinsic propagation losses in these surface waveguides were as high as 4 dB/cm.

When increasing the erbium concentration and population density of the 4I13/2

amplifier level to achieve higher gain, the probability of ETU increases linearly with erbium concentration and quadratically with the 4I13/2 population density. For determining the

macroscopic ETU parameter WETU, we measured the luminescence-decay curves in channel

waveguides with all five Er3+ concentrations, each at 4 different values of the pump power. The extracted concentration-independent donor-donor and donor-acceptor microscopic parameters are CDD = 5.4  10-39 cm6/s and CDA = 4.9 -40 cm6/s, respectively, from which

WETU was calculated as a function of doping concentration. The gain was simulated by use of

a rate-equation system, thereby confirming that ETU limits the available gain.

Using buried channel waveguides, whose intrinsic propagation losses are only 0.2 dB/cm, and optimizing the Er3+ concentration and waveguide length to ~3 cm, for 500 mW of launched pump power a total gain of ~40 dB is predicted, thereby underlining that Er3+-doped potassium double tungstates are extremely high-performing amplifiers at 1.5 µm.

Keywords: rare-earth amplifier, erbium, channel waveguide, potassium double tungstate.

References

[1] D. Geskus, S. Aravazhi, S. M. García-Blanco, M. Pollnau, Adv. Mater. 24 (2012) OP19– OP22.

[2] M. Pollnau, Y. E. Romanyuk, F. Gardillou, C. N. Borca, U. Griebner, S. Rivier, V. Petrov, IEEE J. Sel. Top. Quantun Electron. 13 (2007) 661–671.

[3] N. V. Kuleshov, A. A. Lagatsky, V. G. Shcherbitsky, V. P. Mikhailov, E. Heumann, T. Jensen, A. Diening, G. Huber, Appl. Phys. B 64 (1997) 409–413.

[4] S. Aravazhi, D. Geskus, K. van Dalfsen, S. A. Vázquez-Córdova, C. Grivas, U. Griebner, S. M. García-Blanco, M. Pollnau, Appl. Phys. B 111 (2013) 433–446.

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