TY - JOUR
T1 - Atomic Layer Engineering of Er-Ion Distribution in Highly Doped Er:Al2O3 for Photoluminescence Enhancement
AU - Rönn, John
AU - Karvonen, Lasse
AU - Kauppinen, Christoffer
AU - Perros, Alexander Pyymaki
AU - Peyghambarian, Nasser
AU - Lipsanen, Harri
AU - Säynätjoki, Antti
AU - Sun, Zhipei
N1 - Funding Information: The authors acknowledge the financial support from Aalto ELEC doctoral school, TEKES - the Finnish Funding Agency for Innovation (FiDiPro: NP-Nano and OPEC), Academy of Finland (Grants: 276376, 284548, 285972), the European Unions Seventh Framework Programme (REA Grant Agreement No. 631610), and thank Micronova Nanofabrication Centre for providing the facilities. Publisher Copyright: © 2016 American Chemical Society.
PY - 2016/11/16
Y1 - 2016/11/16
N2 - For the past decade, erbium-doped integrated waveguide amplifiers and lasers have shown excellent potential for on-chip amplification and generation of light at the important telecommunication wavelength regime. However, Er-based integrated devices can only provide small gain per unit length due to the severe energy-transfer between the Er-ions at high concentration levels. Therefore, active ion concentrations have been limited to <1% levels in these devices for optimal performance. Here, we show an efficient and practical way of fabricating Er-doped Al2O3 with Er-concentration as high as ∼3.5% before concentration quenching starts to limit the C-band emission in our material. The Er-doped Al2O3 was fabricated by engineering the distribution of the Er-ions in Al2O3 with the atomic layer deposition (ALD) technique. By choosing a proper precursor for the fabrication of Er2O3, the steric hindrance effect was utilized to increase the distance between the Er-ions in the lateral direction. In the vertical direction, the distance was controlled by introducing subsequent Al2O3 layers between Er2O3 layers. This atomic scale control of the Er-ion distribution allows us to enhance the photoluminescence of our Er:Al2O3 material by up to 16 times stronger when compared to the case where the Er-concentration is ∼0.6%. In addition, long lifetime of approximately 5 ms is preserved in the Er-ions even at such high concentration levels. Thus, our optimized ALD process shows very promising potential for the deposition of optical gain media for integrated photonics structures.
AB - For the past decade, erbium-doped integrated waveguide amplifiers and lasers have shown excellent potential for on-chip amplification and generation of light at the important telecommunication wavelength regime. However, Er-based integrated devices can only provide small gain per unit length due to the severe energy-transfer between the Er-ions at high concentration levels. Therefore, active ion concentrations have been limited to <1% levels in these devices for optimal performance. Here, we show an efficient and practical way of fabricating Er-doped Al2O3 with Er-concentration as high as ∼3.5% before concentration quenching starts to limit the C-band emission in our material. The Er-doped Al2O3 was fabricated by engineering the distribution of the Er-ions in Al2O3 with the atomic layer deposition (ALD) technique. By choosing a proper precursor for the fabrication of Er2O3, the steric hindrance effect was utilized to increase the distance between the Er-ions in the lateral direction. In the vertical direction, the distance was controlled by introducing subsequent Al2O3 layers between Er2O3 layers. This atomic scale control of the Er-ion distribution allows us to enhance the photoluminescence of our Er:Al2O3 material by up to 16 times stronger when compared to the case where the Er-concentration is ∼0.6%. In addition, long lifetime of approximately 5 ms is preserved in the Er-ions even at such high concentration levels. Thus, our optimized ALD process shows very promising potential for the deposition of optical gain media for integrated photonics structures.
KW - atomic layer deposition
KW - erbium
KW - integrated photonics
KW - optical amplifier
KW - photoluminescence
KW - rare-earth ions
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U2 - 10.1021/acsphotonics.6b00283
DO - 10.1021/acsphotonics.6b00283
M3 - Article
SN - 2330-4022
VL - 3
SP - 2040
EP - 2048
JO - ACS Photonics
JF - ACS Photonics
IS - 11
ER -