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  5. Characterization of diced ridge waveguides in pure and Er-doped lithium-niobate-on-insulator (LNOI) substrates
 
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Characterization of diced ridge waveguides in pure and Er-doped lithium-niobate-on-insulator (LNOI) substrates

Publication date
2014
Document type
Conference paper
Author
Rüter, C. E.
Suntsov, S.
Kip, Detlef 
Stone, G.
Dierolf, V.
Hu, H.
Sohler, W.
Editor
Digonnet, Michel J. F.
Jiang, Shibin
Organisational unit
Experimentalphysik und Materialwissenschaften 
DOI
10.1117/12.2036270
URI
https://openhsu.ub.hsu-hh.de/handle/10.24405/14130
Scopus ID
2-s2.0-84901049822
Conference
SPIE OPTO 2014
Publisher
SPIE
Series or journal
Proceedings of SPIE - The International Society for Optical Engineering
ISSN
0277-786X
1996-756X
ISBN
9780819498953
Part of the university bibliography
✅
  • Additional Information
Language
English
Abstract
Lithium-niobate-on-insulator (LNOI) is a new material platform for integrated optics allowing for small bending radii, high intensities and superior electro-optical and nonlinear properties. Ridge waveguides of different width are fabricated on pure and Er-doped LNOI substrates using diamond-blade dicing, resulting in smooth side walls with lower roughness when compared to dry etching techniques. Propagation losses for polarized modes are measured by the Fabry-Perot method using a fiber coupling setup and a tunable laser at 1.5 μm. Loss values as low as ∼1.4dBcm-1 were obtained for quasi-TM (qTM) modes, while losses for qTE modes are slightly higher. Characterization of Er:LNOI ridges is performed using Raman and fluorescence spectroscopy. Spectral scans are obtained using a scanning confocal microscope and a 488nm laser. Besides line broadening that may be attributed to internal strain in the bonded layer and implantation induced defects, analysis of Raman spectra shows no significant difference between waveguide and bulk material. However, Er emission of 2H11/2 and 4S 3/2 to 4I15/2 contains small spatial differences across the layer thickness when compared to Er-doped bulk samples. While Raman intensity has a linear relationship with pump power, the intensity of the Er emission starts saturating already at pump levels of a few mW. To investigate fluorescence of the 4I13/2-4I 15/2 transition inside the diced ridges, a fiber-coupled laser with wavelength 980nm is used for pumping. The emission is broadened and maxima are shifted to longer wavelengths, which may be attributed to defects induced by implantation, strain induced by the bonded LN-SiO2 interface, and re-absorption of fluorescence light.
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