It appears you don't have support to open PDFs in this web browser. To view this file, Open with your PDF reader
Abstract
The reflection of light from moving boundaries is of interest both fundamentally and for applications in frequency conversion, but typically requires high pump power. By using a dispersion-engineered silicon photonic crystal waveguide, we are able to achieve a propagating free carrier front with only a moderate on-chip peak power of 6 W in a 6 ps-long pump pulse. We employ an intraband indirect photonic transition of a co-propagating probe, whereby the probe practically escapes from the front in the forward direction. This forward reflection has up to 35% efficiency and it is accompanied by a strong frequency upshift, which significantly exceeds that expected from the refractive index change and which is a function of group velocity, waveguide dispersion and pump power. Pump, probe and shifted probe all are around 1.5 µm wavelength which opens new possibilities for “on-chip” frequency manipulation and all-optical switching in optical telecommunications.
You have requested "on-the-fly" machine translation of selected content from our databases. This functionality is provided solely for your convenience and is in no way intended to replace human translation. Show full disclaimer
Neither ProQuest nor its licensors make any representations or warranties with respect to the translations. The translations are automatically generated "AS IS" and "AS AVAILABLE" and are not retained in our systems. PROQUEST AND ITS LICENSORS SPECIFICALLY DISCLAIM ANY AND ALL EXPRESS OR IMPLIED WARRANTIES, INCLUDING WITHOUT LIMITATION, ANY WARRANTIES FOR AVAILABILITY, ACCURACY, TIMELINESS, COMPLETENESS, NON-INFRINGMENT, MERCHANTABILITY OR FITNESS FOR A PARTICULAR PURPOSE. Your use of the translations is subject to all use restrictions contained in your Electronic Products License Agreement and by using the translation functionality you agree to forgo any and all claims against ProQuest or its licensors for your use of the translation functionality and any output derived there from. Hide full disclaimer
Details




1 Institute of Optical and Electronic Materials, Hamburg University of Technology, Hamburg, Germany; Department of Physics, Faculty of Science, Menoufia University, Menoufia, Egypt
2 Institute of Optical and Electronic Materials, Hamburg University of Technology, Hamburg, Germany
3 SUPA, School of Physics and Astronomy, University of St. Andrews, St. Andrews, Fife, UK; Tyndall National Institute, Cork, Ireland; Centre for Advanced Photonics and Process Analysis, Cork Institute of Technology, Cork, Ireland
4 State Key Laboratory of Optoelectronic Materials & Technology, Sun Yat-sen University, Guangzhou, China
5 Department of Physics, University of York, York, UK
6 Institute of Optical and Electronic Materials, Hamburg University of Technology, Hamburg, Germany; ITMO University, St. Petersburg, Russia
7 Institute of Optical and Electronic Materials, Hamburg University of Technology, Hamburg, Germany; Institute of Materials Research, Helmholtz-Zentrum Geesthacht, Geesthacht, Germany