journal article·2008-07

Raman amplification in nanoparticles doped glasses

A. Céreyon, A.-M. Jurdyc, V. Martinez, E. Burov, A. Pastouret, B. Champagnon

Journal of Non-Crystalline Solids· Volume 354· Issue 29
Publisher page

Abstract

Abstract Resonant Raman effects are studied for CdSxSe1−x nanoparticles in a silicate glass matrix in order to explore new possibilities of Raman amplification for telecommunication fibers. Nanoparticles with diameters ranging from less than 2 nm up to 6 nm are excited with the 458 nm, 488 nm and 633 nm laser lines corresponding both to resonance and off-resonance conditions. Due to confinement effects the resonance conditions are achieved at a given frequency by varying the size of the nanoparticles. In resonance no enhancement is observed for the silicate glass matrix but the (1LO-CdS), (2LO-CdS), (1LO CdSe + 1 LO CdS) modes are strongly enhanced showing the possibility of resonant Raman amplification of the discrete frequencies of the LO modes and of their overtones.
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Research context

OpenAlex topics: Glass properties and applications · Nonlinear Optical Materials Studies · Photonic Crystal and Fiber Optics

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (12)

Show source-provided references
1. Céreyon · Opt. Mater. · 2006 · 28 · 130110.1016/j.optmat.2006.02.016 ↗
2. Manolescu · Glass Tech. · 2005 · 46 · 85
3. Long · 2002
4. Champagnon · J. Appl. Phys. · 1993 · 73 · 277510.1063/1.353053 ↗
5. Champagnon · J. Chem. Phys. · 1991 · 94 · 710.1063/1.460529 ↗
6. Poilblanc · 2006
7. Watson · J. Non-Cryst. Solids · 1983 · 58 · 32310.1016/0022-3093(83)90032-7 ↗
8. Robinet · J. Raman Spectrosc. · 2006 · 37 · 78910.1002/jrs.1540 ↗
9. Shiang · J. Chem Phys. · 1990 · 95 · 323210.1063/1.457874 ↗
10. Rigneault · 2006
11. Klangsin · Phys. Lett. A · 2008 · 372 · 150810.1016/j.physleta.2007.10.008 ↗
12. Saviot · Phys. Rev. B · 2004 · 69 · 11340210.1103/PhysRevB.69.113402 ↗