Measurement of stimulated Raman side-scattering predominance in directly driven experiment

Author:

Glize K.12ORCID,Zhao X.12ORCID,Zhang Y. H.23ORCID,Lian C. W.4,Tan S.5ORCID,Wu F. Y.12ORCID,Xiao C. Z.5ORCID,Yan R.6ORCID,Zhang Z.237ORCID,Yuan X. H.12ORCID,Zhang J.123ORCID

Affiliation:

1. Key Laboratory for Laser Plasmas (MoE) and School of Physics and Astronomy, Shanghai Jiao Tong University 1 , Shanghai 200240, China

2. Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University 2 , Shanghai 200240, China

3. Beijing National Laboratory for Condensed Matter Physics, Institute of Physics, Chinese Academy of Sciences 3 , Beijing 100190, China

4. Department of Plasma Physics and Fusion Engineering and CAS Key Laboratory of Geospace Environment, University of Science and Technology of China 4 , Hefei, Anhui 230026, China

5. Key Laboratory for Micro-/Nano-Optoelectronic Devices of Ministry of Education, School of Physics and Electronics, Hunan University 5 , Changsha 410082, China

6. Department of Modern Mechanics, University of Science and Technology of China 6 , Hefei, Anhui 230026, China

7. Songshan Lake Materials Laboratory 7 , Dongguan, Guangdong 523808, China

Abstract

Due to its particular geometry, stimulated Raman side-scattering (SRSS) drives scattered light emission in non-usually diagnosed directions, leading to scarce and complex experimental observations. Direct-irradiation campaigns at the SG-II Upgrade facility have measured the scattered light driven by SRSS over a wide range of angles. Typical interaction conditions were as follows: an overlapped laser intensity of 1.2×1015 W cm−2 propagated into a plasma with a density scale length Lnc/4≈250 μm and an electron temperature Te≈2.2 keV. It indicated an emission at large polar angles over a broad azimuthal range, sensitive to the plasma profile, resulting in a loss of about 5% of the total laser energy. Direct comparison with back-scattering measurement, both in the full-aperture back-scattered direction and sampled at smaller polar angles in the same azimuthal plane, has evidenced SRSS as the dominant Raman scattering process. The predominance of SRSS was confirmed by two-dimensional particle-in-cell simulations, and its angular spread has been corroborated by ray-tracing simulations. The main implication is that a complete characterization of the SRS instability and an accurate measurement of the energy losses require the collection of the scattered light in a broad range of directions. Otherwise, spatially limited measurement could lead to an underestimation of the energetic importance of stimulated Raman scattering.

Funder

Strategic Priority Research Program of Chinese Academy of Sciences

Publisher

AIP Publishing

Subject

Condensed Matter Physics

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