PIC simulations of the competition between backward and forward stimulated Raman side scatter in ignition-scale direct-drive coronal conditions

Author:

Wang Q.1ORCID,Xiao C. Z.23ORCID,Xie Y.4ORCID,Cai H. B.1ORCID,Chen J.1ORCID,Liu Z. J.1ORCID,Cao L. H.1ORCID,Zheng C. Y.1ORCID,Liu C. S.5,Rozmus W.6ORCID,Myatt J. F.7ORCID,He X. T.1ORCID

Affiliation:

1. Institute of Applied Physics and Computational Mathematics 1 , Beijing 100094, China

2. School of Physics and Electronics, Hunan University 2 , Changsha 410082, China

3. Collaborative Innovation Center of IFSA (CICIFSA), Shanghai Jiao Tong University 3 , Shanghai 200240, China

4. Laser Fusion Research Center, China Academy of Engineering Physics 4 , Mianyang, Sichuan 621900, China

5. Physics Department, University of Maryland 5 , College Park, Maryland 20742, USA

6. Department of Physics, University of Alberta 6 , Edmonton, Alberta T6G 2E1, Canada

7. Department of Electrical and Computer Engineering, 9211 116 St. NW, University of Alberta 7 , Edmonton Alberta T6G 1H9, Canada

Abstract

The competition between forward stimulated Raman side scatter (FSRSS) and backward stimulated Raman side scatter (BSRSS) is investigated in inhomogeneous plasma using particle-in-cell (PIC) simulations. Experimental observations at the National Ignition Facility have demonstrated the significance of stimulated Raman side scatter or backscatter instability compared to two-plasmon-decay under ignition-scale conditions for various laser beam geometries. Side scatter refers to the geometry where the Raman scattered light is generated in a direction perpendicular to the local density gradient. For an obliquely incident pump, the scattered light can either copropagate (FSRSS) or counter propagate (BSRSS) with respect to the pump. Under ignition-scale conditions, linear analysis shows that both BSRSS and FSRSS are absolutely unstable (temporally growing) at higher densities (ne∼0.2 nc), whereas at lower densities (ne∼0.1 nc), BSRSS becomes convective with substantial gain, while FSRSS remains absolute. Two-dimensional PIC simulations demonstrate that the competition between BSRSS and FSRSS is sensitive to the density. BSRSS tends to dominate at higher densities, while FSRSS becomes dominant at lower densities. At moderate densities (ne∼0.15 nc), FSRSS and BSRSS coexist. Furthermore, an increase in laser intensity leads to enhanced electron trapping, which kinetically strengths and then saturates BSRSS in the lower density region.

Funder

Natural Sciences and Engineering Research Council of Canada

National Natural Science Foundation of China

China Postdoctoral Science Foundation

Publisher

AIP Publishing

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