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DOE OSTI · 3003665

Plasma gradient effect on direct laser acceleration

Tang, H. [Univ. of Michigan, Ann Arbor, MI (United States)] (ORCID:0000000348856863)·Babjak, R. [Czech Academy of Sciences (CAS), Prague (Czech Republic)] (ORCID:0000000221744987)·Yeh, I.-L. [Univ. of California, San Diego, CA (United States)] (ORCID:000000030796717X)·Contreras, V. [Univ. of Michigan, Ann Arbor, MI (United States)] (ORCID:0000000206879496)·Tangtartharakul, K. [Univ. of California, San Diego, CA (United States)] (ORCID:000000017992924X)·Albert, F. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000246128240)·Chen, H. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000201811695)·Shaw, J. L. [Univ. of Rochester, NY (United States)] (ORCID:0000000211188921)·Vranic, M. [Univ. of Lisbon (Portugal)] (ORCID:0000000337640645)·Arefiev, A. V. [Univ. of California, San Diego, CA (United States)] (ORCID:0000000205970976)·Willingale, L. [Univ. of Michigan, Ann Arbor, MI (United States)] (ORCID:0000000343040339)
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Abstract

The transfer of a high-intensity laser pulse energy to a high-energy electron beam via the direct laser acceleration mechanism is shown to be significantly enhanced through control of the plasma density gradient. Experiments performed using the OMEGA EP facility's high-intensity beams altered the plasma density and gradients by changing the Mach number and the angle of the gas-jet nozzle to the laser axis. When a long density gradient at the rear of the target is used, the total high-energy electron number measured was enhanced by 4.5 times compared to a shorter rear gradient. Complementary two-dimensional simulations, which follow the laser field evolution and the corresponding electron dynamics, strongly support the key trends observed in the experiment. The effect is twofold, the long density gradient provides the longest acceleration distance while it minimizes the formation of the sheath field as the electron beam exits into the vacuum. This study shows the importance of tailoring the plasma density.

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Tang, H. [Univ. of Michigan, Ann Arbor, MI (United States)] (ORCID:0000000348856863), Babjak, R. [Czech Academy of Sciences (CAS), Prague (Czech Republic)] (ORCID:0000000221744987), Yeh, I.-L. [Univ. of California, San Diego, CA (United States)] (ORCID:000000030796717X), Contreras, V. [Univ. of Michigan, Ann Arbor, MI (United States)] (ORCID:0000000206879496), Tangtartharakul, K. [Univ. of California, San Diego, CA (United States)] (ORCID:000000017992924X), Albert, F. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000246128240), Chen, H. [Lawrence Livermore National Laboratory (LLNL), Livermore, CA (United States)] (ORCID:0000000201811695), Shaw, J. L. [Univ. of Rochester, NY (United States)] (ORCID:0000000211188921), Vranic, M. [Univ. of Lisbon (Portugal)] (ORCID:0000000337640645), Arefiev, A. V. [Univ. of California, San Diego, CA (United States)] (ORCID:0000000205970976), Willingale, L. [Univ. of Michigan, Ann Arbor, MI (United States)] (ORCID:0000000343040339). 2025-10-29. Plasma gradient effect on direct laser acceleration. https://doi.org/10.1063/5.0252460

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