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PIC simulation of collective Thomson scattering in a non-equilibrium plasma

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目录

Chapter1:background and purpose

1.1 Background

1.2 High power laser experiment of collisionless shock

1.3 Thomson scattering measurement[1]

1.4 Collective and non-collective Thomson scatterings

1.5 Plasma waves and collective Thomson scattering[2]

1.6 Collective Thomson scattering in non-equilibrium plasma

Chapter2:One dimensional Particle in cell (PIC) simulation

2.1 Basic equations in PIC simulation

2.2 Flow chart of PIC simulation

2.3 Simulation settings

2.3 Simulation parameters

3. Result of PIC simulation:Beam instability

3.1 Time evolution of energy and electron phase space

3.2 Wave characteristics

Chapter4:Result of PIC simulation:Virtual Thomson scattering

4.1 Run 3:Without beam

4.2 Run4:with beam

4.3 Dependence on intensity of probe light, EI

4.4 Dependence on beam velocity, ub

Chapter5. Summary and future issues

5.1 Summary

5.2 Future issues

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摘要

Recently,a variety of high energy astrophysical phenomena have been successfully reproduced in laboratory experiments using high power laser facilities. We take part in the experiment of collisionless shocks in collaboration with a group at the Institute of Laser Engineering at Osaka University. The transition region of the collisionless shock is usually in a highly non-equilibrium state. In order to understand the mechanism of energy dissipation at the collisionless shocks,we need to clarify the relaxation processes occurring there. To diagnose such a local plasma,the Thomson scattering (TS) measurement has been widely used. Here,the TS is defined as an elastic scattering of a low frequency incident electromagnetic wave due to its interaction with free electrons in a plasma. Although the TS measurement has been used for a long time to measure the plasma not only in experimental devices but also in space (ionosphere),detailed theory of the TS in a non-equilibrium plasma has not been well established.
  In this thesis we investigate how a non-equilibrium plasma near the shock transition region is observed by the TS measurement. First,we assume that a plasma just upstream of a shock consists of background electrons,ions,and beam electrons. The beam instability generated in such an unstable local plasma is reproduced by using one-dimensional full particle-in-cell (PIC) simulation. Then,a monochromatic electromagnetic wave,as a proxy of the probe light of the TS measurement,is incident upon the system to reproduce virtual collective TS. It is shown that the so-called electron feature of collective TS is strongly enhanced in the beam-plasma system. The characteristics of the enhanced electron feature is discussed in detail.

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