The effect of external magnetic field on the linear stage evolution of Kelvin–Helmholtz instability in laser driven plasma
Introduction
A Kelvin–Helmholtz instability (KHI) occurs when two parallel fluids of different velocities and densities flow alongside each other, with a shear exceeding a critical value [1]. In a collisionless plasma, wave–particle interactions play essential roles in transport and dissipation [2], governing the intermixing of fluids in both natural and engineering systems. Although not expected to appear, KHIs are widespread in inertial confinement fusion [3]. The KHI is also essential to many astrophysical and space phenomena such as the dynamic structure of cometary tails [4], relativistic outflows and oscillations in astrophysical jets [5], [6], mergers between neutron stars or energy and momentum transfer between the solar wind and the magnetosphere of the Earth [7]. Recent observations have found that the KHI plays a very essential role in plasma heating as it develops on small scales, thereby enhancing dissipation such as turbulent viscosity at the boundaries of larger-scale coronal mass ejections and solar jets [1], [8], [9], [10], [11]. Wan et al. [12] first observed a KHI evolving from well-controlled dual-mode seed perturbations. Kinetic simulations show that an electron vortex can generate secondary magnetic reconnection, a formation of secondary magnetic islands and flux ropes. This is a nonlinear effect of electron KHI driven by electron shear flows produced during magnetic reconnection, which leads to strong electron energization in the outflow region. However, this has not been verified experimentally. Simulation and observation have also found that a KHI can generate secondary magnetic reconnection [13], [14], [15], [16].
Laboratory studies are an important platform for observing such macroscopic phenomena in astrophysical plasma. A key assumption of all laser-driven high-energy-density (HED) experiments is that the dynamics of the system is repeatable across experiments as long as the defining metrics of the platform remain constant. Repeatability allows users to map the entire evolution of a system. Wan et al. [17] used the OMEGA EP laser facility to observe single-mode KHI behavior in the supersonic regime. Our experiment also establishes a platform that can be iterated to explore compressible HED shear flows in more detail. In addition, Harding et al. used radiographic diagnosis to induce a new and highly pronounced HED KHI [18]. In recent years, there have been many studies on linear and weakly nonlinear behavior of incompressible KHIs. A slight disturbance at the fluid interface grows linearly and weakly nonlinearly, and it develops from a strong nonlinear effect on a turbulent mixture [19], [20], [21]. However, no past study has used an external magnetic field when observing KHI behavior in the supersonic regime.
In this work, we study the linear evolution of a KHI in the laboratory. We use laser-induced plasma to drive KHI formation and observe the effect of an external magnetic field on KHI development and evolution.
Section snippets
Experimental setup
The experiment was conducted on the Shenguang II (SGII) laser facility at the National Laboratory on High Power Lasers and Physics. Four SG II laser beams, with a wavelength of 0.351 µm, are bunched to deliver a total energy of 1 kJ in a nanosecond square pulse. The four beams are simultaneously focused on a CH foil. The focused spot is 100–150 µm in diameter at full width at half maximum, giving an incident laser intensity of around 1015 W/cm2. The target configuration, as shown in Fig. 1,
Results and discussion
Fig. 2 shows the shadowgraphs taken at delay times of 4, 5 and 6 ns. The delay is defined as the time between the falling probe edges and the main pulses. Because the probe light propagates horizontally from left to right, the optical image is a lateral projection, so only the side of the CH foil can be seen in the figure. The center of the laser beam is at (y, z) = (0, 1.0) in Figs. 2 and 3. The dark black area in the optical image is unlit because the probe light is absorbed or scattered
Conclusion
We have presented the experimental results of a KHI produced by intense laser-driven thin plastic foils. The proposed experiment allows direct measurement of linear KHI evolution and validation of numerical simulation. Optical diagnosis has confirmed the linear stage of KHI evolution. The KHI has different evolutionary features when an external magnetic field is applied in different directions. Theory shows that the external magnetic field has a stronger effect on KHI growth when it is
Acknowledgments
We are very grateful to the Shenguang II and target preparation staff for valuable help and support. This work was supported by the Science Challenge Project (grant no. TZ2016005), the National Natural Science Foundation of China (grant nos. 10905004, 11220101002 and 11622323), and the Fundamental Research Funds for the Central Universities.
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