Haines M G, Wei M S, Beg F N, Stephens R B
Physics Department, Imperial College, London, SW7 2AZ, UK.
Phys Rev Lett. 2009 Jan 30;102(4):045008. doi: 10.1103/PhysRevLett.102.045008.
Experimental data [F. N. Beg, Phys. Plasmas 4, 447 (1997)10.1063/1.872103] indicate that for intense short-pulse laser-solid interactions at intensities up to 5 x 10(18) W cm(-2) the hot-electron temperature proportional, variant(Ilambda(2)) (1/3). A fully relativistic analytic model based on energy and momentum conservation laws for the laser interaction with an overdense plasma is presented here. A general formula for the hot-electron temperature is found that closely agrees with the experimental scaling over the relevant intensity range. This scaling is much lower than ponderomotive scaling. Examination of the electron forward displacement compared to the collisionless skin depth shows that electrons experience only a fraction of a laser-light period before being accelerated forward beyond the laser light's penetration region. Inclusion of backscattered light in a modified model indicates that light absorption approaches 80%-90% for intensity >10(19) W cm(-2).
实验数据[F. N. 贝格,《物理等离子体》4, 447 (1997)10.1063/1.872103]表明,对于强度高达5×10¹⁸ W/cm²的强短脉冲激光与固体相互作用,热电子温度与(Ilambda²)的三分之一成正比。本文提出了一个基于能量和动量守恒定律的全相对论解析模型,用于描述激光与过密等离子体的相互作用。得到了一个热电子温度的通用公式,该公式在相关强度范围内与实验标度关系非常吻合。这种标度关系远低于有质动力标度。与无碰撞趋肤深度相比,对电子向前位移的研究表明,电子在被加速向前超过激光穿透区域之前,仅经历了激光周期的一小部分。在一个改进模型中考虑反向散射光表明,对于强度>10¹⁹ W/cm²,光吸收接近80% - 90%。