两束同色激光场和中红外场驱动氦原子在等离激元中产生的单个阿秒脉冲

Single isolated attosecond pulse generated by helium atom exposed to the two laser pulses with the same color and midinfrared intense laser pulse in the plasmon

通过数值求解一维氦原子由两束同色激光场和中红外形成组合场中的含时薛定谔方程,研究了氦原子在纳米等离激元中发射高次谐波的性质以及合成阿秒脉冲的特点.研究表明,在等离激元中氦原子在组合场驱动下发射的高次谐波相对于均匀场情况下截止位置会得到明显扩展,但等离激元对处在连续态电子的吸收效应会对高次谐波截止位置影响较大,通过改变激元的相对位置能明显提高其中一个轨道对谐波的贡献,抑制另一些电子轨道的贡献.经典分析表明,两个电子轨道发生并合,从而实现单个阿秒脉冲的输出.与原子在均匀场驱动的情况相比,阿秒脉冲的宽度明显缩短,最短可实现28 as的单个脉冲输出.

We have investigated the characteristics of high harmonic and attosecond pulse generated by helium atom exposed to the combined field of two laser pulses with the same color and a midinfrared laser pulse in nano-structure plasmon by solving the one-dimensional time-dependent SchrSdinger equation. It is shown that the cut-off position of the harmonics is obviously extended in the combined field, however, the plasmon structure determined effe0t of absorbing the electron in the continuum states has an important influence on the cut-off position of the harmonics. It is found that the contribution from some single trajectory of electron is enhanced and other trajectories are suppressed by changing the plasmon position, so a single isolated attosecond pulse is obtained. Comparison with the scenario of atoms driven in homogeneous field, the width of the pulse decreases greatly, and an isolated pulse is achieved to be as short as 28 attoseconds.