论文标题

激光脉冲的纵向辐射力和移动颗粒的光学元件

Longitudinal Radiation Force of Laser Pulses and Optics of Moving Particles

论文作者

Kovachev, Lubomir

论文摘要

长期以来,横向和纵向光学作用用于对小颗粒的非接触和无创操纵。出现以下问题:这些力对连续介质中千粒子集合的影响是什么?这项工作的目的是找到辐射力的分析表达和介质介质中激光脉冲产生的潜在密度的分析表达。这使我们能够在激光脉冲斑点的水平上找到有效的平均纵向真力。获得的力与初始脉冲能量成正比,并且与其持续时间成反比。在飞秒区域中,力变得足够强大,可以将中性颗粒限制在脉冲包膜中,并以组速度转换它们。例如,在二氧化硅中,飞秒脉冲的纵向力显着大于分子力。因此,用短脉冲的二氧化硅中的细融化可能是由于这种纵向力破坏了分子键。另外,将脉冲包膜限制在脉冲包膜中后,移动粒子会产生新的线性和非线性效应。偶极子与捕获到脉冲中捕获的颗粒的电磁场的相互作用是在载体之间产生的,而不是在携带的频率下。这种振荡在气体和固体中的THZ中的次数为sub-thz范围。在非线性方向而不是第三谐波中,移动粒子的合奏以比例成正比的频率产生,是信封载体频率的三倍。

For a long time transverse and longitudinal optical forces are used for non-contact and noninvasive manipulation of small individual particles. The following question arises: What is the impact of these forces on the ensemble of thousand particles in continuous media? The aim of this work is to find analytical expression of the radiation force and potential densities creating from laser pulse propagating in dielectric media. This allows us to find an effective averaged longitudinal real force at the level of the laser pulse spot. The obtained force is proportional to initial pulse energy and inversely proportional to its time duration. In the femtosecond region the force becomes strong enough to confine the neutral particles into the pulse envelope and translate them with group velocity. In silica for example, the longitudinal force of a femtosecond pulse is significantly greater than the molecular forces. Thus, the fine ablation in silica with short pulses may be due to this longitudinal force, which breaks down the molecular bonds. Additionally, after confinement into the pulse envelope, the moving particles produce new linear and nonlinear effects. The dipole interaction with the electromagnetic field of the particles captured into the pulse generate at carrier-to-envelope frequency, instead of at the carrying ones. This oscillation is in sub-THz range in gases and in THz in solids. In nonlinear regime instead of third harmonics, the ensemble of moving particles generates at frequency proportional to three times the frequency of the envelope-carrier.

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