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arXiv physics/0311010physics.optics
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镓在飞秒laser激发下的相变:相共存和不完全熔化

Gallium transformation under femtosecond laser excitation: Phase coexistence and incomplete melting

O. P. Uteza, E. G. Gamaly, A. V. Rode, M. Samoc, B. Luther-Davies

摘要:

通过测量镓在775 nm处的介电函数,研究了飞秒激光激发下镓的可逆相变。利用菲涅耳公式,从两个不同入射角下测量的镓层的绝对反射率计算了瞬态介电函数的实部和虚部。直接从实验数据中恢复了随时间变化的电子-声子有效碰撞频率、热传导系数和新相的体积分数,并在没有特别假设的情况下重建了随时间和空间变化的相变层中的电子和晶格温度.我们将电子-声子碰撞率的时间依赖关系转化为温度依赖关系,并首次证明了电子-声子碰撞率具有非线性特征。这种温度依赖性在冷却阶段收敛到已知的平衡函数中。即使当沉积能量是熔化平衡焓的两倍时,激光激发镓层中新相的最大分数也仅达到60%。我们还表明,相变的步伐和一小部分的转换材料强烈依赖于激光激发镓层的厚度,这是几十纳米的数量级的整个范围内的泵浦激光能量密度的损伤阈值。激光激发后的相变动力学可以根据一级相变的经典理论来理解,而非热阶段的持续时间似乎与亚皮秒脉冲长度相当。

英文摘要:

The reversible phase transition induced by femtosecond laser excitation of Gallium has been studied by measuring the dielectric function at 775 nm with ~ 200 fs temporal resolution. The real and imaginary parts of the transient dielectric function were calculated from absolute reflectivity of Gallium layer measured at two different angles of incidence, using Fresnel formulas. The time-dependent electron-phonon effective collision frequency, the heat conduction coefficient and the volume fraction of a new phase were restored directly from the experimental data, and the time and space dependent electron and lattice temperatures in the layer undergoing phase transition were reconstructed without ad hoc assumptions. We converted the temporal dependence of the electron-phonon collision rate into the temperature dependence, and demonstrated, for the first time, that the electron-phonon collision rate has a non-linear character. This temperature dependence converges into the known equilibrium function during the cooling stage. The maximum fraction of a new phase in the laser-excited Gallium layer reached only 60% even when the deposited energy was two times the equilibrium enthalpy of melting. We have also demonstrated that the phase transition pace and a fraction of the transformed material depended strongly on the thickness of the laser-excited Gallium layer, which was of the order of several tens of nanometers for the whole range of the pump laser fluencies up to the damage threshold. The kinetics of the phase transformation after the laser excitation can be understood on the basis of the classical theory of the first-order phase transition while the duration of non-thermal stage appears to be comparable to the sub-picosecond pulse length.

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