Lorusso Antonella, Égerházi László, Szatmári Sándor, Szörényi Tamás
Department of Mathematics and Physics "E. De Giorgi", University of Salento, 73100 Lecce, Italy.
Department of Medical Physics and Informatics, Albert Szent-Györgyi Medical School, University of Szeged, H-6720 Szeged, Hungary.
Materials (Basel). 2024 Jun 3;17(11):2712. doi: 10.3390/ma17112712.
The availability of new-generation femtosecond lasers capable of delivering pulses with energies in the hundreds of mJ, or even in the joules range, has called for a revision of the effect of scaling spot size on the material distribution within the plasma plume. Employing a state-of-the-art Szatmári-type hybrid dye-excimer laser system emitting 248 nm pulses with a maximum energy of 20 mJ and duration of 600 fs, copper films were grown in the classical pulsed laser deposition geometry. The exceptionally clean temporal profile of the laser pulses yielded a femtosecond component of 4.18 ± 0.19 mJ, accompanied by a 0.22 ± 0.01 mJ ASE pedestal on the target surface. While varying the spot sizes, the plasma plume consistently exhibited an extremely forward-peaked distribution. Deposition rates, defined as peak thickness per number of pulses, ranged from 0.030 to 0.114 nm/pulse, with a gradual narrowing of the thickness distribution as the spot area increased from 0.085 to 1.01 mm while keeping the pulse energy constant. The material distribution on the silicon substrates was characterized using the (Θ) = cosΘ + (1 - )cosΘ formalism, revealing exponents characterizing the forward-peaked component of the thickness profile of the film material along the axes, ranging from = 15 up to exceptionally high values exceeding 50, as the spot area increased. Consequently, spot size control and outstanding beam quality ensured that majority of the ablated material was confined to the central region of the plume, indicating the potential of PLD (pulsed laser deposition) for highly efficient localized deposition of exotic materials.
新一代飞秒激光器能够产生能量在数百毫焦甚至焦耳范围内的脉冲,这就要求重新审视光斑尺寸缩放对等离子体羽流内材料分布的影响。使用最先进的萨特马里型混合染料 - 准分子激光系统,该系统发射波长为248nm、最大能量为20mJ且持续时间为600fs的脉冲,在经典的脉冲激光沉积几何结构中生长铜膜。激光脉冲异常纯净的时间轮廓产生了4.18±0.19mJ的飞秒成分,同时在靶表面伴随着0.22±0.01mJ的自发辐射放大(ASE)基座。在改变光斑尺寸时,等离子体羽流始终呈现出极其向前尖峰的分布。沉积速率定义为每脉冲数的峰值厚度,范围从0.030到0.114nm/脉冲,当光斑面积从0.085增加到1.01mm²同时保持脉冲能量恒定时,厚度分布逐渐变窄。使用(Θ) = cosΘ + (1 - )cosΘ形式来表征硅衬底上的材料分布,结果表明,随着光斑面积增加,表征薄膜材料厚度轮廓沿轴向前尖峰成分的指数范围从 = 15到超过50的极高值。因此,光斑尺寸控制和出色的光束质量确保了大部分烧蚀材料局限于羽流的中心区域,这表明脉冲激光沉积(PLD)在高效局部沉积奇异材料方面具有潜力。