首页> 外国专利> Laser crystallization or crystal structure alteration of amorphous or polycrystalline semiconductor layers comprises paired laser pulse irradiation for extended melt time while maintaining a low substrate temperature

Laser crystallization or crystal structure alteration of amorphous or polycrystalline semiconductor layers comprises paired laser pulse irradiation for extended melt time while maintaining a low substrate temperature

机译:非晶或多晶半导体层的激光结晶或晶体结构改变包括成对的激光脉冲辐照,以延长熔化时间,同时保持较低的基板温度

摘要

Amorphous semiconductor layer crystallization or polycrystalline semiconductor layer crystal structure alteration is achieved by paired laser pulse irradiation to provide an extended melt time while maintaining a low substrate temperature. Crystallization of amorphous semiconductor layers or alteration of the crystal structure of polycrystalline semiconductor layers is carried out by irradiation with laser pulses (LP1, LP2) from two pulsed laser beam sources. The laser pulse pair has the following properties: (a) the pulses overlap or pulse LP2 follows pulse LP1 by a short spacing (shorter than the melting time of the target material); (b) pulse LP1 (preferably with a typical width of 10-50 nsec.) causes brief total or partial melting of the irradiated area, while pulse LP2 is homogeneous and is absorbed in the target surface region melted by LP1 to prolong the melting time; (c) pulse LP1 has a wavelength such that it reaches a depth less than or equal to the layer thickness, while pulse LP2 has a wavelength of LP2 such that it reaches a depth in the micron range in the solid material but only a few (up to 30) nm in the liquid material so that the liquid material selectively absorbs the radiation; (d) the intensity, pulse width and pulse spacing have such values that, at similar fluences (F = intensity x pulse width, i.e. I * tau ) of LP1 and LP2, the intensity of LP2 is large enough to avoid re-solidification of the melt after the end of LP1, with the proviso that tau 1 is less than tau 2, I1 is greater than I2 and the ablation threshold for LP2 restricts its fluence.
机译:非晶半导体层结晶或多晶半导体层晶体结构的改变是通过成对的激光脉冲辐照实现的,以提供延长的熔化时间,同时保持较低的基板温度。通过用来自两个脉冲激光束源的激光脉冲(LP1,LP2)照射来进行非晶半导体层的结晶或多晶半导体层的晶体结构的改变。激光脉冲对具有以下特性:(a)脉冲重叠或脉冲LP2跟随脉冲LP1间隔很短(比目标材料的熔化时间短); (b)脉冲LP1(通常具有10-50纳秒的典型宽度)会引起照射区域的短暂完全熔化或部分熔化,而脉冲LP2是均匀的并被LP1熔化的目标表面区域吸收以延长熔化时间; (c)脉冲LP1的波长使其达到的深度小于或等于层厚度,而脉冲LP2的波长为LP2使得其达到固体材料中微米范围内的深度,但仅有几个(液体材料中的最大30)nm,以便液体材料选择性地吸收辐射; (d)强度,脉冲宽度和脉冲间隔具有这样的值:在LP1和LP2的通量(F =强度x脉冲宽度,即I * tau)下,LP2的强度足够大,可以避免重新凝固LP1结束后的熔体温度,tau 1小于tau 2,I1大于I2,并且LP2的烧蚀阈值限制了其通量。

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