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EXTREME ULTRAVIOLET LIGHT SOURCE AND TARGET FOR EXTREME ULTRAVIOLET LIGHT SOURCE TARGET

机译:极紫外光源和靶标极紫外光源的靶标

摘要

An object of the present invention is to provide an extreme ultraviolet light source target which can emits extreme ultraviolet light with high emission efficiency. A solid target made of heavy metal or heavy-metal compound and having a density 0.5 to 80% that of the crystal density is used. When the target is irradiated with a laser beam, plasma of the heavy metal contained in the target is generated, and extreme ultraviolet light having a predetermined wavelength which corresponds to the kind of the heavy metal is emitted from the plasma. When the density of the target is made to be smaller than the crystal density as described above, space distribution of the density of the generated plasma can be controlled, and the region in which plasma absorbs energy of the laser beam overlaps the region in which the plasma emits the extreme ultraviolet light. Thus, emission efficiency can be improved, preventing energy loss. For example, in a case where the SnO2 target having a density 24% of the crystal density is used, the emission efficiency at around 13.5 nm wavelength is higher than in the case where a Sn crystal target is used.
机译:本发明的目的是提供可以以高发射效率发射极紫外光的极紫外光源靶。使用由重金属或重金属化合物制成的固体靶,其密度为晶体密度的0.5%至80%。当用激光束照射靶时,产生包含在靶中的重金属的等离子体,并且从等离子体发射具有与重金属的种类相对应的预定波长的极紫外光。当如上所述使靶的密度小于晶体密度时,可以控制所产生的等离子体的密度的空间分布,并且等离子体吸收激光束的能量的区域与该等离子体的区域重叠。等离子体发出极紫外光。因此,可以提高发射效率,防止能量损失。例如,在使用密度为晶体密度的24%的SnO 2靶的情况下,与使用Sn晶体靶的情况相比,在约13.5nm波长处的发射效率更高。

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