X-ray microanalysis of optical materials for 157nm photolithography

G. Dražič , E. Sarantopoulou , S. Kobe , Z. Kollia , A.C. Cefalas
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引用次数: 5

Abstract

Next generation microelectronic circuits will have minimum dimensions below 100 nm. It is envisioned that 157 nm laser lithography will be the next step of optical lithography, A.C. Cefalas, E. Sarantopoulou, Microelectronic Engineering, V53, (2000) 465, followed by lithographies at shorter wavelengths e.g. 13 nm. At 157 nn vacuum ultraviolet (VUV) illumination of the mask target lithographic features with dimensions less than 100 nm on the photoresist could be achieved. However, there are problems related with the design of the optical projection system. This is mainly because most of the optical materials in one hand have high absorption coefficient and their optical properties degrade constantly with time under VUV irradiation. Taking into consideration the imaging requirements for this type of application, the refractive index variation over the illuminated volume of the optical material should be better than 10-6, and hence optical elements should be prepared from ultra high purity materials. Crystals have been examined with the Jeol 2010 F microscope equipped by the energy dispersive X-ray spectroscopy (EDXS), and it has been proved to be an efficient quality control technique for identifying defects and impurities in crystal samples. A non-uniform distribution of concentration of various elements in wide band gap dielectric crystals in confined space regions from 2 to 50 nm was found, and this result sets the limitations in the optical quality of the crystals.

157nm光刻光学材料的x射线微分析
下一代微电子电路的最小尺寸将低于100纳米。展望157nm激光光刻技术将是光学光刻技术的下一个发展阶段,A.C. Cefalas, E. Sarantopoulou,微电子工程,V53,(2000) 465,随后是更短波长的光刻技术,如13nm。在157 nn的真空紫外(VUV)照射下,可以在光刻胶上实现尺寸小于100 nm的掩模目标光刻特征。然而,光学投影系统的设计存在一些问题。这主要是因为大部分光学材料一方面具有较高的吸收系数,在紫外辐射下光学性能随时间不断退化。考虑到此类应用的成像要求,光学材料在照射体积上的折射率变化应优于10-6,因此光学元件应由超高纯度材料制备。用配备能量色散x射线能谱(EDXS)的Jeol 2010 F显微镜对晶体进行了检测,证明了它是一种有效的质量控制技术,可以识别晶体样品中的缺陷和杂质。宽禁带介电晶体中各种元素的浓度在2 ~ 50 nm的密闭空间内不均匀分布,这一结果限制了晶体的光学质量。
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