Fabrication Of Nanometer Scale Structure Using Thin Film Stress

Dong-il Park, S. Hahm, Jong-Hyun Lee, Jung-Hee Lee
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Abstract

I . I n t r o d u c t i o n For many applications u l t r a f i n e s t ructures have been fabricated by opt ical lithography, dry etching, AFM machining tool and electron beam lithography. However these methods need high cos t and complicated process for la rge scale process. I n t h e past we have reported on nanometer scale formation with 20 nm gap based on polysilicon layer"'. Now we w i l l present a simple nanometer scale formation technique with s i l i c o n layer and w i l l e lucidate the formation mechanism. 11. Experiment A schematic diagram of the key fabrication process f o r wedge type nanostructure is presented i n Figure l ( a ) . A Si3N4 layer of 1600 A was deposited by LPCM a t 700 -C on SIMOX wafer with 4000 A-thick-SiOz. After photolithography pat terning of the electrodes, which were i n i t i a l l y merged, the Si& and Si layers were etched by dry etching The bottom Si02 layer was p a r t i a l l y etched under control, and the samples were annealed i n N2 ambient with the various temperature and t h e time. Figure l (b) shows the schematic view of fabr icated wedge type s t ruc ture with gap. The gap was formed a t the minimum cross sect ion area of the patterned wedge by stress which had been generated during annealing and cooling. Figure 2 shows the qua l i ta t ive dis t r ibut ion of the s t r e s s i n each layer formed during the annealing process"'. The compressive stress formed i n each layers f i n a l l y a c t a s a tens i le stress a t the minimum cross sect ion area of s t ructure . If the t e n s i l e thermal stress was large, the merged area was s p l i t t e d i n t o two par t and formed a gap between them, Figure 3 shows the gap spacing with annealing time evolution a t 1100 "C a f t e r l a t e r a l l y 2 pm and 11 pm Si02 etching. The gap was saturated about 250 nm and a b u t 190 nm f o r 2 ,um and 11 pm Si02 etching respectively. The gap width of 30 samples measured was within *lox of average saturation value. I t was thought tha t the difference of the gaps between the two l a t e r a l Si02 etching conditions was caused by the f a c t tha t the Si02 layer act a s repulsive force for tensi le thermal stress a t minimum cross section area. Figure 4 shows the scanning electron microscopy (SEMI photography of typical fabr icated nanostructure with about 250 nm gap which was formed a f t e r annealing a t 1100 'C for 1 hour Conclusion We fabricated the s i l i con nanostructure wi th nanometer sca le gap using thin film s t r e s s The gap width which was formed i n the layers during thermal annealing a t high temperature could be controlled by annealing temperature and annealing time.
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利用薄膜应力制备纳米尺度结构
我。在光学光刻、干式蚀刻、AFM加工工具和电子束光刻等技术的广泛应用中,制备了大量的光学光刻、干式蚀刻、电子束光刻等技术。但这些方法成本高,工艺复杂,适用于大规模工艺。在过去,我们已经报道了基于多晶硅层的20纳米间隙的纳米级形成。现在,我们将提出一种简单的纳米尺度的形成技术,将纳米尺度的形成技术与纳米层相结合,并阐明形成机理。11. 图1 (A)给出了楔形纳米结构的关键制备工艺示意图。在厚度为4000 A- sioz的SIMOX晶片上,用LPCM法在厚度为700 -C的SIMOX晶片上沉积了1600 A的Si3N4层。在光刻成片后,将硅和硅两层进行干燥蚀刻,底部的二氧化硅层在控制下蚀刻,并在不同温度和时间的N2环境下进行退火。图1 (b)为带间隙的预制楔型结构示意图。该间隙是由退火和冷却过程中产生的应力在图案楔的最小横截面积处形成的。图2显示了在退火过程中形成的每一层中所含的金属的分布情况。我n层形成的压应力f i n y l l c t年代十我勒强调一个t的最小横教派离子面积s t生成。如果热应力较大,则合并面积为1 / 2,并形成间隙,图3显示了在1 / 1100℃下,在2 pm和11 pm Si02刻蚀时,两者之间的间隙随退火时间的演变。在2 μ m和11 μ m的sio2蚀刻下,间隙分别饱和在250 nm和190 nm左右。所测30个样品的间隙宽度均在平均饱和值的*lox以内。本文认为,在不同的sio2刻蚀条件下,两者之间的间隙差异是由于sio2层对拉伸热应力的排斥力小于最小横截面面积造成的。图4显示了典型的扫描电镜(半摄影fabr icated纳米结构差距约250海里,是形成了一个f t e r退火1100 C 1小时的结论我们捏造的年代我l con纳米结构将纳米sca le差距使用薄膜t r e s年代形成的间隙宽度我n层在高温热退火t可以控制退火温度和退火时间。
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