Sprenger Jaclyn K, Sun Huaxing, Cavanagh Andrew S, Roshko Alexana, Blanchard Paul T, George Steven M
Department of Chemistry and Biochemistry, University of Colorado, Boulder, Colorado 80309, United States.
National Institute of Standards and Technology, Boulder, Colorado 80305, United States.
J Phys Chem C Nanomater Interfaces. 2018;122(17). doi: https://doi.org/10.1021/acs.jpcc.8b00796.
Electron-enhanced atomic layer deposition (EE-ALD) was used to deposit boron nitride (BN) thin films at room temperature and 100 °C using sequential exposures of borazine (BNH) and electrons. Electron-stimulated desorption (ESD) of hydrogen surface species and the corresponding creation of reactive dangling bonds are believed to facilitate borazine adsorption and reduce the temperature required for BN film deposition. In situ ellipsometry measurements showed that the BN film thickness increased linearly versus the number of EE-ALD cycles at room temperature. Maximum growth rates of ~3.2 Å/cycle were measured at electron energies of 80-160 eV. BN film growth was self-limiting versus borazine and electron exposures, as expected for an ALD process. The calculated average hydrogen ESD cross section was = 4.2 × 10 cm. Ex situ spectroscopic ellipsometry measurements across the ~1 cm area of the BN film defined by the electron beam displayed good uniformity in thickness. Ex situ X-ray photoelectron spectroscopy and in situ Auger spectroscopy revealed high purity, slightly boron-rich BN films with C and O impurity levels <3 at. %. High-resolution transmission electron microscopy (HR-TEM) imaging revealed polycrystalline hexagonal and turbostratic BN with the basal planes approximately parallel to the substrate surface. Ex situ grazing incidence X-ray diffraction measurements observed peaks consistent with hexagonal BN with domain sizes of 1-2 nm. The BN EE-ALD growth rate of ~3.2 Å/cycle is close to the distance of 3.3 Å between BN planes in hexagonal BN. The growth rate and HR-TEM images suggest that approximately one monolayer of BN is deposited for every BN EE-ALD cycle. TEM and scanning TEM/electron energy loss spectroscopy measurements of BN EE-ALD on trenched wafers also showed preferential BN EE-ALD on the horizontal surfaces. This selective deposition on the horizontal surfaces suggests that EE-ALD may enable bottom-up filling of vias and trenches.
采用电子增强原子层沉积(EE-ALD)技术,在室温及100°C条件下,通过依次暴露硼嗪(BNH)和电子来沉积氮化硼(BN)薄膜。据信,氢表面物种的电子激发脱附(ESD)以及相应的活性悬空键的产生有助于硼嗪的吸附,并降低BN薄膜沉积所需的温度。原位椭偏测量表明,在室温下,BN薄膜厚度随EE-ALD循环次数呈线性增加。在80 - 160 eV的电子能量下,测得的最大生长速率约为3.2 Å/循环。正如原子层沉积(ALD)过程所预期的那样,BN薄膜的生长对硼嗪和电子暴露具有自限性。计算得出的平均氢ESD截面为 = 4.2 × 10 cm。在由电子束定义的约1 cm²面积的BN薄膜上进行的非原位光谱椭偏测量显示,厚度具有良好的均匀性。非原位X射线光电子能谱和原位俄歇能谱表明,BN薄膜纯度高,略富硼,碳和氧杂质含量<3原子%。高分辨率透射电子显微镜(HR-TEM)成像显示为多晶六方和乱层BN,其基面大致平行于衬底表面。非原位掠入射X射线衍射测量观察到与六方BN一致的峰,畴尺寸为1 - 2 nm。BN的EE-ALD生长速率约为3.2 Å/循环,接近六方BN中BN平面之间3.3 Å的间距。生长速率和HR-TEM图像表明,每进行一次BN的EE-ALD循环,大约沉积一个单层的BN。对有沟槽的晶圆上的BN EE-ALD进行的TEM以及扫描TEM/电子能量损失谱测量还表明,在水平表面上BN的EE-ALD具有优先性。这种在水平表面上的选择性沉积表明,EE-ALD可能实现通孔和沟槽的自下而上填充。