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XPS Analyses and Work Function Extraction of Titanium Nitride Electrodes for MOS Technology and Schoktty Diode.

机译:XPS分析和功函数提取MOS技术和斯科蒂二极管的氮化钛电极。

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Titanium nitride (TiN) films have been obtained by DC sputtering deposition in a nitrogen/argon ambient on Si substrates. TiN film have been used as gate electrodes in MOS capacitors, which were fabricated with SiO_2 as gate dielectric, and in Schoktty diodes on n-type Si (100) substrates. 20nm and 100nm thick TiN layers were deposited by DC sputtering in N_2:Ar (20:60 sccm) ambient, with a sputtering power of 1000 W. These films presented electrical resistivity of 300 μΩ.cm and poly crystalline strucure [1]. XPS analysis evidence TiN and TiO_xN_y formation in both 20 nm (Figure 1a) and 100 nm (Figure 1b) thick films. TiO_xN_y formation could be related with the exposure the metal electrode to air. To get MOS capacitors with TiN/SiO_2/Si/AI and AI/TiN/SiO_2/Si/AI structures, the Si substrates were used and were cleaned with a standard RCA method. After, dry thermal oxidation at 1000°C for 2 min was carried out and a 8 nm thick SiO_2 layer on Si was obtained. 20 nm and 100nm thick TiN layer was deposited on SiO_2/Si by DC sputtering. Finally, in some devices a 200nm thick alumininum (Al) layer was deposited on TiN layer by DC sputtering, in order to reduce the TiO_xN_y formation on the metal electrode. MOS capacitor pattern was defined by a mask composed of an array of 200 pm diameter dots. These devices were sintered in conventional furnace in forming gas at 450 °C for 30 minutes and were electrical characterized by capacitance-voltage (C-V) measurements. Figure 2 presents MOS capacitor C-V characteristics.TiN work function values and flat-band voltage were extracted from all C-V measurements using CVC software [2] and 1/C<@@>~2 method [3]. The extracted TiN work function values and flat-band voltage were between 4.0 and 4.3 eV, -0.17 and 0.36 V, respectively. These results agree with results presented on Reference [4]. The variations on work function values are related with the dipole variations due the interface between metal and dielectric. To investigate the TiN work function, Schoktty diodes were fabricated in the same substrate of MOS capacitors. Titanium nitride (TiN) layer were deposited by DC sputtering in a N_2:Ar (20:60 sccm) ambient, with a sputtering power of 1000 W. TiN/Si/AI and AI/TiN/Si/AI diodes were formed with TiN (20nm and 100nm) gate electrodes and Al layer (200nm) were deposited by DC sputtering process. These diodes were sintered in conventional furnace in forming gas at 450 °C for 30 minutes. The electrodes were patterned with a mask composed of an array of 200 μm diameter dots. These diodes were electrical characterized by current-voltage (I-V) measurements (Figure 3 and 4), and the ideality factor between 1.0 and 3.2, and work function values between 4.4 and 4.5 eV were extracted, which is near the work function values for mid-gap electrode application [4,5]. The TiN work function values extracted from MOS capacitors and Schottky diodes with Al/TiN/SiO_2/Si/Al and lI/TiN/Si/Al sctructures were slightly higher than the TiN work function values extracted from same devices with the TiN/SiO_2/Si/Al and TiN/Si/AI structures, indicating that the TiN work function values increases with a lower incorporation of TiO_xN_y on the surface of TiN films.
机译:氮化钛(TIN)膜已通过DC溅射沉积在Si衬底上的氮/氩环境获得。 TiN膜已被用作在MOS电容器的栅极电极,其作为栅极电介质制造了与SiO_2,并在n型Si(100)衬底Schoktty二极管。为20nm和100nm厚的TiN层是通过DC沉积在N_2溅射:氩(20:60 SCCM)周围,以1000层W.这些膜的溅射功率呈现300μΩ.cm的电阻率和多晶strucure [1]。 XPS分析证据TiN和在两个20纳米(图1a)形成TiO_xN_y且100nm(图1b)厚的薄膜。 TiO_xN_y形成可能与曝光的金属电极,以空气有关。为了得到MOS电容有TiN / SiO_2 /的Si / Al和AI /锡/ SiO_2 /的Si / Al结构中,使用Si衬底,并用标准的RCA方法进行清洗。之后,在1000℃下干燥热氧化2分钟进行,得到在Si一个8纳米厚SiO_2层。为20nm和100nm厚的TiN层,通过DC溅射淀积上SiO_2 / Si的。最后,在一些设备中厚200nm alumininum(Al)的层通过DC溅射沉积TiN层上,以减少在金属电极上的形成TiO_xN_y。 MOS电容器图案用的200点微米直径的点的阵列构成的掩模限定。这些装置在常规炉中在450℃下烧结形成气体中进行30分钟,然后电其特征在于,电容 - 电压(C-V)测量。图2呈现MOS电容器C-V characteristics.TiN功函数值,并平带电压是从使用CVC软件[2]和1 / C <@@>〜2方法[3]所有的C-V测量萃取。所提取的TiN的功函数值,并且平带电压分别为4.0和4.3电子伏特,-0.17和0.36 V,之间。这些结果与呈现在参考文献[4]的结果。上的功函数值的变化与由于金属和电介质之间的界面处的偶极子变化有关。为了研究在TiN功函数,Schoktty二极管在MOS电容器的在同一基片被制造。有TiN形成的Ar(20:60 SCCM)的环境,为1000 W.锡/硅/ AI和AI /锡/硅/ AI二极管的溅射功率:氮化钛(TIN)层通过DC在N_2溅射沉积(20纳米和100nm)的栅电极和Al层(200nm的)通过DC溅射方法沉积。这些二极管是在常规炉中在450℃下进行30分钟形成气体烧结。这些电极与一个200个微米直径的圆点排列组成掩模图案化。这些二极管是电,其特征在于电流 - 电压(IV)测量(图3和4),和4.4和4.5电子伏特之间的1.0和3.2,和功函数值之间的理想因子提取,这是接近用于中功函数值-gap电极应用[4,5]。从MOS电容器和肖特基二极管用Al /锡/ SiO_2 /的Si / Al和Li /锡萃取的TiN的功函数值/硅/铝sctructures比从具有相同的设备中提取在TiN的功函数的值稍高的锡/ SiO_2 /的Si / Al和TiN /的Si / Al结构,表明与TiO_xN_y的TiN薄膜的表面上的下掺入在TiN的功函数的值的增加。

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