Van Bui H, Aarnink A A I, Kovalgin A Y, Wolters R A M
MESA+ Institute for Nanotechnology, Chair of Semiconductor Components, University of Twente, P.O. Box 217, 7500 AE Enschede, The Netherlands.
J Nanosci Nanotechnol. 2011 Sep;11(9):8120-5. doi: 10.1166/jnn.2011.5069.
We report the electrical resistivity of atomic layer deposited TiN thin films in the thickness range 2.5-20 nm. The measurements were carried out using the circular transfer length method structures. For the films with thickness in the range of 10-20 nm, the measurements exhibited linear current-voltage (I-V) curves. The sheet resistance R(sh) was determined, and the resistivity was calculated. A value of 120 microohms-cm was obtained for a 20 nm TiN layer. With decreasing film thickness, the resistivity slightly increased and reached 135 microohms-cm for a 10 nm film. However, the measurements on 2.5-5.0 nm thick films revealed non-linear I-V characteristics, implying the dependence of the measured resistance, and therefore the resistivity, of the layers on applied voltage. The influence of the native oxidation due to the exposure of the films to air was taken into account. To fully eliminate this oxidation, a highly-resistive amorphous silicon layer was deposited directly after the ALD of TiN. The electrical measurements on the passivated 2.5- and 3.5 nm TiN layers then exhibited linear I-V characteristics. A resistivity of 400 and 310 microohms-cm was obtained for a 2.5- and 3.5 nm TiN film, respectively.
我们报告了原子层沉积的厚度在2.5 - 20纳米范围内的TiN薄膜的电阻率。测量是使用圆形转移长度法结构进行的。对于厚度在10 - 20纳米范围内的薄膜,测量显示出线性电流 - 电压(I - V)曲线。确定了薄层电阻R(sh),并计算了电阻率。对于20纳米厚的TiN层,得到的值为120微欧厘米。随着薄膜厚度的减小,电阻率略有增加,对于10纳米厚的薄膜达到135微欧厘米。然而,对2.5 - 5.0纳米厚薄膜的测量显示出非线性I - V特性,这意味着所测量的层电阻以及因此电阻率取决于施加的电压。考虑了薄膜暴露于空气中导致的自然氧化的影响。为了完全消除这种氧化,在TiN的原子层沉积之后直接沉积了高电阻非晶硅层。然后对钝化后的2.5纳米和3.5纳米TiN层进行的电学测量显示出线性I - V特性。对于2.5纳米和3.5纳米的TiN薄膜,分别获得了400和310微欧厘米的电阻率。