并五苯MIS结构C-V特征的积累迁移率提取

Keum-dong Jung, C. Lee, Dong-Wook Park, Byung-Gook Park, Hyungcheol Shin, J. Lee
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引用次数: 1

摘要

提出了一种提取并五苯薄膜积累迁移率的新方法。为了得到迁移率,利用并五烯MIS结构的电容-电压特性,得到了负栅偏压下的片电阻和薄膜的累积电荷。提取的迁移率值比常规方法[1]从ofet的I-V特性确定的迁移率值低24%。除了迁移率作为有机电子学的关键性能因素受到关注外,迁移率提取方法本身也得到了广泛的研究。大多数使用I-V特性的方法需要精确的IV方程,如硅长沟道MOSFET模型,但建立通用的OFET I-V方程一直是一个难题。因此,为了提取更可靠的迁移率,本文提出了一种利用并五苯MIS结构的C-V特征提取迁移率的新方法。图1显示了制造器件的横截面视图和俯视图。采用n+-Si晶片作为栅电极,35 nm厚的氧化物作为栅绝缘体。将稀释PMMA旋涂在SiO2上进行表面处理。最后,并五苯和金通过阴影面具依次蒸发。外围区域的宽度W由阴影掩模控制,从15ptm到95ptm。采用14P4284A LCR表,频率为100 Hz -1 MHz,栅极电压为0 V -10 V,在空气中测量C-V特性。在图2中,器件的测量电容值(C101)被分为三个不同的电容:绝缘体电容(C1),并五苯金重叠电容(C2)和外围区域电容(Cp)。由MIM电容直接测得Ci,由C0 = C101 C和C = Ct1tC, C-C关系式间接得到C0和Cp。图3和图4分别显示了不同栅极偏置和测量频率下Ct、t(W=75 rim)的分离情况。要从特定栅极电压(例如VG= -10 V)下的pac= 1 IPhQA中提取积累迁移率pcac,则需要知道在VG= -10 V时的片电阻Psh和单位面积总积累电荷QA。首先,在VG = -10 V时,QA为716.22 nC/cm2,直接由图5曲线[2]对C0的积分得到。根据11C0V2曲线确定集成中的平带电压VFB为-1.08 V。接下来,为了从外围区电容CP得到Psh,采用图6中的R- c网络模型来描述CP随频率的变化,假设整个外围区电阻R均匀,n+ si栅极和触点电阻可忽略。通过类比硅mosfet[3]的小信号栅极电阻模型,得到Cp与频率的关系为
本文章由计算机程序翻译,如有差异,请以英文原文为准。
Extraction of Accumulation Mobility from C-V Characteristics of Pentacene MIS Structures
A novel method for extracting accumulation mobility of pentacene thin films has been proposed. To obtain the mobility, the sheet resistance and the accumulation charge of the film under negative gate bias are obtained from the capacitance-voltage(C-V) characteristics of the pentacene MIS structures. The value of the extracted mobility is 24% lower than that determined from the I-V characteristics ofOFET by conventional method [1]. Besides the attention paid to the mobility as a key performance factor in organic electronics, the mobility extraction method itself has been studied widely. Most of the methods using I-V characteristics require an accurate IV equation such as the silicon long-channel MOSFET model, but establishing a general OFET I-V equation has been a difficult problem. Therefore, to extract more reliable mobility, a novel mobility extraction method using C-V characteristics of pentacene MIS structure is described in this paper. Fig. 1 shows the cross-sectional view and top view of the fabricated devices. An n+-Si wafer is used as a gate electrode, and 35 nm-thick oxide is used as a gate insulator. Dilute PMMA is spin-coated on the SiO2 for the surface treatment. Finally, pentacene and gold are evaporated sequentially through shadow masks. The width W of the peripheral region is controlled by the shadow mask from 15 ptm to 95 ptm. C-V characteristics are measured in air with 14P4284A LCR meter with the frequency of 100 Hz -1 MHz and the gate voltage of-O0 V -10 V. In Fig. 2, the value of measured capacitance(C101) of the device is separated into three different capacitances: the insulator capacitance(C1), pentacene-gold overlapping capacitance(C2), and the peripheral region capacitance(Cp). Ci is directly measured from MIM capacitor, and C0, and Cp are indirectly obtained using the relation of C0,= C101 C, and C,= Ct1tC, C-C. Fig. 3 and Fig. 4 show the separation of Ct,t(W=75 rim) with different gate bias and measuring frequency, respectively. To extract the accumulation mobility pcac from pac= 1 IPhQA at a specific gate voltage, e.g., VG= -10 V, the sheet resistance Psh and the total accumulation charge per unit area QA at VG= -10 V should be known. First, QA of 716.22 nC/cm2 at VG = -10 V is directly obtained from the integration of C0, curve [2] as shown in Fig. 5. The flat band voltage VFB in the integration is determined from 11C0V2 curve to be -1.08 V. Next, to obtain Psh from the peripheral region capacitance CP, R-C network model in Fig. 6 is adopted to describe CP versus frequency behavior assuming uniform resistance R along the whole peripheral region and negligible resistance in the n+-Si gate and the contact. By the analogy with the small-signal gate resistance model of silicon MOSFETs [3], Cp versus frequency relation is given as
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