薄膜晶体管的二维漏极减漏工程

T. King, M. Hack
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In these structures, the LDD region is placed between the channel and the heavily doped drain and spans the entire thickness of the channel, so that the drain dopant concentration varies only in one dimension (parallel to the gate). LDD structures are difficult to implement in poly-Si due to the poor controllability of dopant activation at concentrations below -lo1* ~m-~: underdoping of the LDD region results in decreased drive current in offset-drain structures, while over-doping results in a loss of the benefit of reduced leakage current. In this work, the two-dimensional (2D) engineering of drain doping profiles is demonstrated to provide significant advantages over conventional (1D) LDD engineering approaches for reducing TFT leakage current. Top-gate n-channel poly-Si TFTs were fabricated on quartz wafers using a conventional high- temperature (950°C) process3. After the formation of the heavily doped (nt) source and drain regions, some wafers were given additional implants at high tilt angles, to form lightly doped (n-) 1D or 2D LDD regions underneath the gate, extending -0.3 pm in from the gate edge. The 1D LDD regions were formed by deep implantation of phosphorus to a dose of 2 x 1013 The 2D LDD regions were formed using a combination of high-angle implants: a deep phosphorus implant (identical to the one used to form the 1D LDD structures), and a shallow counterdoping boron implant to confine the n- LDD region to the bottom region of the channel layer. A 1 hour anneal at 55OOC was used to activate the LDD implants. TFT measurements show that the 1D LDD structure provides a noticeable reduction in leakage com- pared with the standard drain structure, as expected: the median value is reduced from 0.94 pA/pm to 0.61 pA/pm, and the 20%-80% distribution spread is decreased from -16x to xllx. However, substantial further reduction is provided by the 2D LDD structure: the median value is reduced to 0.34 pA/pm and to 0.17 pA/pm with counterdoping boron implant doses of 4x 1OI2 cm-2 and 1 x 1013 cm-2, respectively. (The 20%-80% distribution spreads for the-2D LDD structures are -11 x.) Leakage was confirmed to scale linearly with TFT channel width for the devices fabricated in this work, in order to rule out edge contributions. Numerical device simulations4 indicate that 2D variation of the drain profile can significantly impact lateral electric-field strength Ell in the channel region near the drain: Ellmsx is lowered considerably by moving the extended drain region away from the gate electrode, regardless of the dopant concentration in this region. This technique provides a means for manipulating not only the location hut also the physical extent of the high-field region near the drain. Compared with a conventional LDD structure, a 2D-engineered drain structure can provide substantial improvements in TFT leakage, with more resilience against variations in dopant activation in the extended drain region. In summary, 2D engineering of drain doping profiles provides a significant advantage over conventional 1D engineering approaches for achieving low leakage in poly-Si TFTs. Simulations show that this is due to reductions in the extent and magnitude of the lateral electric field in the channel near the drain.","PeriodicalId":244069,"journal":{"name":"52nd Annual Device Research Conference","volume":"7 1","pages":"0"},"PeriodicalIF":0.0000,"publicationDate":"1994-06-20","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"2","resultStr":"{\"title\":\"Two-dimensional drain engineering for leakage reduction in thin-film transistors\",\"authors\":\"T. King, M. 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In these structures, the LDD region is placed between the channel and the heavily doped drain and spans the entire thickness of the channel, so that the drain dopant concentration varies only in one dimension (parallel to the gate). LDD structures are difficult to implement in poly-Si due to the poor controllability of dopant activation at concentrations below -lo1* ~m-~: underdoping of the LDD region results in decreased drive current in offset-drain structures, while over-doping results in a loss of the benefit of reduced leakage current. In this work, the two-dimensional (2D) engineering of drain doping profiles is demonstrated to provide significant advantages over conventional (1D) LDD engineering approaches for reducing TFT leakage current. Top-gate n-channel poly-Si TFTs were fabricated on quartz wafers using a conventional high- temperature (950°C) process3. 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引用次数: 2

摘要

在多晶硅薄膜晶体管中,漏极掺杂谱的二维变化比传统漏极工程技术更有利于实现低漏极。多晶硅(poly-Si)薄膜晶体管(TFTs)用于有源矩阵液晶显示器和图像传感器等对tft泄漏有严格要求的应用中。实验研究表明,影响漏电流的主要因素之一是漏极附近通道区域的电场强度。轻掺杂漏极(LDD)结构先前已被用于减少漏极结处的电场,从而减少TFT漏电流2。在这些结构中,LDD区域位于沟道和高掺杂漏极之间,并横跨整个沟道厚度,因此漏极掺杂剂浓度仅在一维(平行于栅极)上变化。由于掺杂剂在浓度低于-lo1* ~m-~时激活的可控性较差,LDD结构难以在多晶硅中实现:LDD区域的欠掺杂导致偏置漏极结构的驱动电流降低,而过度掺杂导致泄漏电流降低的好处丧失。在这项工作中,二维(2D)漏极掺杂剖面工程被证明比传统(1D) LDD工程方法在降低TFT泄漏电流方面具有显著优势。采用传统的高温(950°C)工艺在石英晶圆上制备顶栅n沟道多晶硅tft。在形成高掺杂(nt)源极和漏极区域后,在高倾斜角度下对一些晶圆进行额外的植入,在栅极下方形成轻掺杂(n-) 1D或2D LDD区域,从栅极边缘延伸-0.3 pm in。二维LDD区域的形成使用高角度植入物的组合:深磷植入物(与用于形成1D LDD结构的植入物相同)和浅反掺杂硼植入物,将n- LDD区域限制在通道层的底部区域。在55OOC下退火1小时激活LDD植入物。TFT测量表明,与标准漏极结构相比,1D LDD结构的泄漏量明显降低,正如预期的那样:中位数从0.94 pA/pm降至0.61 pA/pm, 20%-80%的分布范围从-16倍降至xllx。然而,2D LDD结构提供了进一步的实质性降低:中位值分别降低到0.34 pA/pm和0.17 pA/pm,反掺杂硼植入剂量分别为4 × 10i2 cm-2和1 × 1013 cm-2。(二维LDD结构的20%-80%分布差为-11 x。)为了排除边缘贡献,泄漏被证实与在这项工作中制造的器件的TFT通道宽度成线性比例。数值装置模拟表明,漏极轮廓的二维变化会显著影响漏极附近沟道区域的横向电场强度:无论漏极区域的掺杂浓度如何,将延伸漏极区域移离栅极都能显著降低Ellmsx。这种技术提供了一种手段,不仅可以操纵位置,而且可以操纵排水沟附近高场区域的物理范围。与传统的LDD结构相比,2d工程漏极结构可以显著改善TFT泄漏,并且在扩展漏极区域对掺杂剂激活的变化具有更强的弹性。总之,在实现多晶硅tft的低泄漏方面,漏极掺杂曲线的二维工程比传统的一维工程方法具有显著的优势。模拟结果表明,这是由于漏极附近通道中横向电场的范围和强度减小所致。
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Two-dimensional drain engineering for leakage reduction in thin-film transistors
The variation of drain dopant profiles in two dimensions is shown to be superior to tradi- tional drain-engineering techniques for achieving low leakage in poly-Si thin-film transistors. Polycrystalline silicon (poly-Si) thin-film transistors (TFTs) are used in applications such as active- matrix liquid-crystal displays and image sensors, which have stringent TFT-leakage requirements. Experimental studies have shown that one of the main factors which affects leakage current is the electric-field strength in the channel region near the drain'. Lightly doped drain (LDD) structures have previously been used to reduce the electric field at the drain junction and thereby reduce TFT leakage current2. In these structures, the LDD region is placed between the channel and the heavily doped drain and spans the entire thickness of the channel, so that the drain dopant concentration varies only in one dimension (parallel to the gate). LDD structures are difficult to implement in poly-Si due to the poor controllability of dopant activation at concentrations below -lo1* ~m-~: underdoping of the LDD region results in decreased drive current in offset-drain structures, while over-doping results in a loss of the benefit of reduced leakage current. In this work, the two-dimensional (2D) engineering of drain doping profiles is demonstrated to provide significant advantages over conventional (1D) LDD engineering approaches for reducing TFT leakage current. Top-gate n-channel poly-Si TFTs were fabricated on quartz wafers using a conventional high- temperature (950°C) process3. After the formation of the heavily doped (nt) source and drain regions, some wafers were given additional implants at high tilt angles, to form lightly doped (n-) 1D or 2D LDD regions underneath the gate, extending -0.3 pm in from the gate edge. The 1D LDD regions were formed by deep implantation of phosphorus to a dose of 2 x 1013 The 2D LDD regions were formed using a combination of high-angle implants: a deep phosphorus implant (identical to the one used to form the 1D LDD structures), and a shallow counterdoping boron implant to confine the n- LDD region to the bottom region of the channel layer. A 1 hour anneal at 55OOC was used to activate the LDD implants. TFT measurements show that the 1D LDD structure provides a noticeable reduction in leakage com- pared with the standard drain structure, as expected: the median value is reduced from 0.94 pA/pm to 0.61 pA/pm, and the 20%-80% distribution spread is decreased from -16x to xllx. However, substantial further reduction is provided by the 2D LDD structure: the median value is reduced to 0.34 pA/pm and to 0.17 pA/pm with counterdoping boron implant doses of 4x 1OI2 cm-2 and 1 x 1013 cm-2, respectively. (The 20%-80% distribution spreads for the-2D LDD structures are -11 x.) Leakage was confirmed to scale linearly with TFT channel width for the devices fabricated in this work, in order to rule out edge contributions. Numerical device simulations4 indicate that 2D variation of the drain profile can significantly impact lateral electric-field strength Ell in the channel region near the drain: Ellmsx is lowered considerably by moving the extended drain region away from the gate electrode, regardless of the dopant concentration in this region. This technique provides a means for manipulating not only the location hut also the physical extent of the high-field region near the drain. Compared with a conventional LDD structure, a 2D-engineered drain structure can provide substantial improvements in TFT leakage, with more resilience against variations in dopant activation in the extended drain region. In summary, 2D engineering of drain doping profiles provides a significant advantage over conventional 1D engineering approaches for achieving low leakage in poly-Si TFTs. Simulations show that this is due to reductions in the extent and magnitude of the lateral electric field in the channel near the drain.
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