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多个硅通孔引起的热应力对迁移率和阻止区的影响
引用本文:董刚,刘荡,石涛,杨银堂. 多个硅通孔引起的热应力对迁移率和阻止区的影响[J]. 物理学报, 2015, 64(17): 176601-176601. DOI: 10.7498/aps.64.176601
作者姓名:董刚  刘荡  石涛  杨银堂
作者单位:西安电子科技大学微电子研究所, 宽禁带半导体材料与器件教育部重点实验室, 西安 710071
基金项目:国家自然科学基金(批准号: 61334003)资助的课题.
摘    要:本文主要讨论了多个硅通孔引起的热应力对迁移率和阻止区的影响, 得到了器件沟道沿[100]方向时, 硅通孔之间的角度和间距对电子迁移率和阻止区的影响. 设定两种阻止区区域, 即迁移率变化分别为5%和10%的区域, 且主要考虑相邻TSV之间的区域. 仿真结果表明: 当硅通孔和X轴所成角度为π/4时, 电子迁移率变化和阻止区区域最小, 但是可布置器件区域不规则, 不易于布局. 随着间距的增加, 电子迁移率变化和阻止区区域逐渐增大, 趋向于单个TSV的情况; 当角度为0 时, 电子迁移率变化和阻止区区域变大, 可布置器件区域为硅通孔围成的中心小区域上, 形状比较规则, 便于布局. 而且随着间距的增加, 电子迁移率变化和阻止区区域越来越小, 趋向于单个硅通孔的情况.

关 键 词:硅通孔  热应力  迁移率变化  阻止区
收稿时间:2015-03-15

Effects of thermal stress induced by mulitiple through silicon vias on mobility and keep out zone
Dong Gang,Liu Dang,Shi Tao,Yang Yin-Tang. Effects of thermal stress induced by mulitiple through silicon vias on mobility and keep out zone[J]. Acta Physica Sinica, 2015, 64(17): 176601-176601. DOI: 10.7498/aps.64.176601
Authors:Dong Gang  Liu Dang  Shi Tao  Yang Yin-Tang
Affiliation:Key Laboratory of Ministry of Education for Wide Band-Gap Semiconductor Materials and Devices, Microelectronics Institute, Xidian University, Xi'an 710071, China
Abstract:Effects of thermal stress induced by multiple through silicon vias (TSVs) on mobility and keep out zone (KOZ) are mainly discussed in this paper. It is found that the angle and pitch between TSVs have a great effect on the carrier mobility and KOZ. In this paper, the device channel direction is set along [100]. And two types of KOZ are presented, namely the variations of electron mobility are 5% and 10% respectively. As for the two TSVs, their KOZ sizes change significantly with the angles between TSVs which change from zero to π/4, and the area of a KOZ is the minimum when the angle is π/4. But the zone for device placement is irregular, which is difficult for agreement. The area of a KOZ is the maximum when the angle is zero, and it is easy to make arrangement as the space for device distribution is regular. Based on these analyses, the effects of pitch between TSVs are presented. When the angle is zero, the area of KOZ decreases as the pitch increases and tends to be the same as that of a single TSV. For example, the KOZ, in which the variations of electron mobility are 5% and 10%, will reduce to 8.4 μm and 5.1 μm as the pitch increases to 20 μm, which is close to that of the single TSV. But when the angle is π/4, the KOZ with an electron mobility 5% increases from 5.2 to 6.4 μm as the pitch increases and tends to be the same as that of a single TSV at last. The KOZ with an electron mobility 10% will increase from 4.2 to 4.5 μm. In addition, the above analyses can be extended to the KOE of four TSVs, a more representative pattern. And two kinds of TSV displacement style including “square” and "diamond" TSV patterns are also discussed, the impact of pitch for these two patterns are also given in this paper. For the “square” TSV pattern, the KOZ decreases as the pitch increases. Under this condition, the devices can only be placed in a small square region surrounded by TSVs, but the region is regular, which is beneficial for device arranging. While for the "diamond" TSV pattern, the KOZ increases as the pitch increases. Under this condition, the area for device placement is larger than the “square” TSV pattern, but the region is irregular as it is divided into long narrow parts, which is hard for device placement.
Keywords:through silicon via  thermal stress  mobility variation  keep out zone
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