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    • 4. 发明授权
    • Interlevel dielectric with multiple air gaps between conductive lines of
an integrated circuit
    • 集成电路的导线之间具有多个气隙的层间电介质
    • US5994776A
    • 1999-11-30
    • US63481
    • 1998-04-20
    • Peng FangHomi Fatemi
    • Peng FangHomi Fatemi
    • H01L21/768H01L23/522H01L23/532H01L23/48H01L23/52H01L29/40
    • H01L23/5222H01L21/7682H01L23/5329H01L23/53295H01L2924/0002
    • A method of forming low dielectric insulation between pairs of conductive lines separated by insulating material of a level of interconnection for integrated circuits by selectively removing portions of the insulating material to create spaces for containing a gas with a dielectric constant of slightly above 1. Preferably, the insulating material is a conformal source of silicon oxide, such as tetraethylorthosilicate. The resultant method forms an insulation separating the conductive lines whose composite dielectric constant with the gas in the spaces between the insulating material is not greater than about 3 over a predetermined distance. An integrated circuit having a plurality of semiconductor devices being interconnected by conductive lines separated by insulating material and spaces containing a gas, composite dielectric constant of which is not greater than about 3 over a predetermined distance.
    • 通过选择性地去除绝缘材料的部分以产生用于容纳介电常数略高于1的气体的空间,形成由用于集成电路的互连级别的绝缘材料隔开的导电线之间的低介电绝缘的方法。优选地, 绝缘材料是氧化硅的保形源,例如原硅酸四乙酯。 所得到的方法形成绝缘体,其绝缘材料的绝缘材料的复合介电常数与绝缘材料之间的间隔不大于约3°的预定距离的导线。 一种具有多个半导体器件的集成电路,其通过由绝缘材料隔开的导线和包含气体的空间互相连接,复合介电常数在预定距离以上不大于约3。
    • 5. 发明授权
    • Short channel self aligned VMOS field effect transistor
    • 短沟道自对准VMOS场效应晶体管
    • US5808340A
    • 1998-09-15
    • US714317
    • 1996-09-18
    • Donald L. WollesenHomi Fatemi
    • Donald L. WollesenHomi Fatemi
    • H01L21/336H01L29/423H01L29/45H01L29/49H01L29/78H01L29/76H01L29/94
    • H01L29/78H01L29/66621H01L29/456H01L29/49
    • A field effect transistor with a trench or groove gate having V-shaped walls is formed in a semiconductor substrate and a gate oxide is grown on the V-shaped walls to the surface of substrate and filled with a gate electrode material, such a polysilicon. Preferably, the bottom of the V-shaped walls are rounded before the trench is filled. Source/drain impurities either are diffused or implanted into the areas of the substrate on both sides of the surface oxide of the V-shaped gate. Contacts are made to the source, drain, and gate within field isolation to complete the structure. The resultant FET structure comprises a self aligned V-shaped gate having conventional source and drain surrounded by field isolation but with an effective channel length (L.sub.eff) of less than about one-half of the surface width of the gate. Preferably, the converging walls of the V-shaped gate end in a rounded concave bottom. Because of the V-shaped structure of the gate, the effective saturated length of the channel with drain voltage applied only extends from the edge of the source to just prior to the tip of the V-shaped structure in the interior of the semiconductor substrate. The drain side of the V-shaped structure becomes a depletion region due to the applied drain voltage. Due to this characteristic of such a structure, the surface width of the gate can be, for example, two or more times the distance of the desired channel length thereby permitting conventional lithography to be used to define the gate lengths much shorter than the lithographic limit.
    • 在半导体衬底中形成具有V形壁的沟槽或沟槽栅极的场效应晶体管,并且在V形壁上生长栅极氧化物到衬底表面,并且填充有诸如多晶硅的栅电极材料。 优选地,在填充沟槽之前,V形壁的底部是圆形的。 源极/漏极杂质可以扩散或注入到V形栅极的表面氧化物两侧的衬底区域中。 触点在场隔离中被制成源极,漏极和栅极,以完成结构。 所得到的FET结构包括具有常规源极和漏极的自对准V形栅极,该源极和漏极被场隔离包围,但具有小于栅极表面宽度的约一半的有效沟道长度(Leff)。 优选地,V形门的会聚壁在圆形凹入的底部中。 由于栅极的V形结构,所以施加漏极电压的沟道的有效饱和长度仅从源极的边缘延伸到半导体衬底内部的V形结构的尖端之前。 V形结构的漏极侧由于施加的漏极电压而变为耗尽区。 由于这种结构的这种特性,栅极的表面宽度可以是例如期望沟道长度的两倍或更多倍的距离,从而允许常规光刻用于限定比光刻极限短的栅极长度 。
    • 6. 发明授权
    • Short channel self-aligned VMOS field effect transistor
    • 短沟道自对准VMOS场效应晶体管
    • US5960271A
    • 1999-09-28
    • US42786
    • 1998-03-17
    • Donald L. WollesenHomi Fatemi
    • Donald L. WollesenHomi Fatemi
    • H01L21/336H01L29/423H01L29/45H01L29/49H01L29/78
    • H01L29/78H01L29/66621H01L29/456H01L29/49
    • A field effect transistor with a trench or groove gate having V-shaped walls is formed in a semiconductor substrate and a gate oxide is grown on the V-shaped walls to the surface of substrate and filled with a gate electrode material, such a polysilicon. Preferably, the bottom of the V-shaped walls are rounded before the trench is filled. Source/drain impurities either are diffused or implanted into the areas of the substrate on both sides of the surface oxide of the V-shaped gate. Contacts are made to the source, drain, and gate within field isolation to complete the structure. The resultant FET structure comprises a self aligned V-shaped gate having conventional source and drain surrounded by field isolation but with an effective channel length (L.sub.eff) of less than about one-half of the surface width of the gate. Preferably, the converging walls of the V-shaped gate end in a rounded concave bottom. Because of the V-shaped structure of the gate, the effective saturated length of the channel with drain voltage applied only extends from the edge of the source to just prior to the tip of the V-shaped structure in the interior of the semiconductor substrate. The drain side of the V-shaped structure becomes a depletion region due to the applied drain voltage. Due to this characteristic of such a structure, the surface width of the gate can be, for example, two or more times the distance of the desired channel length thereby permitting conventional lithography to be used to define the gate lengths much shorter than the lithographic limit.
    • 在半导体衬底中形成具有V形壁的沟槽或沟槽栅极的场效应晶体管,并且在V形壁上生长栅极氧化物到衬底表面,并且填充有诸如多晶硅的栅电极材料。 优选地,在填充沟槽之前,V形壁的底部是圆形的。 源极/漏极杂质可以扩散或注入到V形栅极的表面氧化物两侧的衬底区域中。 触点在场隔离中被制成源极,漏极和栅极,以完成结构。 所得到的FET结构包括具有常规源极和漏极的自对准V形栅极,该源极和漏极被场隔离包围,但具有小于栅极表面宽度的约一半的有效沟道长度(Leff)。 优选地,V形门的会聚壁在圆形凹入的底部中。 由于栅极的V形结构,所以施加漏极电压的沟道的有效饱和长度仅从源极的边缘延伸到半导体衬底内部的V形结构的尖端之前。 V形结构的漏极侧由于施加的漏极电压而变为耗尽区。 由于这种结构的这种特性,栅极的表面宽度可以是例如期望沟道长度的两倍或更多倍的距离,从而允许常规光刻用于限定比光刻极限短的栅极长度 。