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    • 2. 发明授权
    • Bias plasma deposition for selective low dielectric insulation
    • 偏压等离子体沉积用于选择性低介电绝缘
    • US5990557A
    • 1999-11-23
    • US964430
    • 1997-11-04
    • Steven AvanzinoDarrell M. ErbRobin CheungRich KleinPervaiz Sultan
    • Steven AvanzinoDarrell M. ErbRobin CheungRich KleinPervaiz Sultan
    • H01L21/316H01L21/768H01L23/522H01L23/485
    • H01L21/02164H01L21/02203H01L21/02211H01L21/02274H01L21/02304H01L21/31612H01L21/7682H01L21/76837H01L23/5222H01L2924/0002
    • A method of forming low dielectric insulation between those pairs of conductive lines, of a level of interconnection for integrated circuits, having a gap of about 0.5 microns or less by depositing a nonconformal source with a poor step function for the insulating material, such as silane (SiH.sub.4) as the silicon (Si) source for silicon dioxide (SiO.sub.2), so as to create, in the gap, a large void whose dielectric constant is slightly greater than 1. After the formation of the void in the 0.5 microns or less gaps, the deposited nonconformal material is etched either simultaneously or sequentially along with deposition to fill the remaining gaps with void free insulation. The surface of the deposited insulating material is planarized at the desired thickness. Alternatively, a thin conformal insulating layer is first deposited as a liner on the conductive lines. The resulting structure of the interconnection level comprises a layer of insulation between and on the conductive lines with the dielectric constant of the insulation between the pairs of conductive lines with gap of 0.5 or less being, in combination with the void, at least about 3 or lower, and all of the remaining gaps are filled with void free insulating material with a dielectric constant of greater than about 3.5.
    • 在这些导电线对之间形成低介电绝缘的方法,该集成电路的互连级别通过沉积具有差的绝缘材料的步进功能的非共形源(例如硅烷)而具有约0.5微米或更小的间隙 (SiH4)作为二氧化硅(SiO 2)的硅(Si)源,以在间隙中产生介电常数略大于1的大空隙。在0.5微米或更小的空隙形成之后 间隙,沉积的非共形材料与沉积同时或顺序蚀刻,以用无空隙绝缘填充剩余的间隙。 沉积的绝缘材料的表面被平坦化为所需的厚度。 或者,首先在导电线上沉积薄的共形绝缘层作为衬垫。 所形成的互连级别的结构包括在导电线之间和之间的导电层之间的绝缘层,其中间隔为0.5或更小的导电线对之间的绝缘体的介电常数与空隙结合为至少约3或 较低,并且所有剩余的间隙都填充有绝缘材料,介电常数大于约3.5。
    • 3. 发明授权
    • Composite insulation with a dielectric constant of less than 3 in a
narrow space separating conductive lines
    • 在狭窄的空间分离导线的介电常数小于3的复合绝缘
    • US5691573A
    • 1997-11-25
    • US481030
    • 1995-06-07
    • Steven AvanzinoDarrell M. ErbRobin CheungRich Klein
    • Steven AvanzinoDarrell M. ErbRobin CheungRich Klein
    • H01L21/768H01L23/522H01L23/532H01L23/485H01L23/52
    • H01L23/5222H01L21/7682H01L23/5329H01L23/53295H01L2924/0002
    • A method of forming low dielectric insulation between those pairs of conductive lines, of a level of interconnection for integrated circuits, having a gap of about 0.5 microns or less by depositing a nonconformal source with a poor step function for the insulating material, such as silane (SiH.sub.4) as the silicon (Si) source for silicon dioxide (SiO.sub.2), so as to create, in the gap, a large void whose dielectric constant is slightly greater than 1. After all of the conductive lines have received a deposit of conformal insulating material and a flowable insulating material, the composite insulating materials are removed, preferably by etching, from those pairs of conductive lines with a gap of about 0.5 microns or less. Now, a nonconformal insulating material with a poor step function is deposited and creates a large void in the open gaps of 0.5 microns or less. After creating the void, the deposition continues and is planarized at the desired composite thickness of insulation. Alternatively, a thin conformal insulating layer is first deposited as a liner on the conductive lines. The resulting structure of the interconnection level comprises a layer of insulation between and on the conductive lines with the dielectric constant of the insulation between the pairs of conductive lines with the gap of 0.5 or less being, in combination with the void, at least about 3 or lower, and all of the remaining gaps are filled with the flowable insulating material and are void free with a composite dielectric constant of greater than about 3.5.
    • 在这些导电线对之间形成低介电绝缘的方法,该集成电路的互连级别具有约0.5微米或更小的间隙,通过沉积具有差的绝缘材料的步进功能的非共形源,例如硅烷 (SiH4)作为二氧化硅(SiO 2)的硅(Si)源,以在间隙中产生介电常数略大于1的大空隙。在所有导电线都已经接收到保形膜 绝缘材料和可流动的绝缘材料,优选通过蚀刻从具有约0.5微米或更小的间隙的那对导电线去除复合绝缘材料。 现在,沉积具有差的阶梯函数的非共形绝缘材料,并且在0.5微米或更小的开放间隙中产生大的空隙。 在形成空隙之后,沉积继续并且在所需的绝缘复合厚度下被平坦化。 或者,首先在导电线上沉积薄的共形绝缘层作为衬垫。 所得到的互连级别的结构包括在导电线之间和之间的导电层之间的绝缘层,导电线对之间的绝缘介电常数为0.5或更小的间隙,与空隙结合为至少约3 或更低,并且所有剩余间隙都填充有可流动绝缘材料,并且无复合介电常数大于约3.5。
    • 8. 发明授权
    • Selective electroplating with direct contact chemical polishing
    • 选择性电镀与直接接触化学抛光
    • US06454916B1
    • 2002-09-24
    • US09477810
    • 2000-01-05
    • Fei WangSteven C. AvanzinoDarrell M. Erb
    • Fei WangSteven C. AvanzinoDarrell M. Erb
    • C25D1700
    • C25D5/22B23H5/08C25D7/12C25D17/001
    • A deposition tool and a method for depositing a material within the recesses in a substrate of semiconductor wafer employs a rotatable diffuser that diffuses the plating material onto the top surface of a substrate. The diffuser is placed into contact with the semiconductor wafer and rotated while the plating material is applied through apertures in the diffuser. The plating material fills recesses patterned into the substrate of the semiconductor wafer but is prevented from forming to a significant degree on the top surface of the semiconductor wafer due to the contact and rotation of the diffuser. Since the plating material is not deposited on the top surface of the semiconductor wafer to any significant degree, chemical mechanical polishing (CMP) planarization is significantly reduced or completely eliminated.
    • 沉积工具和用于在半导体晶片的衬底内的凹槽内沉积材料的方法采用将电镀材料扩散到衬底顶表面上的可旋转漫射器。 扩散器被放置成与半导体晶片接触并且当电镀材料通过扩散器中的孔施加时旋转。 电镀材料填充图案化到半导体晶片的衬底中的凹槽,但是由于扩散器的接触和旋转,防止了在半导体晶片的顶表面上形成很大程度。 由于电镀材料没有以任何显着的程度沉积在半导体晶片的顶表面上,所以化学机械抛光(CMP)平面化被显着地减少或完全消除。
    • 10. 发明授权
    • High capacity semiconductor capacitance device structure
    • 大容量半导体电容器件结构
    • US4745454A
    • 1988-05-17
    • US926600
    • 1986-11-03
    • Darrell M. Erb
    • Darrell M. Erb
    • H01L21/8242H01L27/108H01L29/92H01L27/02H01L29/78
    • H01L27/1085H01L27/10805
    • The present invention provides for a method for manufacturing a charge storage region in a semiconductor substrate for a memory cell in a dynamic RAM, comprising forming an insulating layer on the substrate, forming a masking layer over the insulating layer, forming at least one aperture in the masking layer, the aperture defining the charge storage region in the semiconductor substrate, implanting dopant ions of a first polarity through the aperture for diffusion through the substrate, and implanting dopant ions of a second polarity through the aperture for diffusion through the substrate to a lesser degree than the first polarity dopant diffusion so that the diffusion of the first polarity dopant with respect to the diffusion of the second polarity dopant forms a P-N junction substantially aligned with the edge of the masking layer aperture to define the periphery of the charge storage region. One way of diffusing the second polarity dopant to a lesser degree than the first polarity dopant in the substrate is to select a first polarity dopant which has a diffusivity greater than the second polarity dopant. Another way of achieving the desired diffusion of first polarity dopant with respect to the second polarity dopant is to select the two dopants with diffusivities approximately equal and to diffuse the first polarity dopant before the second polarity dopants is implanted into the semiconductor substrate.
    • 本发明提供一种在动态RAM中用于存储单元的半导体衬底中的电荷存储区域的制造方法,包括在衬底上形成绝缘层,在绝缘层上形成掩模层,形成至少一个孔 掩模层,限定半导体衬底中的电荷存储区域的孔,通过孔径注入第一极性的掺杂离子以通过衬底扩散,以及通过孔径注入第二极性的掺杂剂离子,以通过衬底扩散到 比第一极性掺杂剂扩散程度小,使得第一极性掺杂剂相对于第二极性掺杂剂的扩散的扩散形成基本上与掩模层孔的边缘对准的PN结,以限定电荷存储区域的周边 。 将第二极性掺杂剂扩散到比衬底中的第一极性掺杂剂更小程度的一种方法是选择具有大于第二极性掺杂剂的扩散率的第一极性掺杂剂。 实现第一极性掺杂剂相对于第二极性掺杂剂的期望扩散的另一种方法是选择具有大致相等的扩散率的两种掺杂剂,并且在将第二极性掺杂剂注入到半导体衬底之前扩散第一极性掺杂剂。