High voltage field effect device and method
    1.
    发明授权
    High voltage field effect device and method 有权
    高电压场效应装置及方法

    公开(公告)号:US07301187B2

    公开(公告)日:2007-11-27

    申请号:US11689313

    申请日:2007-03-21

    摘要: Methods and apparatus are provided for a MOSFET (50, 99, 199) exhibiting increased source-drain breakdown voltage (BVdss). Source (S) (70) and drain (D) (76) are spaced apart by a channel (90) underlying a gate (84) and one or more carrier drift spaces (92, 92′) serially located between the channel (90) and the source (70, 70′) or drain (76, 76′). A buried region (96, 96′) of the same conductivity type as the drift space (92, 92′) and the source (70, 70′) or drain (76, 76′) is provided below the drift space (92, 92′), separated therefrom in depth by a narrow gap (94, 94′) and ohmically coupled to the source (70, 70′) or drain (76, 76′). Current flow (110) through the drift space produces a potential difference (Vt) across this gap (94, 94′). As the S-D voltage (Vo) and current (109, Io) increase, this difference (Vt) induces high field conduction between the drift space (92, 92′) and the buried region (96, 96′) and diverts part (112, It) of the S-D current (109, Io) through the buried region (96, 96′) and away from the near surface portions of the drift space (92, 92′) where breakdown generally occurs. Thus, BVdss is increased.

    摘要翻译: 为具有增加的源 - 漏击穿电压(BVdss)的MOSFET(50,99,199)提供了方法和装置。 源极(S)(70)和漏极(D)(76)通过栅极(84)下面的沟道(90)和串联地位于沟道(90)之间的一个或多个载流子漂移空间(92,92')间隔开 )和源极(70,70')或漏极(76,76')。 与漂移空间(92,92')和源极(70,70')或漏极(76,76')相同的导电类型的掩埋区域(96,96')设置在漂移空间(92,92')的下方, 92'),通过狭窄的间隙(94,94')深度地分离,并且与欧姆耦合到源极(70,70')或漏极(76,76')。 穿过漂移空间的电流(110)在该间隙(94,94')上产生电位差(Vt)。 随着SD电压(Vo)和电流(109,Io)的增加,该差值(Vt)引起漂移空间(92,92')和掩埋区域(96,96')之间的高场导通,并且转移部分 ,It)通过掩埋区域(96,96')并远离漂移空间(92,92')的通常发生击穿的漂移空间(92,92')的近表面部分的SD电流(109,Io)。 因此,BVdss增加。

    Bipolar junction transistor structure with improved current gain characteristics
    3.
    发明授权
    Bipolar junction transistor structure with improved current gain characteristics 有权
    具有改善的电流增益特性的双极结晶体管结构

    公开(公告)号:US06828650B2

    公开(公告)日:2004-12-07

    申请号:US10160940

    申请日:2002-05-31

    IPC分类号: H01L2900

    摘要: A Bipolar Junction Transistor (BJT) that reduces the variation in the current gain through the use of a trench pullback structure. The trench pullback structure is comprised of a trench and an active region. The trench reduces recombination in the emitter-base region through increasing the distance charge carriers must travel between the emitter and the base. The trench also reduces recombination by reducing the amount of interfacial traps that the electrons injected from the emitter are exposed to. Further, the trench is pulled back from the emitter allowing an active region where electrons injected from a sidewall of the emitter can contribute to the overall injected emitter current. This structure offers the same current capability and current gain as a device without the trench between the emitter and the base while reducing the current gain variation.

    摘要翻译: 双极结晶体管(BJT),通过使用沟槽回拉结构减少电流增益的变化。 沟槽回拉结构由沟槽和有源区组成。 沟槽通过增加载流子必须在发射极和基极之间行进的距离来减小发射极 - 基极区域中的复合。 沟槽还通过减少从发射体注入的电子暴露的界面陷阱的量来减少重组。 此外,从发射极拉回沟槽,允许从发射极的侧壁注入的电子能够有助于整个注入的发射极电流的有源区。 该结构提供与发射极和基极之间没有沟槽的器件相同的电流能力和电流增益,同时减小电流增益变化。

    Carrier injection protection structure
    4.
    发明授权
    Carrier injection protection structure 有权
    载体注入保护结构

    公开(公告)号:US06787858B2

    公开(公告)日:2004-09-07

    申请号:US10272336

    申请日:2002-10-16

    IPC分类号: H01L2994

    摘要: A structure protects CMOS logic from substrate minority carrier injection caused by the inductive switching of a power device. A single Integrated Circuit (IC) supports one or more power MOSFETs and one or more arrays of CMOS logic. A highly doped ring is formed between the drain of the power MOSFET and the CMOS logic array to provide a low resistance path to ground for the injected minority carriers. Under the CMOS logic is a highly doped buried layer to form a region of high recombination for the injected minority carriers. One or more CMOS devices are formed above the buried layer. The substrate is a resistive and the injected current is attenuated. The well in which the CMOS devices rest forms a low resistance ground plane for the injected minority carriers.

    摘要翻译: 结构保护CMOS逻辑免受由功率器件的感应开关引起的衬底少数载流子注入。 单个集成电路(IC)支持一个或多个功率MOSFET和一个或多个CMOS逻辑阵列。 在功率MOSFET的漏极和CMOS逻辑阵列之间形成高度掺杂的环,以为注入的少数载流子提供低电阻的接地路径。 在CMOS逻辑下是高掺杂掩埋层,以形成注入的少数载流子的高复合区域。 一个或多个CMOS器件形成在掩埋层上方。 衬底是电阻的,并且注入的电流被衰减。 CMOS器件休息的阱为注入的少数载流子形成低电阻接地层。

    High voltage field effect device and method
    5.
    发明申请
    High voltage field effect device and method 有权
    高电压场效应装置及方法

    公开(公告)号:US20060249751A1

    公开(公告)日:2006-11-09

    申请号:US11124469

    申请日:2005-05-06

    IPC分类号: H01L31/00

    摘要: Methods and apparatus are provided for a MOSFET (50, 99, 199) exhibiting increased source-drain breakdown voltage (BVdss). Source (S) (70) and drain (D) (76) are spaced apart by a channel (90) underlying a gate (84) and one or more carrier drift spaces (92, 92′) serially located between the channel (90) and the source (70, 70′) or drain (76, 76′). A buried region (96, 96′) of the same conductivity type as the drift space (92, 92′) and the source (70, 70′) or drain (76, 76′) is provided below the drift space (92, 92′), separated therefrom in depth by a narrow gap (94, 94′) and ohmically coupled to the source (70, 70′) or drain (76, 76′). Current flow (110) through the drift space produces a potential difference (Vt) across this gap (94, 94′). As the S-D voltage (Vo) and current (109, Io) increase, this difference (Vt) induces high field conduction between the drift space (92, 92′) and the buried region (96, 96′) and diverts part (112, It) of the S-D current (109, Io) through the buried region (96, 96′) and away from the near surface portions of the drift space (92, 92′) where breakdown generally occurs. Thus, BVdss is increased.

    摘要翻译: 为具有增加的源 - 漏击穿电压(BVdss)的MOSFET(50,99,199)提供了方法和装置。 源极(S)(70)和漏极(D)(76)通过栅极(84)下面的沟道(90)和串联地位于沟道(90)之间的一个或多个载流子漂移空间(92,92')间隔开 )和源极(70,70')或漏极(76,76')。 与漂移空间(92,92')和源极(70,70')或漏极(76,76')相同的导电类型的掩埋区域(96,96')设置在漂移空间(92,92')的下方, 92'),通过狭窄的间隙(94,94')深度地分离,并且与欧姆耦合到源极(70,70')或漏极(76,76')。 穿过漂移空间的电流(110)在该间隙(94,94')上产生电位差(Vt)。 随着SD电压(Vo)和电流(109,Io)的增加,该差值(Vt)引起漂移空间(92,92')和掩埋区域(96,96')之间的高场导通,并且转移部分 ,It)通过掩埋区域(96,96')并远离漂移空间(92,92')的通常发生击穿的漂移空间(92,92')的近表面部分的SD电流(109,Io)。 因此,BVdss增加。

    HIGH VOLTAGE FIELD EFFECT DEVICE AND METHOD
    6.
    发明申请
    HIGH VOLTAGE FIELD EFFECT DEVICE AND METHOD 有权
    高电压场效应器件及方法

    公开(公告)号:US20070158777A1

    公开(公告)日:2007-07-12

    申请号:US11689313

    申请日:2007-03-21

    IPC分类号: H01L23/58 H01L21/336

    摘要: Methods and apparatus are provided for a MOSFET (50, 99, 199) exhibiting increased source-drain breakdown voltage (BVdss). Source (S) (70) and drain (D) (76) are spaced apart by a channel (90) underlying a gate (84) and one or more carrier drift spaces (92, 92′) serially located between the channel (90) and the source (70, 70′) or drain (76, 76′). A buried region (96, 96′) of the same conductivity type as the drift space (92, 92′) and the source (70, 70′) or drain (76, 76′) is provided below the drift space (92, 92′), separated therefrom in depth by a narrow gap (94, 94′) and ohmically coupled to the source (70, 70′) or drain (76, 76′). Current flow (110) through the drift space produces a potential difference (Vt) across this gap (94, 94′). As the S-D voltage (Vo) and current (109, Io) increase, this difference (Vt) induces high field conduction between the drift space (92, 92′) and the buried region (96, 96′) and diverts part (112, It) of the S-D current (109, Io) through the buried region (96, 96′) and away from the near surface portions of the drift space (92, 92′) where breakdown generally occurs. Thus, BVdss is increased.

    摘要翻译: 为具有增加的源 - 漏击穿电压(BVdss)的MOSFET(50,99,199)提供了方法和装置。 源极(S)(70)和漏极(D)(76)通过栅极(84)下面的沟道(90)和串联地位于沟道(90)之间的一个或多个载流子漂移空间(92,92')间隔开 )和源极(70,70')或漏极(76,76')。 与漂移空间(92,92')和源极(70,70')或漏极(76,76')相同的导电类型的掩埋区域(96,96')设置在漂移空间(92,92')的下方, 92'),通过狭窄的间隙(94,94')深度地分离,并且与欧姆耦合到源极(70,70')或漏极(76,76')。 穿过漂移空间的电流(110)在该间隙(94,94')上产生电位差(Vt)。 随着SD电压(Vo)和电流(109,Io)的增加,该差值(Vt)引起漂移空间(92,92')和掩埋区域(96,96')之间的高场导通,并且转移部分 ,It)通过掩埋区域(96,96')并远离漂移空间(92,92')的通常发生击穿的漂移空间(92,92')的近表面部分的SD电流(109,Io)。 因此,BVdss增加。

    Schottky diode with leakage current control structures
    7.
    发明授权
    Schottky diode with leakage current control structures 有权
    具有漏电流控制结构的肖特基二极管

    公开(公告)号:US09231120B2

    公开(公告)日:2016-01-05

    申请号:US13537299

    申请日:2012-06-29

    摘要: A Schottky diode includes a device structure having a central portion and a plurality of fingers. Distal portions of the fingers overlie leakage current control (LCC) regions. An LCC region is relatively narrow and deep, terminating in proximity to a buried layer of like polarity. Under reverse bias, depletion regions forming in an active region lying between the buried layer and the LCC regions occupy the entire extent of the active region and thereby provide a carrier depleted wall. An analogous depletion region occurs in the active region residing between any pair of adjacent fingers. If the fingers include latitudinal oriented fingers and longitudinal oriented fingers, depletion region blockades in three different orthogonal orientations may occur. The formation of the LCC regions may include the use of a high dose, low energy phosphorous implant using an LCC implant mask and the isolation structures as an additional hard mask.

    摘要翻译: 肖特基二极管包括具有中心部分和多个指状物的器件结构。 手指的远端覆盖泄漏电流控制(LCC)区域。 LCC区域相对较窄和深,终止于类似极性的掩埋层附近。 在反向偏压下,在位于掩埋层和LCC区域之间的有源区域中形成的耗尽区域占据有源区域的整个范围,从而提供载流子耗尽的壁。 类似的耗尽区发生在驻留在任何一对相邻手指之间的有源区域中。 如果手指包括纬向取向的指状物和纵向取向的指状物,则可能发生三个不同正交取向的耗尽区域封锁。 LCC区域的形成可以包括使用使用LCC植入物掩模的高剂量,低能量磷植入物以及作为附加硬掩模的隔离结构。

    Tunable schottky diode with depleted conduction path
    8.
    发明授权
    Tunable schottky diode with depleted conduction path 有权
    可调肖特基二极管具有耗尽的导通路径

    公开(公告)号:US08735950B2

    公开(公告)日:2014-05-27

    申请号:US13605357

    申请日:2012-09-06

    IPC分类号: H01L29/66

    摘要: A device includes a semiconductor substrate, first and second electrodes supported by the semiconductor substrate, laterally spaced from one another, and disposed at a surface of the semiconductor substrate to form an Ohmic contact and a Schottky junction, respectively. The device further includes a conduction path region in the semiconductor substrate, having a first conductivity type, and disposed along a conduction path between the first and second electrodes, a buried region in the semiconductor substrate having a second conductivity type and disposed below the conduction path region, and a device isolating region electrically coupled to the buried region, having the second conductivity type, and defining a lateral boundary of the device. The device isolating region is electrically coupled to the second electrode such that a voltage at the second electrode during operation is applied to the buried region to deplete the conduction path region.

    摘要翻译: 一种器件包括半导体衬底,由半导体衬底支撑的第一和第二电极,彼此横向间隔开,并分别设置在半导体衬底的表面以形成欧姆接触和肖特基结。 该器件还包括半导体衬底中的导电通路区域,具有第一导电类型,并且沿第一和第二电极之间的导电路径设置,半导体衬底中的具有第二导电类型并设置在导电路径下方的掩埋区域 以及电耦合到所述掩埋区域的器件隔离区域,具有所述第二导电类型,并且限定所述器件的横向边界。 器件隔离区域电耦合到第二电极,使得在操作期间第二电极处的电压被施加到掩埋区域以耗尽导电路径区域。

    Single poly NVM devices and arrays
    9.
    发明授权
    Single poly NVM devices and arrays 有权
    单一的NV NV设备和阵列

    公开(公告)号:US08344443B2

    公开(公告)日:2013-01-01

    申请号:US12109736

    申请日:2008-04-25

    摘要: A single-poly non-volatile memory includes a PMOS select transistor (210) formed with a select gate (212), and P+ source and drain regions (211, 213) formed in a shared n-well region (240), a serially connected PMOS floating gate transistor (220) formed with part of a p-type floating gate layer (222) and P+ source and drain regions (221, 223) formed in the shared n-well region (240), and a coupling capacitor (230) formed over a p-well region (250) and connected to the PMOS floating gate transistor (220), where the coupling capacitor (230) includes a first capacitor plate formed with a second part of the p-type floating gate layer (222) and an underlying portion of the p-well region (250).

    摘要翻译: 单多晶非易失性存储器包括形成有选择栅极(212)的PMOS选择晶体管(210),以及形成在共享的n阱区域(240)中的P +源区和漏区(211,213) 形成有形成在共用n阱区域(240)中的p型浮栅(222)和P +源区和漏区(221,223)的一部分的连接PMOS浮栅晶体管(220)和耦合电容器 230),其形成在p阱区(250)上并连接到PMOS浮栅晶体管(220),其中耦合电容器(230)包括形成有p型浮栅的第二部分的第一电容器板( 222)和p阱区(250)的下层部分。