[go: up one dir, main page]

CN104465735B - Embedded gate insulation tunnelling enhancing transistor - Google Patents

Embedded gate insulation tunnelling enhancing transistor Download PDF

Info

Publication number
CN104465735B
CN104465735B CN201410742827.XA CN201410742827A CN104465735B CN 104465735 B CN104465735 B CN 104465735B CN 201410742827 A CN201410742827 A CN 201410742827A CN 104465735 B CN104465735 B CN 104465735B
Authority
CN
China
Prior art keywords
tunneling
base
gate
insulating layer
embedded
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Expired - Fee Related
Application number
CN201410742827.XA
Other languages
Chinese (zh)
Other versions
CN104465735A (en
Inventor
靳晓诗
刘溪
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Shenyang University of Technology
Original Assignee
Shenyang University of Technology
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Shenyang University of Technology filed Critical Shenyang University of Technology
Priority to CN201410742827.XA priority Critical patent/CN104465735B/en
Publication of CN104465735A publication Critical patent/CN104465735A/en
Application granted granted Critical
Publication of CN104465735B publication Critical patent/CN104465735B/en
Expired - Fee Related legal-status Critical Current
Anticipated expiration legal-status Critical

Links

Classifications

    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D12/00Bipolar devices controlled by the field effect, e.g. insulated-gate bipolar transistors [IGBT]
    • HELECTRICITY
    • H01ELECTRIC ELEMENTS
    • H01LSEMICONDUCTOR DEVICES NOT COVERED BY CLASS H10
    • H01L21/00Processes or apparatus adapted for the manufacture or treatment of semiconductor or solid state devices or of parts thereof
    • H01L21/02Manufacture or treatment of semiconductor devices or of parts thereof
    • H01L21/04Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer
    • H01L21/18Manufacture or treatment of semiconductor devices or of parts thereof the devices having potential barriers, e.g. a PN junction, depletion layer or carrier concentration layer the devices having semiconductor bodies comprising elements of Group IV of the Periodic Table or AIIIBV compounds with or without impurities, e.g. doping materials
    • H01L21/28Manufacture of electrodes on semiconductor bodies using processes or apparatus not provided for in groups H01L21/20 - H01L21/268
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D48/00Individual devices not covered by groups H10D1/00 - H10D44/00
    • H10D48/01Manufacture or treatment
    • H10D48/031Manufacture or treatment of three-or-more electrode devices
    • H10D48/032Manufacture or treatment of three-or-more electrode devices of unipolar transistors having ohmic electrodes on emitter-like, base-like, and collector-like regions, e.g. hot electron transistors [HET], metal base transistors [MBT], resonant tunneling transistors [RTT], bulk barrier transistors [BBT], planar doped barrier transistors [PDBT] or charge injection transistors [CHINT]
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D62/00Semiconductor bodies, or regions thereof, of devices having potential barriers
    • H10D62/10Shapes, relative sizes or dispositions of the regions of the semiconductor bodies; Shapes of the semiconductor bodies
    • H10D62/124Shapes, relative sizes or dispositions of the regions of semiconductor bodies or of junctions between the regions
    • HELECTRICITY
    • H10SEMICONDUCTOR DEVICES; ELECTRIC SOLID-STATE DEVICES NOT OTHERWISE PROVIDED FOR
    • H10DINORGANIC ELECTRIC SEMICONDUCTOR DEVICES
    • H10D64/00Electrodes of devices having potential barriers
    • H10D64/20Electrodes characterised by their shapes, relative sizes or dispositions 
    • H10D64/27Electrodes not carrying the current to be rectified, amplified, oscillated or switched, e.g. gates
    • H10D64/311Gate electrodes for field-effect devices
    • H10D64/411Gate electrodes for field-effect devices for FETs
    • H10D64/511Gate electrodes for field-effect devices for FETs for IGFETs
    • H10D64/512Disposition of the gate electrodes, e.g. buried gates
    • H10D64/513Disposition of the gate electrodes, e.g. buried gates within recesses in the substrate, e.g. trench gates, groove gates or buried gates

Landscapes

  • Engineering & Computer Science (AREA)
  • Physics & Mathematics (AREA)
  • Condensed Matter Physics & Semiconductors (AREA)
  • General Physics & Mathematics (AREA)
  • Manufacturing & Machinery (AREA)
  • Computer Hardware Design (AREA)
  • Microelectronics & Electronic Packaging (AREA)
  • Power Engineering (AREA)
  • Thin Film Transistor (AREA)
  • Bipolar Transistors (AREA)

Abstract

本发明涉及一种高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,对比同尺寸MOSFETs或TFETs,利用隧穿绝缘层阻抗与隧穿绝缘层内电场强度之间极为敏感的相互关系实现更好的转移特性;避免了由于栅电极和漏电极之间或栅电极和源电极之间的距离不断缩小而导致的栅源、源栅、栅漏以及漏栅之间寄生电容的明显增大,使器件在保证高转移特性的同时明显降低寄生电容;且由于不存在MOSFETs或TFETs所具有的栅极至漏极重叠区,因此不会引发明显的反向泄漏电流。本发明还提出了一种高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管的具体制造方法。该晶体管显著改善了纳米级集成电路单元的工作特性,适用于推广应用。

The invention relates to a high-transfer characteristic and low parasitic capacitance built-in gate insulation tunneling enhanced transistor. Compared with MOSFETs or TFETs of the same size, the extremely sensitive relationship between the impedance of the tunneling insulating layer and the electric field intensity in the tunneling insulating layer is used to realize a more sensitive relationship. Good transfer characteristics; avoiding the obvious increase of parasitic capacitance between gate-source, source-gate, gate-drain and drain-gate due to the shrinking distance between gate electrode and drain electrode or between gate electrode and source electrode, making The device significantly reduces parasitic capacitance while ensuring high transfer characteristics; and since there is no gate-to-drain overlap region that MOSFETs or TFETs have, it does not cause significant reverse leakage current. The invention also proposes a specific manufacturing method of an embedded gate insulation tunneling enhancement transistor with high transfer characteristics and low parasitic capacitance. The transistor significantly improves the working characteristics of the nanoscale integrated circuit unit and is suitable for popularization and application.

Description

内嵌栅绝缘隧穿增强晶体管Embedded Gate Insulated Tunneling Enhancement Transistor

技术领域:Technical field:

本发明涉及超大规模集成电路制造领域,涉及一种适用于高性能超高集成度集成电路制造的高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管。The invention relates to the field of ultra-large-scale integrated circuit manufacturing, and relates to an embedded gate insulation tunneling enhanced transistor with high transfer characteristics and low parasitic capacitance, which is suitable for the manufacture of high-performance ultra-high integrated integrated circuits.

背景技术:Background technique:

当前,集成电路单元金属氧化物半导体场效应晶体管(MOSFETs)器件沟道长度的不断缩短导致了器件转移特性的下降。亚阈值摆幅随着沟道长度的减小而增大,静态功耗明显增加。虽然通过改善栅电极结构的方式可使这种器件性能的退化有所缓解,但当器件尺寸进一步缩减时,器件的转移特性会重新恶化。Currently, the ever-shortening device channel lengths of integrated circuit unit metal-oxide-semiconductor field-effect transistors (MOSFETs) have resulted in degraded device transfer characteristics. The subthreshold swing increases with decreasing channel length, and the static power consumption increases significantly. Although the degradation of the device performance can be alleviated by improving the structure of the gate electrode, when the device size is further reduced, the transfer characteristics of the device will deteriorate again.

另一方面,随着器件尺寸的不断减小,漏电极与栅电极之间的距离、或源电极与栅电极之间的距离也随之不断减小,这就使得器件的栅源、源栅、栅漏以及漏栅寄生电容显著增大,使集成电路的功耗增大,使信号的传播时延及负反馈增大,并影响增益带宽乘积。On the other hand, with the continuous reduction of device size, the distance between the drain electrode and the gate electrode, or the distance between the source electrode and the gate electrode is also continuously reduced, which makes the gate-source, source-gate of the device , Gate-to-drain and drain-gate parasitic capacitance increases significantly, which increases the power consumption of the integrated circuit, increases the signal propagation delay and negative feedback, and affects the gain-bandwidth product.

隧穿场效应晶体管(TFETs),对比于MOSFETs器件的转移特性,虽然其平均亚阈值摆幅有所提升,然而其正向导通电流过小,且由于尺寸缩小所产生的寄生电容,对比MOSFETs并无改善。Tunneling Field Effect Transistors (TFETs), compared with the transfer characteristics of MOSFETs, although its average subthreshold swing has been improved, but its forward conduction current is too small, and the parasitic capacitance generated due to size reduction, compared with MOSFETs and No improvement.

通过引入化合物半导体、锗化硅或锗等禁带宽度更窄的材料来生成为TFETs的隧穿部分,可增大隧穿几率以提升转移特性,然而增大了生产成本,也增加了工艺难度。此外,采用高介电常数绝缘材料作为栅极与衬底之间的绝缘介质层,虽然能够改善栅极对沟道电场分布的控制能力,却不能从本质上提高硅材料的隧穿几率,因此对于TFETs的转移特性改善很有限。The tunneling part of TFETs can be generated by introducing materials with narrower band gaps such as compound semiconductors, silicon germanium or germanium, which can increase the tunneling probability and improve the transfer characteristics, but increases the production cost and process difficulty. In addition, the use of high dielectric constant insulating material as the insulating dielectric layer between the gate and the substrate can improve the control ability of the gate to the electric field distribution of the channel, but it cannot substantially increase the tunneling probability of the silicon material, so There is limited improvement in the transfer characteristics of TFETs.

此外,由于TFETs和MOSFETs器件都是通过栅电极电场效应对栅极绝缘层及半导体内部的电场、电势及载流子分布进行控制,为了提升栅电极对半导体内部的控制能力,需采用高介电常数和不断减薄的栅极绝缘层来加强栅电极的控制能力,但同时也缩短了栅电极和漏区、栅电极和源区之间的距离,使得栅极和漏极重合区域处在栅极反向偏置时会产生较大的栅极致漏极泄漏(GIDL)电流或栅极致源极泄漏(GISL)电流。In addition, since both TFETs and MOSFETs control the electric field, potential and carrier distribution inside the gate insulating layer and semiconductor through the electric field effect of the gate electrode, in order to improve the control ability of the gate electrode to the inside of the semiconductor, high dielectric The constant and thinning gate insulating layer strengthens the control ability of the gate electrode, but at the same time shortens the distance between the gate electrode and the drain region, the gate electrode and the source region, so that the overlapping area of the gate electrode and the drain electrode is at the gate electrode Larger gate-induced-drain leakage (GIDL) or gate-induced-source leakage (GISL) currents are generated when the polarity is reverse-biased.

发明内容:Invention content:

发明目的purpose of invention

为在兼容现有基于硅工艺技术的前提下显著提升纳米级集成电路基本单元器件的转移特性,确保器件在降低亚阈值摆幅的同时具有良好的正向电流导通特性,彻底解决由于器件尺寸不断缩小所导致的寄生电容明显增大的问题,并显著降低器件的反向泄漏电流,本发明提供一种适用于高性能、高集成度集成电路制造的高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管。In order to significantly improve the transfer characteristics of nanoscale integrated circuit basic unit devices on the premise of being compatible with existing silicon-based process technologies, ensure that the devices have good forward current conduction characteristics while reducing sub-threshold swings, and completely solve the problem of device size The problem of significantly increasing parasitic capacitance caused by continuous shrinkage, and significantly reducing the reverse leakage current of the device, the present invention provides a high-transfer characteristic and low parasitic capacitance embedded gate insulation suitable for high-performance, high-integration integrated circuit manufacturing Tunneling enhancement transistor.

技术方案Technical solutions

本发明是通过以下技术方案来实现的:The present invention is achieved through the following technical solutions:

内嵌栅绝缘隧穿增强晶体管,采用只包含单晶硅衬底1的体硅晶圆作为生成器件衬底,或采用同时包含单晶硅衬底1和晶圆绝缘层2的SOI晶圆作为生成器件的衬底;发射区3、基区4和集电区5位于体硅晶圆的单晶硅衬底1或SOI晶圆的晶圆绝缘层2的上方;发射极9位于发射区3的上方;集电极10位于集电区5的上方;导电层6内嵌于基区4内,并被基区4三面包围;隧穿绝缘层7内嵌于导电层6内,并被导电层6)三面包围;栅电极8内嵌于隧穿绝缘层7内,并被隧穿绝缘层7三面包围;阻挡绝缘层11位于器件单元之间和各电极之间,对各器件单元之间和各电极之间起隔离作用。For the embedded gate insulation tunneling enhanced transistor, a bulk silicon wafer containing only a single crystal silicon substrate 1 is used as a device substrate, or an SOI wafer containing both a single crystal silicon substrate 1 and a wafer insulating layer 2 is used as a The substrate for generating the device; the emitter region 3, the base region 4 and the collector region 5 are located above the monocrystalline silicon substrate 1 of the bulk silicon wafer or the wafer insulating layer 2 of the SOI wafer; the emitter 9 is located in the emitter region 3 above; the collector 10 is located above the collector region 5; the conductive layer 6 is embedded in the base region 4 and surrounded by three sides of the base region 4; the tunnel insulating layer 7 is embedded in the conductive layer 6 and is surrounded by the conductive layer 6) Surrounded on three sides; the gate electrode 8 is embedded in the tunneling insulating layer 7, and is surrounded by the tunneling insulating layer 7 on three sides; the blocking insulating layer 11 is located between the device units and between the electrodes, for each device unit and Between the electrodes play a role in isolation.

发射极9与集电极10之间通过阻挡绝缘层11隔离;发射区3与集电区5之间通过阻挡绝缘层11隔离。The emitter 9 and the collector 10 are isolated by a blocking insulating layer 11 ; the emitter region 3 and the collector region 5 are isolated by a blocking insulating layer 11 .

为达到本发明所述的器件功能,本发明提出高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,其核心结构特征为:In order to achieve the device functions described in the present invention, the present invention proposes a high transfer characteristic and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, and its core structural features are:

栅电极8、隧穿绝缘层7和导电层6均内嵌于基区4内,只有上表面与阻挡绝缘层11接触。The gate electrode 8 , the tunneling insulating layer 7 and the conductive layer 6 are all embedded in the base region 4 , and only the upper surface is in contact with the blocking insulating layer 11 .

栅电极8与发射区3之间依次夹有隧穿绝缘层7、导电层6和基区4;A tunnel insulating layer 7, a conductive layer 6 and a base region 4 are sequentially interposed between the gate electrode 8 and the emitter region 3;

栅电极8与集电区4之间依次夹有隧穿绝缘层7、导电层6和基区4;A tunnel insulating layer 7, a conductive layer 6 and a base region 4 are sequentially sandwiched between the gate electrode 8 and the collector region 4;

栅电极8是控制隧穿绝缘层7产生隧穿效应的电极,是控制器件开启和关断的电极。The gate electrode 8 is an electrode for controlling the tunneling effect generated by the tunneling insulating layer 7, and is an electrode for controlling the turning on and off of the device.

隧穿绝缘层7为用于产生栅绝缘层隧穿电流的绝缘层。The tunneling insulating layer 7 is an insulating layer for generating gate insulating layer tunneling current.

导电层6与基区4形成欧姆接触,是金属材料,或者是同基区4具有相同杂质类型的、且掺杂浓度大于1018每立方厘米的半导体材料。The conductive layer 6 forms an ohmic contact with the base region 4 and is a metal material, or a semiconductor material having the same impurity type as the base region 4 and a doping concentration greater than 10 18 per cubic centimeter.

发射区3与基区4之间、集电区5与基区4之间具有相反杂质类型、且发射区3与发射极9之间形成欧姆接触、集电区3与集电极10之间形成欧姆接触。There are opposite impurity types between the emitter region 3 and the base region 4, between the collector region 5 and the base region 4, and an ohmic contact is formed between the emitter region 3 and the emitter electrode 9, and an ohmic contact is formed between the collector region 3 and the collector electrode 10. ohmic contact.

内嵌栅绝缘隧穿增强晶体管,以N型为例,发射区3、基区4和集电区5分别为N区、P区和N区,其具体的工作原理为:当集电极10正偏,且栅电极8处于低电位时,栅电极8与导电层6之间没有形成足够的电势差,此时隧穿绝缘层7处于高阻状态,没有明显隧穿电流通过,因此使得基区4和发射区3之间无法形成足够大的基区电流来驱动高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,即器件处于关断状态;随着栅电极8电压的逐渐升高,栅电极8与导电层6之间的电势差逐渐增大,使得位于栅电极8与导电层6之间隧穿绝缘层7内的电场强度也随之逐渐增大,当隧穿绝缘层7内的电场强度位于临界值以下时,隧穿绝缘层7依然保持良好的高阻状态,栅电极和发射极之间的电势差几乎完全降在隧穿绝缘层7的内壁和外壁两侧之间,也就使得基区和发射区之间的电势差极小,因此基区几乎没有电流流过,器件也因此保持良好的关断状态,而当隧穿绝缘层7内的电场强度位于临界值以上时,隧穿绝缘层7会由于隧穿效应而产生明显的隧穿电流,并且隧穿电流则会随着栅电极8电势的增大以极快的速度陡峭上升,这就使得隧穿绝缘层7在栅电极极短的电势变化区间内由高阻态迅速转换为低阻态,当隧穿绝缘层7处于低阻态,此时隧穿绝缘层7在栅电极8和导电层6之间所形成的电阻要远小于导电层6和发射极3之间所形成的电阻,这就使得基区4和发射区3之间形成了足够大的正偏电压,并且在隧穿效应的作用下,在隧穿绝缘层7的内壁和外壁之间产生大量电子移动,即为基区4提供电流源,基区4电流经发射区3增强后由集电极流出,此时器件处于开启状态;Embedded gate insulation tunneling enhancement transistor, taking N type as an example, emitter region 3, base region 4 and collector region 5 are N region, P region and N region respectively, and its specific working principle is: when the collector electrode 10 is positive When the gate electrode 8 is at a low potential, there is not enough potential difference formed between the gate electrode 8 and the conductive layer 6. At this time, the tunneling insulating layer 7 is in a high-resistance state, and no obvious tunneling current passes through, so that the base region 4 A large enough base current cannot be formed between the emitter region 3 and the embedded gate insulation tunneling enhancement transistor with high transfer characteristics and low parasitic capacitance, that is, the device is in an off state; as the voltage of the gate electrode 8 gradually increases, the gate The potential difference between the electrode 8 and the conductive layer 6 gradually increases, so that the electric field intensity in the tunneling insulating layer 7 between the gate electrode 8 and the conductive layer 6 also gradually increases. When the electric field in the tunneling insulating layer 7 When the strength is below the critical value, the tunneling insulating layer 7 still maintains a good high-resistance state, and the potential difference between the gate electrode and the emitter is almost completely dropped between the inner wall and the outer wall of the tunneling insulating layer 7, which makes The potential difference between the base region and the emitter region is extremely small, so there is almost no current flowing in the base region, and the device remains in a good off state. When the electric field strength in the tunneling insulating layer 7 is above the critical value, the tunneling The insulating layer 7 will generate obvious tunneling current due to the tunneling effect, and the tunneling current will rise steeply at a very fast speed with the increase of the potential of the gate electrode 8, which makes the tunneling insulating layer 7 The high-resistance state is rapidly converted to a low-resistance state within a very short potential change interval. When the tunneling insulating layer 7 is in a low-resistance state, the resistance formed by the tunneling insulating layer 7 between the gate electrode 8 and the conductive layer 6 is It should be much smaller than the resistance formed between the conductive layer 6 and the emitter 3, which makes a sufficiently large forward bias voltage formed between the base region 4 and the emitter region 3, and under the action of the tunneling effect, the tunneling A large amount of electron movement is generated between the inner wall and the outer wall of the insulating layer 7, which provides a current source for the base region 4, and the current of the base region 4 flows out from the collector after being enhanced by the emitter region 3, and the device is in an open state at this time;

优点及效果Advantages and effects

本发明具有如下优点及有益效果:The present invention has following advantage and beneficial effect:

1.高转移特性1. High transfer characteristics

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,利用隧穿绝缘层阻抗与隧穿绝缘层内电场强度之间极为敏感的相互关系,通过对内嵌于基区4的隧穿绝缘层7选取适当的隧道绝缘材料,并对内嵌的深度、隧穿绝缘层7的厚度进行适当调节,就可以隧穿绝缘层7在栅电极极小的电势变化区间内实现高阻态和低阻态之间的转换,且其通过隧穿绝缘层7上产生的隧穿电流作为引发发射集流出的大量电子电流的驱动电流,与普通TFETs只是利用少量的半导体带间隧穿电流作为器件的导通电流相比,具有更好的正向电流导通特性,基于上述原因,对比于普通结构的MOSFETs、TFETs或普通的双极晶体管,高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,可以实现更高的转移特性。High transfer characteristics and low parasitic capacitance Embedded gate insulation tunneling enhancement transistor, using the extremely sensitive relationship between the impedance of the tunneling insulating layer and the electric field strength in the tunneling insulating layer, through the tunneling insulating layer embedded in the base region 4 7 Select an appropriate tunnel insulating material, and properly adjust the depth of embedding and the thickness of the tunnel insulating layer 7, so that the tunnel insulating layer 7 can achieve high resistance and low resistance within the extremely small potential change range of the gate electrode. The transition between states, and the tunneling current generated on the tunneling insulating layer 7 is used as the driving current to induce a large amount of electron current flowing out of the emitter collection, and ordinary TFETs only use a small amount of tunneling current between semiconductor bands as the conduction of the device. Compared with the passing current, it has better forward current conduction characteristics. Based on the above reasons, compared with ordinary structure MOSFETs, TFETs or ordinary bipolar transistors, high transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistors, Higher transfer characteristics can be achieved.

2.低寄生电容特性2. Low parasitic capacitance characteristics

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,对比于MOSFETs或TFETs,发射极9和源电极的作用相当,集电极10和漏电极的作用相当,由于栅电极8、隧穿绝缘层7以及导电层6均内嵌于基区4的内部,只有上表面与阻挡绝缘层11相接触并远离发射极9和集电极10,这就避免了如同MOSFETs或TFETs则那样的由于栅电极和漏电极之间或栅电极和源电极之间的距离不断缩小而导致的栅源、源栅、栅漏以及漏栅之间寄生电容的明显增大,使器件在保证高转移特性的同时,降低了同尺寸下MOSFETs或TFETs所产生的寄生电容。High transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, compared with MOSFETs or TFETs, the role of the emitter 9 and the source electrode is equivalent, and the role of the collector 10 and the drain electrode is equivalent, because the gate electrode 8, the tunneling insulating layer 7 and the conductive layer 6 are all embedded in the base region 4, and only the upper surface is in contact with the blocking insulating layer 11 and away from the emitter 9 and the collector 10, which avoids the gate electrode and the collector electrode 10 like MOSFETs or TFETs. The significant increase in the parasitic capacitance between the gate-source, source-gate, gate-drain, and drain-gate due to the shrinking distance between the drain electrodes or between the gate electrode and the source electrode makes the device reduce the Parasitic capacitance generated by MOSFETs or TFETs of the same size.

3.低反向泄漏电流3. Low reverse leakage current

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,由于栅电极8与发射区3或集电区5之间的距离取决于隧穿绝缘层7和导电层6的水平长度总和,且和MOSFETs或TFETs相比,在栅电极8与发射区3之间,或者在栅电极8与集电极之间不存在MOSFETs或TFETs所具有的栅极至漏极重叠区,因此不会引发明显的反向泄漏电流。High transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, because the distance between the gate electrode 8 and the emitter region 3 or the collector region 5 depends on the sum of the horizontal lengths of the tunneling insulating layer 7 and the conductive layer 6, and Compared with MOSFETs or TFETs, there is no gate-to-drain overlap region between the gate electrode 8 and the emitter region 3, or between the gate electrode 8 and the collector electrode, which MOSFETs or TFETs have, so no significant reaction is caused. to the leakage current.

附图说明Description of drawings

图1为本发明内嵌栅绝缘隧穿增强晶体管在体硅衬底上形成的二维结构示意图;1 is a schematic diagram of a two-dimensional structure of an embedded gate insulation tunneling enhancement transistor formed on a bulk silicon substrate in the present invention;

图2是步骤一示意图,Figure 2 is a schematic diagram of Step 1,

图3是步骤二示意图,Figure 3 is a schematic diagram of step two,

图4是步骤三示意图,Figure 4 is a schematic diagram of step three,

图5是步骤四示意图,Figure 5 is a schematic diagram of step four,

图6是步骤五示意图,Figure 6 is a schematic diagram of step five,

图7是步骤六示意图,Figure 7 is a schematic diagram of step six,

图8是步骤七示意图,Figure 8 is a schematic diagram of step seven,

图9是步骤八示意图,Figure 9 is a schematic diagram of Step 8,

图10是步骤九示意图,Figure 10 is a schematic diagram of step nine,

图11是步骤十示意图,Figure 11 is a schematic diagram of step ten,

图12是步骤十一示意图。Fig. 12 is a schematic diagram of step eleven.

附图标记说明:Explanation of reference signs:

1、单晶硅衬底;2、晶圆绝缘层;3、发射区;4、基区;5、集电区;6、导电层;7、隧穿绝缘层;8、栅电极;9、发射极;10、集电极;11、阻挡绝缘层。1. Single crystal silicon substrate; 2. Wafer insulating layer; 3. Emitter region; 4. Base region; 5. Collector region; 6. Conductive layer; 7. Tunneling insulating layer; 8. Gate electrode; 9. Emitter; 10, collector; 11, blocking insulating layer.

具体实施方式detailed description

下面结合附图对本发明做进一步的说明:Below in conjunction with accompanying drawing, the present invention will be further described:

如图1为本发明内嵌栅绝缘隧穿增强晶体管在体硅衬底上形成的二维结构示意图;具体包括单晶硅衬底1;晶圆绝缘层2;发射区3;基区4;集电区5;导电层6;隧穿绝缘层7;栅电极8;发射极9;集电极10;阻挡绝缘层11。Figure 1 is a schematic diagram of a two-dimensional structure of an embedded gate insulation tunneling enhancement transistor formed on a bulk silicon substrate in the present invention; specifically, it includes a single crystal silicon substrate 1; a wafer insulating layer 2; an emitter region 3; a base region 4; Collector region 5; conductive layer 6; tunnel insulating layer 7; gate electrode 8; emitter 9; collector 10; blocking insulating layer 11.

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,采用只包含单晶硅衬底1的体硅晶圆作为生成器件衬底,或采用同时包含单晶硅衬底1和晶圆绝缘层2的SOI晶圆作为生成器件的衬底;发射区3、基区4和集电区5位于体硅晶圆的单晶硅衬底1或SOI晶圆的晶圆绝缘层2的上方;发射极9位于发射区3的上方;集电极10位于集电区5的上方;导电层6内嵌于基区4内,并被基区4三面包围;隧穿绝缘层7内嵌于导电层6内,并被导电层6三面包围;栅电极8内嵌于隧穿绝缘层7内,并被隧穿绝缘层7三面包围;阻挡绝缘层11位于器件单元之间和各电极之间,对各器件单元之间和各电极之间起隔离作用。High transfer characteristics and low parasitic capacitance Embedded gate insulation tunneling enhancement transistor, using a bulk silicon wafer containing only a single crystal silicon substrate 1 as the device substrate, or using a single crystal silicon substrate 1 and a wafer insulating layer at the same time 2 of the SOI wafer as the substrate for generating devices; the emitter region 3, the base region 4 and the collector region 5 are located above the single crystal silicon substrate 1 of the bulk silicon wafer or the wafer insulating layer 2 of the SOI wafer; The electrode 9 is located above the emitter region 3; the collector electrode 10 is located above the collector region 5; the conductive layer 6 is embedded in the base region 4 and surrounded by three sides of the base region 4; the tunnel insulating layer 7 is embedded in the conductive layer 6 and surrounded by the conductive layer 6 on three sides; the gate electrode 8 is embedded in the tunneling insulating layer 7 and surrounded by the tunneling insulating layer 7 on three sides; the blocking insulating layer 11 is located between the device units and between the electrodes, for each Between the device units and between the electrodes play an isolation role.

为达到本发明所述的器件功能,本发明提出高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,其核心结构特征为:In order to achieve the device functions described in the present invention, the present invention proposes a high transfer characteristic and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, and its core structural features are:

栅电极8、隧穿绝缘层7和导电层6均内嵌于基区4内,只有上表面与阻挡绝缘层11接触。The gate electrode 8 , the tunneling insulating layer 7 and the conductive layer 6 are all embedded in the base region 4 , and only the upper surface is in contact with the blocking insulating layer 11 .

栅电极8与发射区3之间依次夹有隧穿绝缘层7、导电层6和基区4;A tunnel insulating layer 7, a conductive layer 6 and a base region 4 are sequentially interposed between the gate electrode 8 and the emitter region 3;

栅电极8与集电区4之间依次夹有隧穿绝缘层7、导电层6和基区4;A tunnel insulating layer 7, a conductive layer 6 and a base region 4 are sequentially sandwiched between the gate electrode 8 and the collector region 4;

栅电极8是控制隧穿绝缘层7产生隧穿效应的电极,是控制器件开启和关断的电极。The gate electrode 8 is an electrode for controlling the tunneling effect generated by the tunneling insulating layer 7, and is an electrode for controlling the turning on and off of the device.

隧穿绝缘层7为用于产生栅绝缘层隧穿电流的绝缘层。The tunneling insulating layer 7 is an insulating layer for generating gate insulating layer tunneling current.

导电层6与基区4形成欧姆接触,是金属材料,或者是同基区4具有相同杂质类型的、且掺杂浓度大于1018每立方厘米的半导体材料。The conductive layer 6 forms an ohmic contact with the base region 4 and is a metal material, or a semiconductor material having the same impurity type as the base region 4 and a doping concentration greater than 10 18 per cubic centimeter.

发射区3与基区4之间、集电区5与基区4之间具有相反杂质类型、且发射区3与发射极9之间形成欧姆接触、集电区3与集电极10之间形成欧姆接触。There are opposite impurity types between the emitter region 3 and the base region 4, between the collector region 5 and the base region 4, and an ohmic contact is formed between the emitter region 3 and the emitter electrode 9, and an ohmic contact is formed between the collector region 3 and the collector electrode 10. ohmic contact.

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,以N型为例,发射区3、基区4和集电区5分别为N区、P区和N区,其具体的工作原理为:当集电极10正偏,且栅电极8处于低电位时,栅电极8与导电层6之间没有形成足够的电势差,此时隧穿绝缘层7处于高阻状态,没有明显隧穿电流通过,因此使得基区4和发射区3之间无法形成足够大的基区电流来驱动高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,即器件处于关断状态;随着栅电极8电压的逐渐升高,栅电极8与导电层6之间的电势差逐渐增大,使得位于栅电极8与导电层6之间隧穿绝缘层7内的电场强度也随之逐渐增大,当隧穿绝缘层7内的电场强度位于临界值以下时,隧穿绝缘层7依然保持良好的高阻状态,栅电极和发射极之间的电势差几乎完全降在隧穿绝缘层7的内壁和外壁两侧之间,也就使得基区和发射区之间的电势差极小,因此基区几乎没有电流流过,器件也因此保持良好的关断状态,而当隧穿绝缘层7内的电场强度位于临界值以上时,隧穿绝缘层7会由于隧穿效应而产生明显的隧穿电流,并且隧穿电流则会随着栅电极8电势的增大以极快的速度陡峭上升,这就使得隧穿绝缘层7在栅电极极短的电势变化区间内由高阻态迅速转换为低阻态,当隧穿绝缘层7处于低阻态,此时隧穿绝缘层7在栅电极8和导电层6之间所形成的电阻要远小于导电层6和发射极3之间所形成的电阻,这就使得基区4和发射区3之间形成了足够大的正偏电压,并且在隧穿效应的作用下,在隧穿绝缘层7的内壁和外壁之间产生大量电子移动,即为基区4提供电流源,因此使得基区4和发射区3之间形成了足够大的基区电流来驱动高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,即器件处于开启状态;High transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, taking N-type as an example, the emitter region 3, base region 4 and collector region 5 are N region, P region and N region respectively, and its specific working principle is : When the collector electrode 10 is positively biased and the gate electrode 8 is at a low potential, there is no sufficient potential difference formed between the gate electrode 8 and the conductive layer 6, and the tunneling insulating layer 7 is in a high-resistance state at this time, and no obvious tunneling current passes through , so that it is impossible to form a large enough base current between the base region 4 and the emitter region 3 to drive the embedded gate insulation tunneling enhancement transistor with high transfer characteristics and low parasitic capacitance, that is, the device is in the off state; with the voltage of the gate electrode 8 gradually increases, the potential difference between the gate electrode 8 and the conductive layer 6 gradually increases, so that the electric field intensity in the tunneling insulating layer 7 between the gate electrode 8 and the conductive layer 6 also gradually increases, when the tunneling When the electric field strength in the insulating layer 7 is below the critical value, the tunneling insulating layer 7 still maintains a good high-resistance state, and the potential difference between the gate electrode and the emitter is almost completely dropped on both sides of the inner and outer walls of the tunneling insulating layer 7 Between the base region and the emitter region, the potential difference between the base region and the emitter region is extremely small, so there is almost no current flowing in the base region, and the device remains in a good off state. When the electric field strength in the tunneling insulating layer 7 is at the critical When the value is above , the tunneling insulating layer 7 will generate obvious tunneling current due to the tunneling effect, and the tunneling current will rise steeply at a very fast speed with the increase of the potential of the gate electrode 8, which makes the tunneling The insulating layer 7 rapidly switches from a high-resistance state to a low-resistance state during the extremely short potential change interval of the gate electrode. The resistance formed between the conductive layer 6 and the emitter 3 is much smaller than the resistance formed between the conductive layer 6 and the emitter 3, which makes a sufficiently large forward bias voltage formed between the base region 4 and the emitter region 3, and in the tunneling effect Under the action, a large amount of electron movement is generated between the inner wall and the outer wall of the tunneling insulating layer 7, that is, a current source is provided for the base region 4, so that a sufficiently large base region current is formed between the base region 4 and the emitter region 3 to drive High transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, that is, the device is in the on state;

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,利用隧穿绝缘层阻抗与隧穿绝缘层内电场强度之间极为敏感的相互关系,通过对内嵌于基区4的隧穿绝缘层7选取适当的隧道绝缘材料,并对内嵌的深度、隧穿绝缘层7的厚度进行适当调节,就可以隧穿绝缘层7在栅电极极小的电势变化区间内实现高阻态和低阻态之间的转换,且其通过隧穿绝缘层7上产生的隧穿电流作为引发发射集流出的大量电子电流的驱动电流,与普通TFETs只是利用少量的半导体带间隧穿电流作为器件的导通电流相比,具有更好的正向电流导通特性,基于上述原因,对比于普通结构的MOSFETs、TFETs或普通的双极晶体管,高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,可以实现更高的转移特性。High transfer characteristics and low parasitic capacitance Embedded gate insulation tunneling enhancement transistor, using the extremely sensitive relationship between the impedance of the tunneling insulating layer and the electric field strength in the tunneling insulating layer, through the tunneling insulating layer embedded in the base region 4 7 Select an appropriate tunnel insulating material, and properly adjust the depth of embedding and the thickness of the tunnel insulating layer 7, so that the tunnel insulating layer 7 can achieve high resistance and low resistance within the extremely small potential change range of the gate electrode. The transition between states, and the tunneling current generated on the tunneling insulating layer 7 is used as the driving current to induce a large amount of electron current flowing out of the emitter collection, and ordinary TFETs only use a small amount of tunneling current between semiconductor bands as the conduction of the device. Compared with the passing current, it has better forward current conduction characteristics. Based on the above reasons, compared with ordinary structure MOSFETs, TFETs or ordinary bipolar transistors, high transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistors, Higher transfer characteristics can be achieved.

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,对比于MOSFETs或TFETs,发射极9和源电极的作用相当,集电极10和漏电极的作用相当,由于栅电极8、隧穿绝缘层7以及导电层6均内嵌于基区4的内部,只有上表面与阻挡绝缘层11相接触并远离发射极9和集电极10,这就避免了如同MOSFETs或TFETs则那样的由于栅电极和漏电极之间或栅电极和源电极之间的距离不断缩小而导致的栅源、源栅、栅漏以及漏栅之间寄生电容的明显增大,使器件在保证高转移特性的同时,降低了同尺寸下MOSFETs或TFETs所产生的寄生电容。High transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, compared with MOSFETs or TFETs, the role of the emitter 9 and the source electrode is equivalent, and the role of the collector 10 and the drain electrode is equivalent, because the gate electrode 8, the tunneling insulating layer 7 and the conductive layer 6 are all embedded in the base region 4, and only the upper surface is in contact with the blocking insulating layer 11 and away from the emitter 9 and the collector 10, which avoids the gate electrode and the collector electrode 10 like MOSFETs or TFETs. The significant increase in the parasitic capacitance between the gate-source, source-gate, gate-drain, and drain-gate due to the shrinking distance between the drain electrodes or between the gate electrode and the source electrode makes the device reduce the Parasitic capacitance generated by MOSFETs or TFETs of the same size.

高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管,由于栅电极8与发射区3或集电区5之间的距离取决于隧穿绝缘层7和导电层6的水平长度总和,且和MOSFETs或TFETs相比,在栅电极8与发射区3之间,或者在栅电极8与集电极之间不存在MOSFETs或TFETs所具有的栅极至漏极重叠区,因此不会引发明显的反向泄漏电流。High transfer characteristics and low parasitic capacitance embedded gate insulation tunneling enhancement transistor, because the distance between the gate electrode 8 and the emitter region 3 or the collector region 5 depends on the sum of the horizontal lengths of the tunneling insulating layer 7 and the conductive layer 6, and Compared with MOSFETs or TFETs, there is no gate-to-drain overlap region between the gate electrode 8 and the emitter region 3, or between the gate electrode 8 and the collector electrode, which MOSFETs or TFETs have, so no significant reaction is caused. to the leakage current.

本发明所提出的高转移特性低寄生电容内嵌栅绝缘隧穿增强晶体管的单元及阵列在体硅晶圆上的具体制造工艺步骤如下:The specific manufacturing process steps of the cells and arrays of the embedded gate insulation tunneling enhancement transistor with high transfer characteristics and low parasitic capacitance on the bulk silicon wafer proposed by the present invention are as follows:

步骤一、如图2所示,提供一个SOI晶圆,SOI晶圆的下方为SOI晶圆的单晶硅衬底1,SOI晶圆的中间为晶圆绝缘层2,SOI晶圆上方的单晶硅薄膜用于形成器件的发射区3、基区4和集电区5,通过光刻、刻蚀等工艺在所提供的SOI晶圆上形成如图2所示的长方体状单晶硅孤岛阵列区域,该区域用于进一步形成器件的发射区3、基区4和集电区5;Step 1, as shown in Figure 2, provide an SOI wafer, the bottom of the SOI wafer is the monocrystalline silicon substrate 1 of the SOI wafer, the middle of the SOI wafer is the wafer insulating layer 2, and the single crystal silicon substrate 1 above the SOI wafer The crystalline silicon thin film is used to form the emitter region 3, the base region 4 and the collector region 5 of the device, and a rectangular parallelepiped single crystal silicon island as shown in Figure 2 is formed on the provided SOI wafer through photolithography, etching and other processes An array area, which is used to further form the emitter region 3, the base region 4 and the collector region 5 of the device;

步骤二、如图3所示,在晶圆上方淀积绝缘介质后平坦化表面,初步形成阻挡绝缘层11;Step 2, as shown in FIG. 3, after depositing an insulating medium on the wafer, the surface is planarized, and a blocking insulating layer 11 is preliminarily formed;

步骤三、如图4所示,通过离子注入工艺,在长方体状单晶硅孤岛阵列的每一个区域上形成发射区3、基区4和集电区5,其中基区4的掺杂类型要与发射区3和集电区5相反;Step 3, as shown in Figure 4, through the ion implantation process, an emitter region 3, a base region 4 and a collector region 5 are formed on each region of the rectangular parallelepiped single crystal silicon island array, wherein the doping type of the base region 4 must be Contrary to the emitter region 3 and the collector region 5;

步骤四、如图5所示,通过刻蚀工艺,在基区4上刻蚀出凹槽状区域。Step 4, as shown in FIG. 5 , a groove-shaped region is etched on the base region 4 through an etching process.

步骤五、如图6所示,在晶圆上方淀积金属或具有和基区4相同杂质类型的超重掺杂的多晶硅,使步骤四中所形成的凹槽内部完全被填充,再将表面平坦化至露出基区4,初步形成导电层6;Step five, as shown in Figure 6, deposit metal or over-doped polysilicon with the same impurity type as the base region 4 above the wafer, so that the inside of the groove formed in step four is completely filled, and then the surface is flattened Thinning to expose the base region 4, initially forming the conductive layer 6;

步骤六、如图7所示,通过刻蚀工艺,在导电层6上刻蚀出凹槽状区域,进一步形成导电层6。Step 6. As shown in FIG. 7 , a groove-shaped region is etched on the conductive layer 6 through an etching process to further form the conductive layer 6 .

步骤七、如图8所示,在晶圆上方淀积隧穿绝缘层介质,使步骤六中所形成的凹槽内部完全被填充,再将表面平坦化至露出导电层6,初步形成隧穿绝缘层7;Step 7, as shown in Figure 8, deposit a tunneling insulating layer dielectric on the wafer, so that the inside of the groove formed in step 6 is completely filled, and then planarize the surface to expose the conductive layer 6, initially forming a tunnel insulating layer 7;

步骤八、如图9所示,通过刻蚀工艺,在隧穿绝缘层7上刻蚀出凹槽状区域,进一步形成隧穿绝缘层7。Step 8. As shown in FIG. 9 , a groove-shaped region is etched on the tunneling insulating layer 7 through an etching process to further form the tunneling insulating layer 7 .

步骤九、如图10所示,在晶圆上方淀积金属材料或重掺杂多晶硅,使步骤八中所形成的凹槽内部完全被填充,再将表面平坦化至露出隧穿绝缘层7,形成栅电极8;Step 9, as shown in FIG. 10 , deposit metal material or heavily doped polysilicon on the wafer, so that the inside of the groove formed in step 8 is completely filled, and then planarize the surface to expose the tunnel insulating layer 7, forming the gate electrode 8;

步骤十、如图11所示,在晶圆上方淀积绝缘介质层并平坦化表面,进一步形成阻挡绝缘层11;Step ten, as shown in FIG. 11 , deposit an insulating dielectric layer on the wafer and planarize the surface, and further form a blocking insulating layer 11;

步骤十一、如图12所示,在位于发射区3和集电区5的上方的阻挡绝缘层11内部刻蚀出用于形成发射极9和集电极10的通孔,并在晶圆上表面淀积金属层,使通孔被金属填充,再对金属层进行刻蚀,形成发射极9和集电极10。Step eleven, as shown in FIG. 12 , etch through holes for forming the emitter 9 and the collector 10 inside the blocking insulating layer 11 above the emitter region 3 and the collector region 5 , and place the holes on the wafer A metal layer is deposited on the surface to fill the through hole with metal, and then the metal layer is etched to form the emitter 9 and the collector 10 .

Claims (10)

1. embedded gate insulation tunnelling enhancing transistor, it is characterised in that:Using only comprising monocrystalline substrate(1)Body Silicon Wafer make Monocrystalline substrate is included simultaneously for generating device substrate, or use(1)With wafer insulating barrier(2)SOI wafer be used as maker The substrate of part;Launch site(3), base(4)And collecting zone(5)Positioned at the monocrystalline substrate of body Silicon Wafer(1)Or the crystalline substance of SOI wafer Circle insulating barrier(2)Top;Emitter stage(9)Positioned at launch site(3)Top;Colelctor electrode(10)Positioned at collecting zone(5)Top; Conductive layer(6)It is embedded in base(4)It is interior, and by base(4)Three bread enclose;Tunneling insulation layer(7)It is embedded in conductive layer(6)It is interior, And by conductive layer(6)Three bread enclose;Gate electrode(8)It is embedded in tunneling insulation layer(7)It is interior, and it is tunneled over insulating barrier(7)Three bread Enclose;Barrier insulating layer(11)Embedding gate insulation tunnelling positioned at single high transfer characteristic low parasitic capacitance strengthens the top of transistor.
2. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Emitter stage(9)With current collection Pole(10)Between pass through barrier insulating layer(11)Isolation;Launch site(3)With collecting zone(5)Between pass through barrier insulating layer(11)Every From.
3. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Gate electrode(8), tunnelling it is exhausted Edge layer(7)And conductive layer(6)It is embedded in base(4)It is interior, only upper surface and barrier insulating layer(11)Contact.
4. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Gate electrode(8)With transmitting Area(3)Between accompany tunneling insulation layer successively(7), conductive layer(6)And base(4).
5. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Gate electrode(8)With current collection Area(5)Between accompany tunneling insulation layer successively(7), conductive layer(6)And base(4).
6. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Gate electrode(8)It is control Tunneling insulation layer(7)The electrode of tunneling effect is produced, is the electrode that control device is switched on and off.
7. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Tunneling insulation layer(7)For Insulating barrier for producing gate insulation layer tunnelling current.
8. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Conductive layer(6)With base (4)Form Ohmic contact, conductive layer(6)It is metal material either same base(4)It is with identical dopant type and adulterate it is dense Degree is more than 1018Semi-conducting material per cubic centimeter.
9. embedded gate insulation tunnelling enhancing transistor according to claim 1, it is characterised in that:Launch site(3)With base (4)Between, collecting zone(5)With base(4)Between there is opposite impurity type, and launch site(3)With emitter stage(9)Between formed Ohmic contact, collecting zone(5)With colelctor electrode(10)Between form Ohmic contact.
10. a kind of embedded gate insulation tunnelling as claimed in claim 1 strengthens the manufacture method of transistor, it is characterised in that:Should Processing step is as follows:
Step 1: providing a SOI wafer, the lower section of SOI wafer is the monocrystalline substrate of SOI wafer(1), in SOI wafer Between be wafer insulating barrier(2), the monocrystalline silicon thin film above SOI wafer is used for the launch site for forming device(3), base(4)And collection Electric area(5), rectangular-shape monocrystalline silicon isolated island array region is provided by photoetching, etching technics in the SOI wafer provided, should Region is used for the launch site for further forming device(3), base(4)And collecting zone(5);
Step 2: planarizing surface after deposit dielectric above wafer, barrier insulating layer is preliminarily formed(11);
Step 3: by ion implantation technology, launch site is formed on each region of rectangular-shape monocrystalline silicon isolated island array (3), base(4)And collecting zone(5), wherein base(4)Doping type will and launch site(3)And collecting zone(5)Conversely;
Step 4: by etching technics, in base(4)On etch grooved regions;
Step 5: depositing metal above wafer or having and base(4)The polysilicon of the overweight doping of identical dopant type, makes Inside grooves formed in step 4 are completely filled, then by surface planarisation to exposing base(4), preliminarily form conductive layer (6);
Step 6: by etching technics, in conductive layer(6)On etch grooved regions, further form conductive layer(6);
Step 7: depositing tunneling insulation layer medium above wafer, it is completely filled the inside grooves formed in step 6, Again by surface planarisation to exposing conductive layer(6), preliminarily form tunneling insulation layer(7);
Step 8: by etching technics, in tunneling insulation layer(7)On etch grooved regions, further formed tunnelling insulation Layer(7);
Step 9: depositing metal material or heavily doped polysilicon above wafer, make the inside grooves formed in step 8 complete It is filled entirely, then by surface planarisation to exposing tunneling insulation layer(7), form gate electrode(8);
Step 10: depositing insulating medium layer above wafer and planarizing surface, barrier insulating layer is further formed(11);
Step 11: positioned at launch site(3)And collecting zone(5)Top barrier insulating layer(11)Inside is etched for shape Into emitter stage(9)And colelctor electrode(10)Through hole, and in wafer upper surface deposited metal, be filled with metal through hole, then right Metal level is performed etching, and forms emitter stage(9)And colelctor electrode(10).
CN201410742827.XA 2014-12-08 2014-12-08 Embedded gate insulation tunnelling enhancing transistor Expired - Fee Related CN104465735B (en)

Priority Applications (1)

Application Number Priority Date Filing Date Title
CN201410742827.XA CN104465735B (en) 2014-12-08 2014-12-08 Embedded gate insulation tunnelling enhancing transistor

Applications Claiming Priority (1)

Application Number Priority Date Filing Date Title
CN201410742827.XA CN104465735B (en) 2014-12-08 2014-12-08 Embedded gate insulation tunnelling enhancing transistor

Publications (2)

Publication Number Publication Date
CN104465735A CN104465735A (en) 2015-03-25
CN104465735B true CN104465735B (en) 2017-07-21

Family

ID=52911505

Family Applications (1)

Application Number Title Priority Date Filing Date
CN201410742827.XA Expired - Fee Related CN104465735B (en) 2014-12-08 2014-12-08 Embedded gate insulation tunnelling enhancing transistor

Country Status (1)

Country Link
CN (1) CN104465735B (en)

Families Citing this family (1)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
CN113540225B (en) * 2021-07-19 2022-06-10 西安电子科技大学 A high-performance recessed-gate tunneling field effect transistor based on a quasi-off-band heterojunction and a preparation method thereof

Family Cites Families (5)

* Cited by examiner, † Cited by third party
Publication number Priority date Publication date Assignee Title
FR2914489A1 (en) * 2007-04-02 2008-10-03 St Microelectronics Crolles 2 METHOD FOR MANUFACTURING ELECTRONIC COMPONENTS
CN101728394B (en) * 2009-12-01 2011-11-09 清华大学 Groove type non-volatilisation memory for multi-digit storage
CN102412302B (en) * 2011-10-13 2013-09-18 北京大学 Tunneling field-effect transistor for inhibiting bipolar effect and preparation method thereof
CN203521424U (en) * 2013-10-12 2014-04-02 沈阳工业大学 Half Gate Controlled Source Schottky Barrier Tunneling Field Effect Transistor
CN103779418B (en) * 2014-02-08 2016-08-31 华为技术有限公司 A kind of tunneling field-effect transistor and preparation method thereof

Also Published As

Publication number Publication date
CN104465735A (en) 2015-03-25

Similar Documents

Publication Publication Date Title
CN104409487B (en) The two-way breakdown protection double grid insulation tunnelling enhancing transistor of body silicon and its manufacture method
CN107819027A (en) A kind of source and drain resistive formula H-shaped grid-control two-way switch transistor and its manufacture method
CN103531592B (en) Three gate control type nodeless mesh body pipes of high mobility low source and drain resistance
CN104465737B (en) Body silicon double grid insulation tunnelling base bipolar transistor and its manufacture method
CN104409508B (en) The two-way breakdown protection double grid insulation tunnelling enhancing transistor of SOI substrate and manufacture method
CN104282751A (en) High-integration-level and high-mobility-ratio source, drain and gate auxiliary control type junction-free transistor
CN104465735B (en) Embedded gate insulation tunnelling enhancing transistor
CN107706235B (en) A rectangular gate-controlled U-shaped channel bidirectional switch tunneling transistor and its manufacturing method
CN104485354B (en) SOI substrate folds gate insulation tunnelling enhancing transistor and its manufacture method
CN104538442A (en) Tunnel field effect transistor and preparation method thereof
CN104282753B (en) Highly integrated shape source and drain grid auxiliary control U-shaped raceway groove high mobility nodeless mesh body pipe of subsisting
CN104393033B (en) Gate insulation tunnelling groove base bipolar transistor with breakdown protection function
CN107833925A (en) A kind of source and drain resistive formula two-way switch field-effect transistor and its manufacture method
CN104409489B (en) High-integrated groove insulated gate tunneling bipolar enhancement transistor and manufacture method thereof
CN104485353B (en) Insulated gate tunneling bipolar transistor with U-shaped tunneling insulating layer and manufacturing process
CN107799606B (en) Discrete double rectangular gate-controlled source-drain resistive switching transistor of double conductivity type and manufacturing method thereof
CN107731913B (en) Discrete double rectangular gate-controlled U-shaped channel source-drain double tunneling transistor and manufacturing method thereof
CN107833926B (en) Square cylindrical gate embedded U-shaped channel field effect transistor and its manufacturing method
CN104485352B (en) Groove embeds gate insulation tunnelling enhancing transistor and its manufacturing method
CN104465736B (en) It is embedded to fold grid shape of a saddle insulation tunnelling enhancing transistor and its manufacture method
CN104409490B (en) SOI substrate double grid insulation tunnelling base bipolar transistor and its manufacture method
CN104465731B (en) Gate insulation tunnelling groove bipolar transistor with U-shaped tunnel layer base stage
CN107819036A (en) Source and drain symmetrically interchangeable double bracket shape grid-control tunneling transistor and its manufacture method
CN104409486B (en) Low subthreshold oscillation range and high voltage withstanding insulated gate tunneling transistor and preparing method thereof
CN104282737B (en) High-integration-level H-shaped source, drain and gate auxiliary control U-shaped channel high-mobility-ratio junction-free transistor

Legal Events

Date Code Title Description
C06 Publication
PB01 Publication
SE01 Entry into force of request for substantive examination
GR01 Patent grant
CF01 Termination of patent right due to non-payment of annual fee

Granted publication date: 20170721

Termination date: 20171208

CF01 Termination of patent right due to non-payment of annual fee