CN107819029A - A kind of potential barrier controlling type H-shaped grid-control bidirectional tunneling transistor and its manufacture method - Google Patents
A kind of potential barrier controlling type H-shaped grid-control bidirectional tunneling transistor and its manufacture method Download PDFInfo
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Abstract
本发明涉及一种势垒调控式H形栅控双向隧穿晶体管及其制造方法,本发明所述器件具有H形栅电极、势垒调节栅和左右对称的结构特征,具有较强的栅极控制能力并且可以通过调节源漏可互换电极电压控制金属源漏可互换区作为源区或漏区,改变隧穿电流方向。本发明具有低静态功耗、反向泄漏电流、较强的栅极控制能力、低亚阈值摆幅和可实现双向开关功能的优点。对比于普通MOSFETs型器件,利用隧穿效应实现更优秀的开关特性;对比于普通的隧穿场效应晶体管,本发明具有普通的隧穿场效应晶体管所不具备的源漏可互换的双向对称开关特性,因此适合推广应用。
The invention relates to a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor and a manufacturing method thereof. The device in the invention has H-shaped gate electrodes, barrier adjustment gates, and left-right symmetrical structural features, and has a strong gate Control capability and can control the metal source-drain interchangeable region as the source region or the drain region by adjusting the source-drain interchangeable electrode voltage, and change the tunneling current direction. The invention has the advantages of low static power consumption, reverse leakage current, strong gate control capability, low sub-threshold swing and bidirectional switch function. Compared with ordinary MOSFETs type devices, the tunneling effect is used to realize better switching characteristics; compared with ordinary tunneling field effect transistors, the present invention has two-way symmetry with interchangeable source and drain that ordinary tunneling field effect transistors do not possess Switching characteristics, so it is suitable for popularization and application.
Description
技术领域technical field
本发明涉及超大规模集成电路制造领域,具体涉及一种适用于低功耗集成电路制造的具有低泄漏电流的势垒调控式H形栅控双向隧穿晶体管及其制造方法。The invention relates to the field of ultra-large-scale integrated circuit manufacturing, in particular to a low-leakage barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor suitable for low-power integrated circuit manufacturing and a manufacturing method thereof.
背景技术Background technique
集成电路的基本单元MOSFETs根据摩尔定律的要求,尺寸会变得越来越小,随之而来的不仅仅是在制造工艺上的难度加深,各种不良效应也越发的凸显。如今集成电路设计所采用的MOSFETs型器件由于其工作时自身产生电流的物理机制的限制,其亚阈值摆幅不能低于60mV/dec。而普通隧穿场效应晶体管作为开关型器件使用时,利用载流子在半导体能带之间发生隧穿效应作为电流的导通机制,其亚阈值摆幅要明显优于MOSFETs型器件的60mv/dec极限。然而,普通隧穿场效应晶体管源区和漏区采用不同导电类型的杂质,这种非对称结构特征导致其无法在功能上完全取代具有对称结构特征的MOSFETs型器件。以N型隧穿场效应晶体管为例,如果将其源极和漏极互换,即漏极为低电位,源极为高电位,则隧穿场效应晶体管将始终处于导通状态,导通电流的大小不再能够依靠栅电极而得到良好控制和调节,这使得整个隧穿场效应晶体管的开关特性失效。According to the requirements of Moore's law, the basic unit MOSFETs of integrated circuits will become smaller and smaller in size, which will not only increase the difficulty of the manufacturing process, but also cause various adverse effects to become more prominent. Due to the limitations of the physical mechanism of current generation in the MOSFETs used in IC design today, the subthreshold swing cannot be lower than 60mV/dec. When the ordinary tunneling field effect transistor is used as a switching device, the tunneling effect of carriers between the semiconductor energy bands is used as the conduction mechanism of the current, and its sub-threshold swing is significantly better than the 60mv/ dec limit. However, the source and drain regions of ordinary tunneling field effect transistors use impurities of different conductivity types. This asymmetric structural feature makes it unable to completely replace MOSFETs with symmetrical structural features in terms of functionality. Taking the N-type tunneling field effect transistor as an example, if its source and drain are interchanged, that is, the drain is at a low potential and the source is at a high potential, the tunneling field effect transistor will always be in the on state, and the conduction current The size can no longer be well controlled and adjusted by means of the gate electrode, which renders the switching characteristics of the entire tunneling field effect transistor useless.
发明内容Contents of the invention
发明目的:Purpose of the invention:
为了有效结合和利用MOSFETs型器件源极、漏极可互换和普通隧穿场效应晶体管低亚阈值摆幅的优点,解决MOSFETs型器件亚阈值摆幅无法降低和普通隧穿场效应晶体管只能作为单向开关的不足,本发明提出一种势垒调控式H形栅控双向隧穿晶体管及其制造方法。该晶体管具有逻辑功能与当前基于MOSFETs集成电路完全兼容的优势特点,源漏两端结构的对称性使其可以通过对源极和漏极的电压互换实现源漏双向对称开关的功能,即具有源漏电极可互换的双向开关特性,此外还具有正反向电流比高、低亚阈值摆幅、高正向导通电流等工作特性。In order to effectively combine and utilize the advantages of interchangeable sources and drains of MOSFETs type devices and the low subthreshold swing of ordinary tunneling field effect transistors, solve the problem that the subthreshold swing of MOSFETs type devices cannot be reduced and ordinary tunneling field effect transistors can only As the deficiency of the unidirectional switch, the present invention proposes a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor and a manufacturing method thereof. The transistor has the advantage that the logic function is fully compatible with current integrated circuits based on MOSFETs. The symmetry of the structure at both ends of the source and drain enables it to realize the function of bidirectional symmetrical switching of the source and drain by exchanging the voltage of the source and drain, that is, it has The source-drain electrode can be interchanged with bi-directional switching characteristics. In addition, it also has working characteristics such as high forward and reverse current ratio, low sub-threshold swing, and high forward conduction current.
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:
一种势垒调控式H形栅控双向隧穿晶体管,包含SOI晶圆的硅衬底,SOI晶圆的硅衬底上方为SOI晶圆的衬底绝缘层,SOI晶圆的衬底绝缘层的上方为单晶硅薄膜、势垒调控栅、栅电极绝缘层以及绝缘介质阻挡层的部分区域,单晶硅薄膜具有“凹”字形几何特征,为杂质浓度低于1016cm-3的单晶硅半导体材料,单晶硅薄膜所形成的凹槽形结构内侧表面与前后外侧表面附有栅电极绝缘层;重掺杂源漏可互换区a和重掺杂源漏可互换区b分别通过对单晶硅薄膜所形成的凹槽形结构的两侧垂直部分的上方中间部分掺杂形成,杂质峰值浓度不低于1018cm-3;重掺杂源漏可互换区a的前后表面和内侧表面与源漏可互换本征区a相互接触,并被其三面围绕;重掺杂源漏可互换区b的前后表面和内侧表面与源漏可互换本征区b相互接触,并被其三面围绕;源漏可互换本征区a和源漏可互换本征区b分别位于单晶硅薄膜凹槽形结构的两侧垂直部分上端的未被进行有意掺杂工艺的内侧区域,为杂质浓度低于1016cm-3的单晶硅半导体材料;单晶硅薄膜、源漏可互换本征区a、源漏可互换本征区b、重掺杂源漏可互换区a和重掺杂源漏可互换区b共同组成了一个凹槽形结构;栅电极绝缘层位于单晶硅薄膜所形成的凹槽形结构底部水平部分的上表面和前后表面以及单晶硅薄膜凹槽形结构两侧垂直部分的内侧表面和前后表面;H形栅电极由金属材料或多晶硅材料构成,对单晶硅薄膜所形成的凹槽形结构的两侧垂直部分的上方部分的内侧表面和前后表面形成三面包裹,俯视SOI晶圆,H形栅电极沿源漏方向呈英文大写字母H形状,H形栅电极与单晶硅薄膜凹槽形结构之间通过栅电极绝缘层彼此绝缘,H形栅电极只对单晶硅薄膜所形成的凹槽形结构的两侧垂直部分的上方部分具有场效应控制作用,对单晶硅薄膜所形成的凹槽形结构的两侧垂直部分的下方区域以及底部水平部分区域没有明显场效应控制作用;势垒调控栅由金属材料或多晶硅材料构成,位于单晶硅薄膜所形成的凹槽形结构底部水平部分的上表面和前后表面,对单晶硅薄膜所形成的凹槽形结构底部水平部分形成三面包裹,并通过栅电极绝缘层与单晶硅薄膜彼此绝缘隔离,势垒调控栅只对单晶硅薄膜所形成的凹槽形结构底部水平部分有场效应控制作用,对单晶硅薄膜所形成的凹槽形结构的两侧垂直部分的上方部分没有明显场效应控制作用;H形栅电极位于单晶硅薄膜所形成的凹槽形结构的凹槽内侧的部分的下表面与势垒调控栅之间具有绝缘介质阻挡层的部分区域,H形栅电极与势垒调控栅之间通过绝缘介质阻挡层彼此绝缘隔离;源漏可互换电极a由金属材料构成,位于重掺杂源漏可互换区a的上方;源漏可互换电极b也由金属材料构成,位于重掺杂源漏可互换区b的上方,源漏可互换电极a、源漏可互换电极b和H形栅电极这三个电极之间通过绝缘介质阻挡层彼此绝缘;势垒调控栅的左右两侧呈对称结构,能在源漏可互换电极a和源漏可互换电极b对称互换的情况下实现同样的输出特性。A potential barrier control type H-shaped gate-controlled bidirectional tunneling transistor, comprising a silicon substrate of an SOI wafer, a substrate insulating layer of the SOI wafer above the silicon substrate of the SOI wafer, and a substrate insulating layer of the SOI wafer The upper part of the monocrystalline silicon film, the barrier control gate, the gate electrode insulating layer and the insulating dielectric barrier layer, the monocrystalline silicon film has a "concave" geometric feature, and is a single-crystal silicon film with an impurity concentration lower than 10 16 cm -3 Crystalline silicon semiconductor material, the inner surface of the groove-shaped structure formed by single crystal silicon thin film and the front and rear outer surfaces are attached with a gate electrode insulating layer; the heavily doped source-drain interchangeable region a and the heavily doped source-drain interchangeable region b It is formed by doping the upper middle part of the vertical part on both sides of the groove-shaped structure formed by the single-crystal silicon film respectively, and the impurity peak concentration is not lower than 10 18 cm -3 ; the heavily doped source-drain interchangeable region a The front, rear and inner surfaces are in contact with the source-drain interchangeable intrinsic region a and are surrounded by three sides; the front, rear and inner surfaces of the heavily doped source-drain interchangeable region b are in contact with the source-drain interchangeable intrinsic region b are in contact with each other and surrounded by three sides; the source-drain interchangeable intrinsic region a and the source-drain interchangeable intrinsic region b are respectively located at the upper ends of the vertical parts on both sides of the groove-shaped structure of the single-crystal silicon film that have not been intentionally doped The inner region of the impurity process is a single crystal silicon semiconductor material with an impurity concentration lower than 10 16 cm -3 ; single crystal silicon thin film, source-drain interchangeable intrinsic region a, source-drain interchangeable intrinsic region b, heavily doped The impurity source-drain interchangeable region a and the heavily doped source-drain interchangeable region b together form a groove-shaped structure; the gate electrode insulating layer is located on the upper surface of the bottom horizontal part of the groove-shaped structure formed by the single crystal silicon film and the front and rear surfaces, as well as the inner surface and the front and rear surfaces of the vertical parts on both sides of the groove-shaped structure of the monocrystalline silicon film; The inner surface and the front and rear surfaces of the upper part of the vertical part form a three-sided package. Looking down on the SOI wafer, the H-shaped gate electrode is in the shape of an English capital letter H along the source-drain direction. The gate electrode insulating layer is insulated from each other, and the H-shaped gate electrode only has a field effect control effect on the upper part of the vertical part on both sides of the groove-shaped structure formed by the single-crystal silicon film. The areas below the vertical parts on both sides of the structure and the horizontal part of the bottom have no obvious field effect control; the barrier regulation gate is made of metal material or polysilicon material, and is located on the horizontal part of the bottom of the groove-shaped structure formed by a single crystal silicon film. The surface and the front and rear surfaces form a three-sided package on the bottom horizontal part of the groove-shaped structure formed by the single-crystal silicon film, and are insulated from each other by the gate electrode insulating layer and the single-crystal silicon film. The horizontal part at the bottom of the groove-shaped structure formed has a field effect control effect, and has no obvious field effect control effect on the upper part of the vertical parts on both sides of the groove-shaped structure formed by the single crystal silicon film; the H-shaped gate electrode is located on the single crystal silicon film. There is an insulating medium between the lower surface of the part inside the groove of the groove-shaped structure formed by the film and the barrier control gate In a part of the barrier layer, the H-shaped gate electrode and the barrier control gate are insulated and isolated from each other by an insulating dielectric barrier layer; the source-drain interchangeable electrode a is made of metal material, and is located in the heavily doped source-drain interchangeable region a above; the source-drain interchangeable electrode b is also made of metal material, located above the heavily doped source-drain interchangeable region b, the source-drain interchangeable electrode a, the source-drain interchangeable electrode b and the H-shaped gate electrode The three electrodes are insulated from each other by an insulating dielectric barrier layer; the left and right sides of the barrier control gate have a symmetrical structure, and the same can be achieved under the condition that the source-drain interchangeable electrode a and the source-drain interchangeable electrode b are symmetrically interchangeable. output characteristics.
一种势垒调控式H形栅控双向隧穿晶体管制备方法的具体制造步骤如下:The specific manufacturing steps of a method for preparing a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor are as follows:
步骤一:提供一个SOI晶圆,最下方为SOI晶圆的硅衬底,硅衬底的上面是衬底绝缘层,衬底绝缘层的上表面为单晶硅薄膜,通过光刻或刻蚀工艺,对SOI晶圆上方的单晶硅薄膜进行刻蚀,除去前后两侧以及中间部分区域的单晶硅薄膜,形成具有凹槽形结构特征的单晶硅薄膜;Step 1: Provide an SOI wafer, the bottom of which is the silicon substrate of the SOI wafer, the upper surface of the silicon substrate is a substrate insulating layer, and the upper surface of the substrate insulating layer is a single crystal silicon film. process, etch the single crystal silicon film above the SOI wafer, remove the single crystal silicon film on the front and back sides and the middle part, and form a single crystal silicon film with groove-shaped structural features;
步骤二:通过氧化或淀积、刻蚀工艺,在单晶硅薄膜所形成的凹槽形结构的前后外侧表面和凹槽两侧垂直部分的内侧表面及凹槽底部水平部分的上方表面形成栅电极绝缘层;Step 2: Form gates on the front and rear outer surfaces of the groove-shaped structure formed by the single crystal silicon film, the inner surfaces of the vertical parts on both sides of the groove, and the upper surface of the horizontal part of the bottom of the groove through oxidation or deposition and etching processes. electrode insulation layer;
步骤三:在SOI晶圆上方淀积绝缘介质,平坦化至表面露出单晶硅薄膜,初步形成绝缘介质阻挡层;Step 3: Deposit an insulating dielectric on the SOI wafer, planarize until the surface exposes a single crystal silicon film, and initially form an insulating dielectric barrier layer;
步骤四:通过刻蚀工艺,对步骤三中所形成的位于单晶硅薄膜凹槽结构底部水平部分的前后表面的部分绝缘介质阻挡层进行刻蚀至露出栅电极绝缘层,进一步形成绝缘介质阻挡层;Step 4: Etching part of the insulating dielectric barrier layer formed in step 3 on the front and rear surfaces of the bottom horizontal part of the single crystal silicon film groove structure to expose the gate electrode insulating layer to further form an insulating dielectric barrier Floor;
步骤五:通过淀积工艺,在SOI晶圆上方淀积金属或多晶硅,平坦化表面至露出单晶硅薄膜,初步形成势垒调控栅;Step 5: Deposit metal or polysilicon on top of the SOI wafer through a deposition process, planarize the surface until the single crystal silicon film is exposed, and initially form a barrier control gate;
步骤六:先通过刻蚀工艺刻蚀掉单晶硅薄膜所形成的凹槽结构底部水平部分的上方的绝缘介质阻挡层至露出栅电极绝缘层,在通过淀积工艺在SOI晶圆上方淀积金属或多晶硅,平坦化表面至露出单晶硅薄膜,进一步形成势垒调控栅;Step 6: Firstly, etch away the insulating dielectric barrier layer above the horizontal part of the bottom of the groove structure formed by the single crystal silicon film through an etching process to expose the gate electrode insulating layer, and then deposit it on the SOI wafer through a deposition process. Metal or polysilicon, planarize the surface to expose the single crystal silicon film, and further form the barrier control gate;
步骤七:通过刻蚀工艺刻蚀掉步骤六所形成的势垒调控栅的上方区域,进一步形成势垒调控栅;Step 7: Etching away the upper region of the barrier control gate formed in step 6 by an etching process to further form the barrier control gate;
步骤八:淀积工艺,在SOI晶圆上方淀积绝缘介质,平坦化表面至露出单晶硅薄膜,进一步形成绝缘介质阻挡层;Step 8: Deposition process, depositing an insulating dielectric on the SOI wafer, planarizing the surface to expose the single crystal silicon film, and further forming an insulating dielectric barrier layer;
步骤九:通过光刻或刻蚀工艺,对在步骤八中所形成的部分绝缘介质阻挡层进行部分刻蚀,再在SOI晶圆上方淀积金属或多晶硅,平坦化表面至露出单晶硅薄膜,形成H形栅电极;Step 9: Partially etch the part of the insulating dielectric barrier layer formed in step 8 by photolithography or etching process, and then deposit metal or polysilicon on the SOI wafer, and planarize the surface to expose the single crystal silicon film , forming an H-shaped gate electrode;
步骤十:通过离子注入工艺,单晶硅薄膜所形成的凹槽结构的两侧垂直部分上表面的中间外侧部分进行掺杂,形成重掺杂源漏可互换区a和重掺杂源漏可互换区b;Step 10: Through the ion implantation process, the middle and outer parts of the upper surface of the vertical parts on both sides of the groove structure formed by the single crystal silicon film are doped to form a heavily doped source and drain interchangeable region a and a heavily doped source and drain interchangeable zone b;
步骤十一:通过淀积工艺,在SOI晶圆上方淀积绝缘介质,形成其余部分的绝缘介质阻挡层;平坦化表面后通过刻蚀工艺去除重掺杂源漏可互换区a和重掺杂源漏可互换区b上方的绝缘介质阻挡层至露出重掺杂源漏可互换区a和重掺杂源漏可互换区b的上表面,再通过淀积工艺向刻蚀形成的通孔中注入金属至通孔被完全填充,最后将表面平坦化处理,形成源漏可互换电极a和源漏可互换电极b。Step 11: Deposit an insulating dielectric on top of the SOI wafer through a deposition process to form the rest of the insulating dielectric barrier layer; after planarizing the surface, remove the heavily doped source-drain interchangeable region a and heavily doped The insulating dielectric barrier layer above the impurity source-drain interchangeable region b is exposed to the upper surface of the heavily doped source-drain interchangeable region a and the heavily doped source-drain interchangeable region b, and then formed by etching towards the doped source-drain interchangeable region b. The metal is injected into the through hole until the through hole is completely filled, and finally the surface is planarized to form the source-drain interchangeable electrode a and the source-drain interchangeable electrode b.
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.源漏对称可互换的双向开关特性;1. Symmetrical interchangeable bidirectional switching characteristics of source and drain;
本发明所述器件为势垒调控式H形栅控双向隧穿晶体管,单晶硅薄膜的左右两端分别具有彼此独立的隧穿结构,由于器件具有左右对称结构,在H形栅电极的控制作用下,单晶硅薄膜左右两端在与栅电极绝缘层接触的表面附近同时发生隧穿,结合势垒调控栅对单晶硅薄膜中间部分电势的调控作用,使器件形成正向导通和反向阻挡,通过调节源漏可互换电极a和源漏可互换电极b的电压控制重掺杂源漏可互换区a和重掺杂源漏可互换区b作为源区或漏区,因此可改变隧穿电流方向,实现本发明的源漏对称可互换的双向开关特性。The device described in the present invention is a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor. The left and right ends of the single crystal silicon film have tunnel structures independent of each other. Under the action, the left and right ends of the single crystal silicon film tunnel simultaneously near the surface in contact with the gate electrode insulating layer, combined with the regulating effect of the barrier regulation gate on the potential of the middle part of the single crystal silicon film, the device forms forward conduction and reverse conduction. To block, control the heavily doped source-drain interchangeable region a and the heavily doped source-drain interchangeable region b as the source region or the drain region by adjusting the voltage of the source-drain interchangeable electrode a and the source-drain interchangeable electrode b , so the tunneling current direction can be changed, and the source-drain symmetry and interchangeable bidirectional switching characteristics of the present invention can be realized.
2.低亚阈值摆幅;2. Low subthreshold swing;
由于本发明是利用带带隧穿效应作为场效应晶体管的导通机制,在H形栅电极栅的控制作用下,使得能带在相同的栅电压下更容易发生弯曲,调节隧穿电流的大小,相较于MOSFETs型器件可获得更低的亚阈值摆幅。Since the present invention utilizes the band-band tunneling effect as the conduction mechanism of the field effect transistor, under the control of the H-shaped gate electrode, the energy band is more likely to be bent under the same gate voltage, and the size of the tunneling current is adjusted. , a lower subthreshold swing can be obtained compared to MOSFETs-type devices.
3.低静态功耗、低反向泄漏电流和高正反向电流比;3. Low static power consumption, low reverse leakage current and high forward and reverse current ratio;
以导通类型为N型为例,重掺杂源漏可互换区a和重掺杂源漏可互换区b此时为P型掺杂,当重掺杂源漏可互换区a、重掺杂源漏可互换区b之间存在电势差时,且当H形栅电极处于亚阈值或反偏状态,由于势垒调控栅一直工作在正偏状态,位于单晶硅薄膜两侧的源漏可互换本征区a和源漏可互换本征区b的电势低于单晶硅薄膜中间部分受势垒调控栅控制部分的电势,受H形栅电极的场效应的控制的在源漏可互换本征区a和源漏可互换本征区b所堆积的空穴和重掺杂源漏可互换区a和重掺杂源漏可互换区b内的空穴都无法通过受势垒调控栅控制的在单晶硅薄膜中间部分所形成势垒,与普通MOSFETs或隧道场效应晶体管结构相比,既不存在漏电极和栅电极之间的较强场强区域,即形不成大量由隧道效应所形成的电子空穴对,且由于势垒调控栅的辅助控制作用,在单晶硅薄膜中间部分所形成的势垒可有效阻挡在重掺杂源漏可互换区a和重掺杂源漏可互换区b之间、在源漏可互换本征区a和源漏可互换本征区b之间的空穴电流的形成。因此本发明具有低静态功耗、低反向泄漏电流和高正反向电流比的优点。Taking the conduction type as N-type as an example, the heavily doped source-drain interchangeable region a and the heavily doped source-drain interchangeable region b are P-type doped at this time, when the heavily doped source-drain interchangeable region a , When there is a potential difference between the heavily doped source-drain interchangeable region b, and when the H-shaped gate electrode is in the subthreshold or reverse biased state, since the barrier control gate has been working in the forward biased state, it is located on both sides of the single crystal silicon film The potential of the source-drain interchangeable intrinsic region a and the source-drain interchangeable intrinsic region b is lower than the potential of the middle part of the single crystal silicon film controlled by the barrier regulating gate, and is controlled by the field effect of the H-shaped gate electrode The holes accumulated in the source-drain interchangeable intrinsic region a and the source-drain interchangeable intrinsic region b and the holes in the heavily doped source-drain interchangeable region a and the heavily doped source-drain interchangeable region b Holes cannot pass through the potential barrier formed in the middle part of the single crystal silicon film controlled by the barrier control gate. Compared with the structure of ordinary MOSFETs or tunnel field effect transistors, there is no strong field between the drain electrode and the gate electrode. Strong region, that is, a large number of electron-hole pairs formed by the tunnel effect cannot be formed, and due to the auxiliary control effect of the barrier regulation gate, the potential barrier formed in the middle part of the single crystal silicon film can effectively block the heavily doped source and drain. Formation of hole current between the interchangeable region a and the heavily doped source-drain interchangeable region b, and between the source-drain interchangeable intrinsic region a and the source-drain interchangeable intrinsic region b. Therefore, the invention has the advantages of low static power consumption, low reverse leakage current and high forward and reverse current ratio.
附图说明Description of drawings
图1为本发明一种势垒调控式H形栅控双向隧穿晶体管的俯视图;1 is a top view of a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor of the present invention;
图2为本发明一种势垒调控式H形栅控双向隧穿晶体管的沿虚线A的剖面图;Fig. 2 is a sectional view along the dotted line A of a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor of the present invention;
图3为本发明一种势垒调控式H形栅控双向隧穿晶体管的沿虚线B的剖面图;3 is a cross-sectional view along the dotted line B of a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor of the present invention;
图4为步骤一的俯视图;Fig. 4 is the top view of step 1;
图5为步骤一的沿虚线A的剖面图;Fig. 5 is the sectional view along the dotted line A of step 1;
图6为步骤一的沿虚线B的剖面图;Fig. 6 is a sectional view along the dotted line B of step 1;
图7为步骤一的沿虚线C的剖面图;Fig. 7 is a sectional view along the dotted line C of step one;
图8为步骤二的俯视图;Fig. 8 is the top view of step 2;
图9为步骤二的沿虚线A的剖面图;Fig. 9 is a sectional view along the dotted line A of step 2;
图10为步骤二的沿虚线B的剖面图;Fig. 10 is a sectional view along the dotted line B of step 2;
图11为步骤二的沿虚线C的剖面图;Fig. 11 is a sectional view along the dotted line C of step 2;
图12为步骤二的沿虚线D的剖面图;Fig. 12 is a sectional view along the dotted line D of step 2;
图13为步骤二的沿虚线E的剖面图;Fig. 13 is a sectional view along the dotted line E of step 2;
图14为步骤三的俯视图;Fig. 14 is the top view of step 3;
图15为步骤三的沿虚线A的剖面图;Fig. 15 is a sectional view along the dotted line A of step 3;
图16为步骤三的沿虚线B的剖面图;Fig. 16 is a sectional view along the dotted line B of step 3;
图17为步骤三的沿虚线C的剖面图;Fig. 17 is a sectional view along the dotted line C of step 3;
图18为步骤三的沿虚线D的剖面图;Fig. 18 is a sectional view along the dotted line D of step 3;
图19为步骤三的沿虚线E的剖面图;Fig. 19 is a sectional view along the dotted line E of step 3;
图20为步骤四的俯视图;Figure 20 is a top view of step 4;
图21为步骤四的沿虚线A的剖面图;Fig. 21 is a sectional view along the dotted line A of step 4;
图22为步骤四的沿虚线B的剖面图;Fig. 22 is a sectional view along the dotted line B of step 4;
图23为步骤五的俯视图;Figure 23 is a top view of step five;
图24为步骤五的沿虚线A的剖面图;Fig. 24 is a sectional view along the dotted line A of step five;
图25为步骤五的沿虚线B的剖面图;Fig. 25 is a sectional view along the dotted line B of step five;
图26为步骤六的俯视图;Figure 26 is a top view of step six;
图27为步骤六的沿虚线A的剖面图;Fig. 27 is a sectional view along the dotted line A of step six;
图28为步骤六的沿虚线B的剖面图;Fig. 28 is a sectional view along the dotted line B of step six;
图29为步骤六的沿虚线C的剖面图;Fig. 29 is a sectional view along the dotted line C of step six;
图30为步骤七的俯视图;Figure 30 is a top view of step seven;
图31为步骤七的沿虚线A的剖面图;Fig. 31 is a sectional view along the dotted line A of step 7;
图32为步骤七的沿虚线B的剖面图;Fig. 32 is a sectional view along the dotted line B of step 7;
图33为步骤七的沿虚线C的剖面图;Fig. 33 is a sectional view along the dotted line C of step seven;
图34为步骤八的俯视图;Figure 34 is a top view of step eight;
图35为步骤八的沿虚线A的剖面图;Fig. 35 is a sectional view along the dotted line A of step eight;
图36为步骤八的沿虚线B的剖面图;Fig. 36 is a sectional view along the dotted line B of step eight;
图37为步骤八的沿虚线C的剖面图;Fig. 37 is a sectional view along the dotted line C of step eight;
图38为步骤九的俯视图;Figure 38 is a top view of step nine;
图39为步骤九的沿虚线A的剖面图;Fig. 39 is a sectional view along the dotted line A of step nine;
图40为步骤九的沿虚线B的剖面图;Fig. 40 is a sectional view along the dotted line B of step nine;
图41为步骤九的沿虚线C的剖面图;Fig. 41 is a sectional view along the dotted line C of step nine;
图42为步骤十的俯视图;Figure 42 is a top view of step ten;
图43为步骤十的沿虚线A的剖面图;Fig. 43 is a sectional view along the dotted line A of step ten;
图44为步骤十的沿虚线B的剖面图;Fig. 44 is a sectional view along the dotted line B of step ten;
图45为步骤十一的俯视图;Figure 45 is a top view of step eleven;
图46为步骤十一的沿虚线A的剖面图;Fig. 46 is a sectional view along the dotted line A of step eleven;
图47为步骤十一的沿虚线B的剖面图。Fig. 47 is a cross-sectional view along the dotted line B in step eleven.
附图标记说明:Explanation of reference signs:
1、单晶硅薄膜;2、势垒调控栅;3、源漏可互换本征区a;4、源漏可互换本征区b;5、重掺杂源漏可互换区a;6、重掺杂源漏可互换区b;7、栅电极绝缘层;8、H形栅电极;9、源漏可互换电极a;10、源漏可互换电极b;11、衬底绝缘层;12、硅衬底;13、绝缘介质阻挡层。1. Single crystal silicon thin film; 2. Barrier control gate; 3. Source-drain interchangeable intrinsic region a; 4. Source-drain interchangeable intrinsic region b; 5. Heavily doped source-drain interchangeable region a ; 6. Heavily doped source-drain interchangeable region b; 7. Gate electrode insulating layer; 8. H-shaped gate electrode; 9. Source-drain interchangeable electrode a; 10. Source-drain interchangeable electrode b; 11. Substrate insulating layer; 12, silicon substrate; 13, insulating dielectric barrier layer.
具体实施方式Detailed ways
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、图2和图3所示,一种势垒调控式H形栅控双向隧穿晶体管,包含SOI晶圆的硅衬底12,SOI晶圆的硅衬底12上方为SOI晶圆的衬底绝缘层11,SOI晶圆的衬底绝缘层11的上方为单晶硅薄膜1、势垒调控栅2、栅电极绝缘层7以及绝缘介质阻挡层13的部分区域,单晶硅薄膜1具有“凹”字形几何特征,为杂质浓度低于1016cm-3的单晶硅半导体材料,单晶硅薄膜1所形成的凹槽形结构内侧表面与前后外侧表面附有栅电极绝缘层7;重掺杂源漏可互换区a5和重掺杂源漏可互换区b 6分别通过对单晶硅薄膜1所形成的凹槽形结构的两侧垂直部分的上方中间部分掺杂形成,杂质峰值浓度不低于1018cm-3;重掺杂源漏可互换区a 5的前后表面和内侧表面与源漏可互换本征区a 3相互接触,并被其三面围绕;重掺杂源漏可互换区b 6的前后表面和内侧表面与源漏可互换本征区b 4相互接触,并被其三面围绕;源漏可互换本征区a 3和源漏可互换本征区b 4分别位于单晶硅薄膜1凹槽形结构的两侧垂直部分上端的未被进行有意掺杂工艺的内侧区域,为杂质浓度低于1016cm-3的单晶硅半导体材料;单晶硅薄膜1、源漏可互换本征区a 3、源漏可互换本征区b 4、重掺杂源漏可互换区a 5和重掺杂源漏可互换区b 6共同组成了一个凹槽形结构;栅电极绝缘层7位于单晶硅薄膜1所形成的凹槽形结构底部水平部分的上表面和前后表面以及单晶硅薄膜1凹槽形结构两侧垂直部分的内侧表面和前后表面;H形栅电极8由金属材料或多晶硅材料构成,对单晶硅薄膜1所形成的凹槽形结构的两侧垂直部分的上方部分的内侧表面和前后表面形成三面包裹,俯视SOI晶圆,H形栅电极8沿源漏方向呈英文大写字母H形状,H形栅电极8与单晶硅薄膜1凹槽形结构之间通过栅电极绝缘层7彼此绝缘,H形栅电极8只对单晶硅薄膜1所形成的凹槽形结构的两侧垂直部分的上方部分具有场效应控制作用,对单晶硅薄膜1所形成的凹槽形结构的两侧垂直部分的下方区域以及底部水平部分区域没有明显场效应控制作用;势垒调控栅2由金属材料或多晶硅材料构成,位于单晶硅薄膜1所形成的凹槽形结构底部水平部分的上表面和前后表面,对单晶硅薄膜1所形成的凹槽形结构底部水平部分形成三面包裹,并通过栅电极绝缘层7与单晶硅薄膜1彼此绝缘隔离,势垒调控栅2只对单晶硅薄膜1所形成的凹槽形结构底部水平部分有场效应控制作用,对单晶硅薄膜1所形成的凹槽形结构的两侧垂直部分的上方部分没有明显场效应控制作用;H形栅电极8位于单晶硅薄膜1所形成的凹槽形结构的凹槽内侧的部分的下表面与势垒调控栅2之间具有绝缘介质阻挡层13的部分区域,H形栅电极8与势垒调控栅2之间通过绝缘介质阻挡层13彼此绝缘隔离;源漏可互换电极a 9由金属材料构成,位于重掺杂源漏可互换区a 5的上方;源漏可互换电极b 10也由金属材料构成,位于重掺杂源漏可互换区b 6的上方,源漏可互换电极a 9、源漏可互换电极b 10和H形栅电极8这三个电极之间通过绝缘介质阻挡层13彼此绝缘;势垒调控栅2的左右两侧呈对称结构,能在源漏可互换电极a 9和源漏可互换电极b 10对称互换的情况下实现同样的输出特性。As shown in FIG. 1, FIG. 2 and FIG. 3, a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor includes a silicon substrate 12 of an SOI wafer, and an SOI wafer is above the silicon substrate 12 of the SOI wafer. The substrate insulating layer 11 of the SOI wafer is above the substrate insulating layer 11 of the single crystal silicon film 1, the barrier control gate 2, the gate electrode insulating layer 7 and the partial area of the insulating dielectric barrier layer 13, and the single crystal silicon film 1 has the geometric feature of "concave" and is a single crystal silicon semiconductor material with an impurity concentration lower than 10 16 cm -3 . The inner surface of the groove-shaped structure formed by the single crystal silicon film 1 and the front and rear outer surfaces are attached with a gate electrode insulating layer 7. The heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6 are respectively doped by doping the upper middle part of the vertical part on both sides of the groove-shaped structure formed by the single crystal silicon film 1 Formed, the impurity peak concentration is not lower than 10 18 cm -3 ; the front, rear and inner surfaces of the heavily doped source-drain interchangeable region a5 are in contact with the source-drain interchangeable intrinsic region a3, and are surrounded by three sides ; The front, rear and inner surfaces of the heavily doped source-drain interchangeable region b 6 are in contact with the source-drain interchangeable intrinsic region b 4 and are surrounded by three sides; the source-drain interchangeable intrinsic region a 3 and the source The drain-interchangeable intrinsic regions b4 are respectively located at the upper ends of the vertical parts on both sides of the groove-shaped structure of the single-crystal silicon thin film 1 , and the inner regions that have not been intentionally doped Crystalline silicon semiconductor material; single crystal silicon film 1, source-drain interchangeable intrinsic region a 3, source-drain interchangeable intrinsic region b 4, heavily doped source-drain interchangeable region a 5 and heavily doped source-drain The interchangeable regions b and 6 together form a groove-shaped structure; the gate electrode insulating layer 7 is located on the upper surface and the front and rear surfaces of the bottom horizontal part of the groove-shaped structure formed by the single-crystal silicon film 1 and the groove of the single-crystal silicon film 1 The inside surface and the front and rear surfaces of the vertical parts on both sides of the groove-shaped structure; The front and back surfaces form three-sided wrapping, looking down on the SOI wafer, the H-shaped gate electrode 8 is in the shape of an English capital letter H along the source-drain direction, and the gate electrode insulating layer is passed between the H-shaped gate electrode 8 and the groove-shaped structure of the single crystal silicon film 1 7 are insulated from each other, and the H-shaped gate electrode 8 only has a field effect control effect on the upper part of the vertical part on both sides of the groove-shaped structure formed by the single-crystal silicon film 1, and the groove-shaped structure formed by the single-crystal silicon film 1 The areas below the vertical parts on both sides and the horizontal part of the bottom have no obvious field effect control function; the barrier control gate 2 is made of metal material or polysilicon material, and is located at the bottom horizontal part of the groove-shaped structure formed by the single crystal silicon film 1 The upper surface and the front and rear surfaces wrap three sides of the bottom horizontal part of the groove-shaped structure formed by the single crystal silicon film 1, and are insulated and isolated from the single crystal silicon film 1 by the gate electrode insulating layer 7, and the barrier control gate 2 is only for The horizontal portion at the bottom of the groove-shaped structure formed by the single crystal silicon film 1 has a field effect control function, and the groove formed by the single crystal silicon film 1 The upper part of the vertical parts on both sides of the H-shaped structure has no obvious field effect control function; the lower surface of the H-shaped gate electrode 8 located inside the groove of the groove-shaped structure formed by the single crystal silicon film 1 is in contact with the barrier control gate 2 There is an insulating dielectric barrier layer 13 in between, and the H-shaped gate electrode 8 and the barrier control gate 2 are insulated and isolated from each other by the insulating dielectric barrier layer 13; the source-drain interchangeable electrode a 9 is made of metal material, located at Doped above the source-drain interchangeable region a5; the source-drain interchangeable electrode b10 is also made of metal material, located above the heavily doped source-drain interchangeable region b6, and the source-drain interchangeable electrode a9 1. The source-drain interchangeable electrode b 10 and the H-shaped gate electrode 8 are insulated from each other by an insulating dielectric barrier layer 13; The same output characteristics can be achieved under the condition that the electrode a 9 and the source-drain interchangeable electrode b 10 are symmetrically interchanged.
本发明提供一种势垒调控式H形栅控双向隧穿晶体管,具有左右对称的结构特征,通过调节源漏可互换电极a 9和源漏可互换电极b 10的电压控制重掺杂源漏可互换区a 5和重掺杂源漏可互换区b 6作为源区或漏区,改变隧穿电流方向,使器件实现双向隧穿导通的源漏对称可互换特性。以重掺杂源漏可互换区a 5和重掺杂源漏可互换区b 6为P型杂质为例,当重掺杂源漏可互换区a 5、重掺杂源漏可互换区b 6之间存在电势差时,且当H形栅电极8处于负压反偏状态,受H形栅场效应作用影响,重掺杂源漏可互换区a 5会向源漏可互换本征区a 3提供空穴、重掺杂源漏可互换区b 6会向源漏可互换本征区b 4提供空穴,因此会在源漏可互换本征区a 3和源漏可互换本征区b 4均产生空穴堆积,使得源漏可互换本征区a 3和源漏可互换本征区b 4此时均显现P型状态,所堆积的空穴使得源漏可互换本征区a3和源漏可互换本征区b 4在H形栅电极8的作用下阻值下降,即源区、漏区均处于低阻状态,但由于势垒调控栅2始终施加正向电压,对两侧的源漏可互换本征区a 3和源漏可互换本征区b 4内的空穴形成势垒,且对两侧的重掺杂源漏可互换区a 5、重掺杂源漏可互换区b 6内的空穴也形成势垒,且受势垒调控栅2所施加正向电压场效应的影响,受控于势垒调控栅2的单晶硅薄膜1的中间部分会呈现N型半导体状态,使得显现P型特征的源漏可互换本征区a3与此时为N型的单晶硅薄膜1的中间部分在漏源电压作用下形成反偏的PN结结构,因此当H形栅电极8处于负压反偏状态,由于在晶体管内部存在着上述反偏的PN结结构,晶体管整体呈现高阻阻断状态;随着H形栅电极8被施加的电压从负电压逐渐上升至平带电压附近,重掺杂源漏可互换区a 5不会向源漏可互换本征区a 3提供大量空穴,重掺杂源漏可互换区b6不会向源漏可互换本征区b 4提供大量空穴,同时由于此时源漏可互换本征区a 3和源漏可互换本征区b 4内场强较低,能带弯曲程度较小,因此也不会在源漏可互换本征区a 3和源漏可互换本征区b 4的导带和价带之间产生大量隧穿电子空穴对,因此在源漏可互换本征区a 3和源漏可互换本征区b 4内既形不成大量空穴堆积,也形不成大量电子堆积,晶体管的源漏可互换本征区a 3和源漏可互换本征区b 4均处于高阻状态,即源区和漏区处于高阻状态,因此整个晶体管不会有明显电流流过,器件此时具有优秀的关断特性和亚阈值特性;随着H形栅电极8被施加的电压进一步由平带电压上升至正向偏置状态,此时源漏可互换本征区a 3和源漏可互换本征区b 4内受H形栅电极8场效应作用影响,会出现较大电场强度和较强能带弯曲,因此会发生明显的隧道效应,使得源漏可互换本征区a 3和源漏可互换本征区b 4内形成大量电子空穴对,其中作为源区一端的源漏可互换本征区所产生的空穴会经由该端的重掺杂源漏可互换区排出,所产生的电子会经由受势垒调控栅2控制的单晶硅薄膜1的中间部分所形成的N型区域,流向作为漏区一端的源漏可互换本征区,与作为漏区一端的源漏可互换本征区内由隧道效应所产生的价带空穴发生复合。而作为漏区一端的源漏可互换本征区内由隧道效应所产生的导带电子会经由作为漏区的重掺杂源漏可互换区,与其价带空穴发生复合,通过上述物理过程形成连续的导通电流。由于隧道效应所产生的电子空穴对浓度会随着H形栅电极8所被施加电压的上升而逐步上升,当隧道效应所产生的电子空穴对浓度增加到一定程度时,晶体管由亚阈值状态过渡至正向导通状态。The present invention provides a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor, which has left-right symmetrical structural features, and controls heavy doping by adjusting the voltages of source-drain interchangeable electrode a9 and source-drain interchangeable electrode b10 The source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6 are used as source regions or drain regions to change the tunneling current direction and enable the device to realize the source-drain symmetric interchangeable characteristics of bidirectional tunneling conduction. Taking the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6 as an example of P-type impurities, when the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region When there is a potential difference between the interchangeable regions b and 6, and when the H-shaped gate electrode 8 is in a negative voltage reverse bias state, affected by the field effect of the H-shaped gate, the heavily doped source-drain interchangeable region a5 will flow toward the source-drain interchangeable region The interchangeable intrinsic region a 3 provides holes, and the heavily doped source-drain interchangeable region b 6 provides holes to the source-drain interchangeable intrinsic region b 4 , so the source-drain interchangeable intrinsic region a 3 and the source-drain interchangeable intrinsic region b 4 both produce hole accumulation, so that the source-drain interchangeable intrinsic region a 3 and the source-drain interchangeable intrinsic region b 4 both present a P-type state at this time, and the accumulated The holes make the source-drain interchangeable intrinsic region a3 and the source-drain interchangeable intrinsic region b4 decrease in resistance under the action of the H-shaped gate electrode 8, that is, both the source region and the drain region are in a low-resistance state, but Since the barrier regulating gate 2 always applies a forward voltage, a potential barrier is formed for the holes in the source-drain interchangeable intrinsic region a3 and the source-drain interchangeable intrinsic region b4 on both sides, and the holes on both sides The holes in the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6 also form potential barriers, and are affected by the field effect of the forward voltage applied by the barrier control gate 2, and are affected by The middle part of the single crystal silicon thin film 1 controlled by the barrier control gate 2 will present an N-type semiconductor state, so that the source-drain interchangeable intrinsic region a3 exhibiting P-type characteristics and the single crystal silicon thin film 1 which is N-type at this time The middle part of the transistor forms a reverse-biased PN junction structure under the action of the drain-source voltage. Therefore, when the H-shaped gate electrode 8 is in a negative-voltage reverse-biased state, the transistor as a whole presents a high resistance because of the above-mentioned reverse-biased PN junction structure inside the transistor. Blocking state; as the voltage applied to the H-shaped gate electrode 8 gradually rises from the negative voltage to near the flat-band voltage, the heavily doped source-drain interchangeable region a5 will not contribute to the source-drain interchangeable intrinsic region a3 Provide a large number of holes, the heavily doped source-drain interchangeable region b6 will not provide a large number of holes to the source-drain interchangeable intrinsic region b4, and at the same time because the source-drain interchangeable intrinsic region a3 and source-drain The field strength in the interchangeable intrinsic region b 4 is low, and the degree of energy band bending is small, so it will not be in the conduction band of the source-drain interchangeable intrinsic region a 3 and the source-drain interchangeable intrinsic region b 4 A large number of tunneling electron-hole pairs are generated between the valence band and the source-drain interchangeable intrinsic region a 3 and the source-drain interchangeable intrinsic region b 4. Neither a large amount of hole accumulation nor a large amount of Electron accumulation, the source-drain interchangeable intrinsic region a3 and the source-drain interchangeable intrinsic region b4 of the transistor are both in a high-resistance state, that is, the source region and drain region are in a high-resistance state, so the entire transistor will not have obvious The current flows, and the device has excellent turn-off characteristics and sub-threshold characteristics at this time; as the voltage applied to the H-shaped gate electrode 8 further rises from the flat-band voltage to the forward bias state, the source and drain can be interchanged at this time. Influenced by the field effect of the H-shaped gate electrode 8 in the constitutive region a3 and the source-drain interchangeable intrinsic region b4, there will be a large electric field intensity and strong energy band bending, so an obvious tunnel effect will occur, making the source A large The amount of electron-hole pairs, in which the holes generated by the source-drain interchangeable intrinsic region at one end of the source region will be discharged through the heavily doped source-drain interchangeable region at this end, and the generated electrons will be regulated by the barrier The N-type region formed by the middle part of the monocrystalline silicon thin film 1 controlled by the gate 2 flows to the source-drain interchangeable intrinsic region as one end of the drain region, and the source-drain interchangeable intrinsic region as one end of the drain region is formed by The valence band holes generated by the tunneling effect recombine. The conduction band electrons generated by the tunnel effect in the source-drain interchangeable intrinsic region at one end of the drain region will recombine with the valence band holes through the heavily doped source-drain interchangeable region as the drain region, through the above The physical process forms a continuous conduction current. The concentration of electron-hole pairs generated by the tunnel effect will gradually increase with the increase of the voltage applied to the H-shaped gate electrode 8. When the concentration of electron-hole pairs generated by the tunnel effect increases to a certain extent, the transistor will change from subthreshold to state transitions to the forward conduction state.
由于器件在源漏方向上具有左右对称的结构特征,因此不同于普通的隧穿场效应晶体管,本发明所提出的一种势垒调控式H形栅控双向隧穿晶体管,其源区和漏区可以实现互换功能。Since the device has left-right symmetrical structural features in the source-drain direction, it is different from ordinary tunneling field-effect transistors. The barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor proposed in the present invention has a source region and a drain region The zone can realize the interchange function.
为达到本发明所述的器件功能,本发明提出一种势垒调控式H形栅控双向隧穿晶体管,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 barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor, whose core structural features are:
本发明所述器件为一种势垒调控式H形栅控双向隧穿晶体管,两侧呈对称结构。由势垒调控栅2控制单晶硅薄膜1的中间部分,通过将其设置在特定的固定电压值,对重掺杂源漏可互换区的多数载流子形成势垒,抑制反偏及亚阈值状态下的泄漏电流的大小。势垒调控栅2所控制的单晶硅薄膜1的中间部分与重掺杂源漏可互换区a 5、重掺杂源漏可互换区b 6具有极性相反载流子类型。由于本发明所述器件所具有的对称结构,通过控制源漏可互换电极a 9和源漏可互换电极b 10控制重掺杂源漏可互换区a 5和重掺杂源漏可互换区b 6作为源区或漏区,实现器件源漏可互换的双向开关特性。The device of the present invention is a potential barrier regulating type H-shaped gate-controlled bidirectional tunneling transistor, with symmetrical structures on both sides. The middle part of the single crystal silicon thin film 1 is controlled by the barrier control gate 2, and by setting it at a specific fixed voltage value, a potential barrier is formed for the majority carriers in the heavily doped source-drain interchangeable region, and reverse bias and The magnitude of the leakage current in the subthreshold state. The middle part of the single crystal silicon thin film 1 controlled by the barrier control gate 2 and the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6 have carrier types with opposite polarities. Due to the symmetrical structure of the device of the present invention, the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain can be controlled by controlling the source-drain interchangeable electrode a9 and the source-drain interchangeable electrode b10. The interchangeable area b 6 is used as a source area or a drain area to realize the bidirectional switching characteristic that the source and drain of the device are interchangeable.
本发明所述器件为一种势垒调控式H形栅控双向隧穿晶体管,具有H形栅电极的结构,与栅电极绝缘层7的外侧表面相互接触,并对栅电极绝缘层7形成三面围绕,俯视观看呈现英文大写字母H形结构特征,对单晶硅薄膜1所形成的凹槽形结构的两侧垂直部分的上方部分,即对源漏可互换本征区a 3和源漏可互换本征区b 4具有明显的场效应控制作用,当H形栅电极8处于正偏状态时,对比于平面结构,位于H形栅电极8拐角区域附近的电场强度会得到加强,导致在源漏可互换本征区a 3和源漏可互换本征区b 4内产生载流子的概率在同等栅电压下增大,使得亚阈值摆幅有所下降、正向导通电流有所增大;The device of the present invention is a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor, which has an H-shaped gate electrode structure, is in contact with the outer surface of the gate electrode insulating layer 7, and forms three sides of the gate electrode insulating layer 7. Surrounded by a top view, it presents the characteristic of an English capital letter H-shaped structure. For the upper part of the vertical part on both sides of the groove-shaped structure formed by the single crystal silicon film 1, that is, for the source-drain interchangeable intrinsic region a 3 and the source-drain The interchangeable intrinsic region b4 has an obvious field effect control function. When the H-shaped gate electrode 8 is in the forward biased state, compared with the planar structure, the electric field intensity near the corner area of the H-shaped gate electrode 8 will be strengthened, resulting in The probability of generating carriers in the source-drain interchangeable intrinsic region a3 and the source-drain interchangeable intrinsic region b4 increases at the same gate voltage, so that the subthreshold swing decreases and the forward conduction current has increased;
本发明所提出的一种势垒调控式H形栅控双向隧穿晶体管制备方法的具体制造步骤如下:The specific manufacturing steps of a barrier-regulated H-shaped gate-controlled bidirectional tunneling transistor preparation method proposed by the present invention are as follows:
步骤一:如图4、图5、图6和图7所示,提供一个SOI晶圆,最下方为SOI晶圆的硅衬底12,硅衬底的上面是衬底绝缘层11,衬底绝缘层11的上表面为单晶硅薄膜1,通过光刻或刻蚀工艺,对SOI晶圆上方的单晶硅薄膜1进行刻蚀,除去前后两侧以及中间部分区域的单晶硅薄膜1,形成具有凹槽形结构特征的单晶硅薄膜1;Step 1: As shown in Fig. 4, Fig. 5, Fig. 6 and Fig. 7, an SOI wafer is provided, the bottom is the silicon substrate 12 of the SOI wafer, the top of the silicon substrate is the substrate insulating layer 11, and the substrate The upper surface of the insulating layer 11 is a single crystal silicon thin film 1, and the single crystal silicon thin film 1 above the SOI wafer is etched by photolithography or etching process, and the single crystal silicon thin film 1 on the front and back sides and the middle part are removed , forming a single crystal silicon thin film 1 with groove-shaped structural features;
步骤二:如图8、图9、图10、图11、图12和图13所示,通过氧化或淀积、刻蚀工艺,在单晶硅薄膜1所形成的凹槽形结构的前后外侧表面和凹槽两侧垂直部分的内侧表面及凹槽底部水平部分的上方表面形成栅电极绝缘层7;Step 2: As shown in Fig. 8, Fig. 9, Fig. 10, Fig. 11, Fig. 12 and Fig. 13, through oxidation or deposition and etching process, the front and rear sides of the groove-shaped structure formed by the single crystal silicon film 1 A gate electrode insulating layer 7 is formed on the surface and the inner surface of the vertical part on both sides of the groove and the upper surface of the horizontal part at the bottom of the groove;
步骤三:如图14、图15、图16、图17、图18和图19所示,在SOI晶圆上方淀积绝缘介质,平坦化至表面露出单晶硅薄膜1,初步形成绝缘介质阻挡层13;Step 3: As shown in Fig. 14, Fig. 15, Fig. 16, Fig. 17, Fig. 18 and Fig. 19, an insulating dielectric is deposited on the SOI wafer, planarized until the surface exposes the single crystal silicon film 1, and an insulating dielectric barrier is initially formed layer 13;
步骤四:如图20、图21和图22所示,通过刻蚀工艺,对步骤三中所形成的位于单晶硅薄膜1凹槽结构底部水平部分的前后表面的部分绝缘介质阻挡层13进行刻蚀至露出栅电极绝缘层7,进一步形成绝缘介质阻挡层13;Step 4: As shown in Fig. 20, Fig. 21 and Fig. 22, through an etching process, part of the insulating dielectric barrier layer 13 formed in step 3, which is located on the front and rear surfaces of the horizontal part of the bottom horizontal part of the groove structure of the single crystal silicon film 1 Etching until the gate electrode insulating layer 7 is exposed, and further forming an insulating dielectric barrier layer 13;
步骤五:如图23、图24和图25所示,通过淀积工艺,在SOI晶圆上方淀积金属或多晶硅,平坦化表面至露出单晶硅薄膜1,初步形成势垒调控栅2;Step 5: As shown in Fig. 23, Fig. 24 and Fig. 25, through the deposition process, deposit metal or polysilicon on top of the SOI wafer, planarize the surface until the single crystal silicon film 1 is exposed, and initially form the barrier control gate 2;
步骤六:如图26、图27、图28和图29所示,先通过刻蚀工艺刻蚀掉单晶硅薄膜1所形成的凹槽结构底部水平部分的上方的绝缘介质阻挡层13至露出栅电极绝缘层7,在通过淀积工艺在SOI晶圆上方淀积金属或多晶硅,平坦化表面至露出单晶硅薄膜1,进一步形成势垒调控栅2;Step 6: As shown in Fig. 26, Fig. 27, Fig. 28 and Fig. 29, the insulating dielectric barrier layer 13 above the horizontal part of the bottom of the groove structure formed by the single crystal silicon film 1 is etched away by an etching process to expose The gate electrode insulating layer 7 is deposited metal or polysilicon on the SOI wafer through a deposition process, planarizing the surface to expose the single crystal silicon film 1, and further forming the barrier control gate 2;
步骤七:如图30、图31、图32和图33所示,通过刻蚀工艺刻蚀掉步骤六所形成的势垒调控栅2的上方区域,进一步形成势垒调控栅2;Step 7: As shown in FIG. 30 , FIG. 31 , FIG. 32 and FIG. 33 , the upper region of the barrier regulating gate 2 formed in step 6 is etched away by an etching process, and the barrier regulating gate 2 is further formed;
步骤八:如图34、图35、图36和图37所示,淀积工艺,在SOI晶圆上方淀积绝缘介质,平坦化表面至露出单晶硅薄膜1,进一步形成绝缘介质阻挡层13;Step 8: As shown in Fig. 34, Fig. 35, Fig. 36 and Fig. 37, the deposition process is to deposit an insulating dielectric on the SOI wafer, planarize the surface to expose the single crystal silicon film 1, and further form an insulating dielectric barrier layer 13 ;
步骤九:如图38、图39、图40和图41所示,通过光刻或刻蚀工艺,对在步骤八中所形成的部分绝缘介质阻挡层13进行部分刻蚀,再在SOI晶圆上方淀积金属或多晶硅,平坦化表面至露出单晶硅薄膜1,形成H形栅电极8;Step 9: As shown in FIG. 38, FIG. 39, FIG. 40 and FIG. 41, through a photolithography or etching process, partially etch the part of the insulating dielectric barrier layer 13 formed in step 8, and then place it on the SOI wafer Deposit metal or polysilicon on the top, planarize the surface to expose the single crystal silicon film 1, and form an H-shaped gate electrode 8;
步骤十:如图42、图43和图44所示,通过离子注入工艺,单晶硅薄膜1所形成的凹槽结构的两侧垂直部分上表面的中间外侧部分进行掺杂,形成重掺杂源漏可互换区a 5和重掺杂源漏可互换区b 6;Step 10: As shown in Fig. 42, Fig. 43 and Fig. 44, through the ion implantation process, the middle and outer parts of the upper surface of the vertical parts on both sides of the groove structure formed by the single crystal silicon film 1 are doped to form heavily doped Source-drain interchangeable region a5 and heavily doped source-drain interchangeable region b6;
步骤十一:如图45、图46和图47所示,通过淀积工艺,在SOI晶圆上方淀积绝缘介质,形成其余部分的绝缘介质阻挡层13;平坦化表面后通过刻蚀工艺去除重掺杂源漏可互换区a5和重掺杂源漏可互换区b 6上方的绝缘介质阻挡层13至露出重掺杂源漏可互换区a 5和重掺杂源漏可互换区b 6的上表面,再通过淀积工艺向刻蚀形成的通孔中注入金属至通孔被完全填充,最后将表面平坦化处理,形成源漏可互换电极a 9和源漏可互换电极b 10。Step 11: As shown in Fig. 45, Fig. 46 and Fig. 47, an insulating dielectric is deposited on the SOI wafer through a deposition process to form the rest of the insulating dielectric barrier layer 13; after the surface is planarized, it is removed by an etching process The insulating dielectric barrier layer 13 above the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6 exposes the heavily doped source-drain interchangeable region a5 and the heavily doped source-drain interchangeable region b6. Replace the upper surface of the region b6, and then inject metal into the through hole formed by etching through the deposition process until the through hole is completely filled, and finally planarize the surface to form the source-drain interchangeable electrode a9 and the source-drain interchangeable electrode a9. Interchange electrode b 10.
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Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20040164342A1 (en) * | 2001-08-30 | 2004-08-26 | Micron Technology, Inc. | Integrated circuit memory device and method |
| CN1851903A (en) * | 2005-04-22 | 2006-10-25 | 韩国科学技术院 | Multi-bit non-volatile memory having dual gates, method of manufacturing the same, and multi-bit cell operating method |
-
2017
- 2017-10-31 CN CN201711050865.9A patent/CN107819029B/en active Active
Patent Citations (2)
| Publication number | Priority date | Publication date | Assignee | Title |
|---|---|---|---|---|
| US20040164342A1 (en) * | 2001-08-30 | 2004-08-26 | Micron Technology, Inc. | Integrated circuit memory device and method |
| CN1851903A (en) * | 2005-04-22 | 2006-10-25 | 韩国科学技术院 | Multi-bit non-volatile memory having dual gates, method of manufacturing the same, and multi-bit cell operating method |
Non-Patent Citations (1)
| Title |
|---|
| 杨光锐等: "具有辅助栅的新型低泄露U沟道无结场效应晶体管", 《科技创新导报》 * |
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