High-voltage super-junction lateral double-diffused metal-oxide semiconductor with a partial lightly doped pillar

A novel super-junction lateral double-diffused metal-oxide semiconductor(SJ-LDMOS) with a partial lightly doped P pillar(PD) is proposed.Firstly,the reduction in the partial P pillar charges ensures the charge balance and suppresses the substrate-assisted depletion effect.Secondly,the new electric field peak produced by the P/P-junction modulates the surface electric field distribution.Both of these result in a high breakdown voltage(BV).In addition,due to the same conduction paths,the specific on-resistance(R on,sp) of the PD SJ-LDMOS is approximately identical to the conventional SJ-LDMOS.Simulation results indicate that the average value of the surface lateral electric field of the PD SJ-LDMOS reaches 20V/μm at a 15μm drift length,resulting in a BV of 300V.     

具有纵向辅助耗尽衬底层的新型横向双扩散金属氧化物半导体场效应晶体管

为了优化横向双扩散金属氧化物半导体场效应晶体管(lateral double-diffused MOSFET,LDMOS)的击穿特性及器件性能,在传统LDMOS结构的基础上,提出了一种具有纵向辅助耗尽衬底层(assisted depletesubstrate layer,ADSL)的新型LDMOS.新加入的ADSL层使得漏端下方的纵向耗尽区大幅向衬底扩展,从而利用电场调制效应在ADSL层底部引入新的电场峰,使纵向电场得到优化,同时横向表面电场也因为电场调制效应而得到了优化.通过ISE仿真表明,当传统LDMOS与ADSL LDMOS的漂移区长度都是70μm时,击穿电压由462 V增大到897 V,提高了94%左右,并且优值也从0.55 MW/cm~2提升到1.24 MW/cm~2,提升了125%.因此,新结构ADSL LDMOS的器件性能较传统LDMOS有了极大的提升.进一步对ADSL层进行分区掺杂优化,在新结构的基础上,击穿电压在双分区时上升到938 V,三分区时为947 V.     

阶梯氧化层新型折叠硅横向双扩散功率器件

为了设计功率集成电路所需的低功耗横向功率器件, 提出了一种具有阶梯氧化层折叠硅横向双扩散金属-氧化物-半导体(step oxide folding LDMOS, SOFLDMOS)新结构. 这种结构将阶梯氧化层覆盖在具有周期分布的折叠硅表面, 利用阶梯氧化层的电场调制效应, 通过在表面电场分布中引入新的电场峰而使表面电场分布均匀, 提高了器件的耐压范围, 解决了文献提出的折叠积累型横向双扩散金属-氧化物-半导体器件击穿电压受限的问题. 通过三维仿真软件ISE分析获得, SOFLDMOS 结构打破了硅的极限关系, 充分利用了电场调制效应、多数载流子积累和硅表面导电区倍增效应, 漏极饱和电流比一般LDMOS 提高3.4倍左右, 可以在62 V左右的反向击穿电压条件下, 获得0.74 mΩ·cm²超低的比导通电阻, 远低于传统LDMOS相同击穿电压下2.0 mΩ·cm²比导通电阻, 为实现低压功率集成电路对低功耗横向功率器件的要求提供了一种可选的方案.     

A super-junction SOI-LDMOS with low resistance electron channel

A novel super-junction LDMOS with low resistance channel(LRC), named LRC-LDMOS based on the silicon-oninsulator(SOI) technology is proposed. The LRC is highly doped on the surface of the drift region, which can significantly reduce the specific on resistance(Ron,sp) in forward conduction. The charge compensation between the LRC, N-pillar,and P-pillar of the super-junction are adjusted to satisfy the charge balance, which can completely deplete the whole drift,thus the breakdown voltage(BV) is enhanced in reverse blocking. The three-dimensional(3 D) simulation results show that the BV and R_(on,sp) of the device can reach 253 V and 15.5 mΩ·cm~2, respectively, and the Baliga's figure of merit(FOM = BV~2/R_(on,sp)) of 4.1 MW/cm~2 is achieved, breaking through the silicon limit.     

新型缓冲层分区电场调制横向双扩散超结功率器件

为了突破传统横向双扩散金属-氧化物-半导体器件(lateral double-diffused MOSFET)击穿电压与比导通电阻的极限关系,本文在缓冲层横向双扩散超结功率器件(super junction LDMOS-SJ LDMOS)结构基础上,提出了具有缓冲层分区新型SJ-LDMOS结构.新结构利用电场调制效应将分区缓冲层产生的电场峰引入超结(super junction)表面而优化了SJ-LDMOS的表面电场分布,缓解了横向LDMOS器件由于受纵向电场影响使横向电场分布不均匀、横向单位耐压量低的问题.利用仿真分析软件ISE分析表明,优化条件下,当缓冲层分区为3时,提出的缓冲层分区SJ-LDMOS表面电场最优,击穿电压达到饱和时较一般LDMOS结构提高了50%左右,较缓冲层SJ-LDMOS结构提高了32%左右,横向单位耐压量达到18.48 V/μm.击穿电压为382 V的缓冲层分区SJ-LDMOS,比导通电阻为25.6 mΩ·cm2,突破了一般LDMOS击穿电压为254 V时比导通电阻为71.8 mΩ·cm2的极限关系.     

Terminal-optimized 700-V LDMOS with improved breakdown voltage and ESD robustness

A novel terminal-optimized triple RESURF LDMOS(TOTR-LDMOS) is proposed and verified in a 0.25-μm bipolarCMOS-DMOS(BCD) process. By introducing a low concentration region to the terminal region, the surface electric field of the TOTR-LDMOS decreases, helping to improve the breakdown voltage(BV) and electrostatic discharge(ESD) robustness. Both traditional LDMOS and TOTR-LDMOS are fabricated and investigated by transmission line pulse(TLP) tests,direct current(DC) tests, and TCAD simulations. The results show that comparing with the traditional LDMOS, the BV of the TOTR-LDMOS increases from 755 V to 817 V without affecting the specific on-resistance(R_(on,sp)) of 6.99 ?·mm~2.Meanwhile, the ESD robustness of the TOTR-LDMOS increases by 147%. The TOTR-LDMOS exhibits an excellent performance among the present 700-V LDMOS devices.     

Fast-switching SOI-LIGBT with compound dielectric buried layer and assistant-depletion trench

A lateral insulated gate bipolar transistor (LIGBT) based on silicon-on-insulator (SOI) structure is proposed and investigated. This device features a compound dielectric buried layer (CDBL) and an assistant-depletion trench (ADT). The CDBL is employed to introduce two high electric field peaks that optimize the electric field distributions and that, under the same breakdown voltage (BV) condition, allow the CDBL to acquire a drift region of shorter length and a smaller number of stored carriers. Reducing their numbers helps in fast-switching. Furthermore, the ADT contributes to the rapid extraction of the stored carriers from the drift region as well as the formation of an additional heat-flow channel. The simulation results show that the BV of the proposed LIGBT is increased by 113% compared with the conventional SOI LIGBT of the same length L_D. Contrastingly, the length of the drift region of the proposed device (11.2 μ) is about one third that of a traditional device (33 μ) with the same BV of 141 V. Therefore, the turn-off loss (E_OFF) of the CDBL SOI LIGBT is decreased by 88.7% compared with a conventional SOI LIGBT when the forward voltage drop (V_F) is 1.64 V. Moreover, the short-circuit failure time of the proposed device is 45% longer than that of the conventional SOI LIGBT. Therefor, the proposed CDBL SOI LIGBT exhibits a better V_F-E_OFF tradeoff and an improved short-circuit robustness.     

Partial-SOI high voltage laterally double-diffused MOS with a partially buried n~+-layer

A novel partial silicon-on-insulator laterally double-diffused metal-oxide-semiconductor transistor （PSOI LDMOS） with a thin buried oxide layer is proposed in this paper. The key structure feature of the device is an n＋-layer, which is partially buried on the bottom interface of the top silicon layer （PBNL PSOI LDMOS）. The undepleted interface n＋-layer leads to plenty of positive charges accumulated on the interface, which will modulate the distributions of the lateral and vertical electric fields for the device, resulting in a high breakdown voltage （BV）. With the same thickness values of the top silicon layer （10 p.m） and buried oxide layer （0.375 μm）, the BV of the PBNL PSOI LDMOS increases to 432 V from 285 V of the conventional PSOI LDMOS, which is improved by 51.6%.     

Analysis of the breakdown mechanism for an ultra high voltage high-side thin layer silicon-on-insulator p-channel lateral double-diffused metal\ben oxide semiconductor

This paper discusses the breakdown mechanism and proposes a new simulation and test method of breakdown voltage (BV) for an ultra-high-voltage (UHV) high-side thin layer silicon-on-insulator (SOI) p-channel low-density metal-oxide semiconductor (LDMOS). Compared with the conventional simulation method, the new one is more accordant with the actual conditions of a device that can be used in the high voltage circuit. The BV of the SOI p-channel LDMOS can be properly represented and the effect of reduced bulk field can be revealed by employing the new simulation method. Simulation results show that the off-state (on-state) BV of the SOI p-channel LDMOS can reach 741 (620) V in the 3-μm-thick buried oxide layer, 50-μm-length drift region, and at -400 V back-gate voltage, enabling the device to be used in a 400 V UHV integrated circuit.     

具有纵向漏极场板的低导通电阻绝缘体上硅横向双扩散金属氧化物半导体器件新结构

为降低绝缘体上硅(SOI)横向双扩散金属氧化物半导体(LDMOS)器件的导通电阻,同时提高器件击穿电压,提出了一种具有纵向漏极场板的低导通电阻槽栅槽漏SOI-LDMOS器件新结构.该结构特征为采用了槽栅槽漏结构,在纵向上扩展了电流传导区域,在横向上缩短了电流传导路径,降低了器件导通电阻;漏端采用了纵向漏极场板,该场板对漏端下方的电场进行了调制,从而减弱了漏极末端的高电场,提高了器件的击穿电压.利用二维数值仿真软件MEDICI对新结构与具有相同器件尺寸的传统SOI结构、槽栅SOI结构、槽栅槽漏SOI结构进行了比较.结果表明:在保证各自最高优值的条件下,与这三种结构相比,新结构的比导通电阻分别降低了53%,23%和提高了87%,击穿电压则分别提高了4%、降低了9%、提高了45%.比较四种结构的优值,具有纵向漏极场板的槽栅槽漏SOI结构优值最高,这表明在四种结构中新结构保持了较低导通电阻,同时又具有较高的击穿电压.     

具有N型缓冲层REBULF Super Junction LDMOS

针对功率集成电路对低损耗LDMOS (lateral double-diffused MOSFET)类器件的要求,在N型缓冲层super junction LDMOS (buffered SJ-LDMOS)结构基础上, 提出了一种具有N型缓冲层的REBULF (reduced BULk field) super junction LDMOS结构. 这种结构不但消除了N沟道SJ-LDMOS由于P型衬底带来的衬底辅助耗尽效应问题, 使super junction的N区和P区电荷完全补偿, 而且同时利用REBULF的部分N型缓冲层电场调制效应, 在表面电场分布中引入新的电场峰而使横向表面电场分布均匀, 提高了器件的击穿电压. 通过优化部分N型埋层的位置和参数, 利用仿真软件ISE分析表明, 新型REBULF SJ-LDMOS 的击穿电压较一般LDMOS提高了49%左右, 较文献提出的buffered SJ-LDMOS结构提高了30%左右. 关键词： lateral double-diffused MOSFET super junction 击穿电压 表面电场     

Compound buried layer SOI high voltage device with a step buried oxide

A silicon-on-insulator (SOI) high performance lateral double-diffusion metal oxide semiconductor (LDMOS) on a compound buried layer (CBL) with a step buried oxide (SBO CBL SOI) is proposed.The step buried oxide locates holes in the top interface of the upper buried oxide (UBO) layer.Furthermore,holes with high density are collected in the interface between the polysilicon layer and the lower buried oxide (LBO) layer.Consequently,the electric fields in both the thin LBO and the thick UBO are enhanced by these holes,leading to an improved breakdown voltage.The breakdown voltage of the SBO CBL SOI LDMOS increases to 847 V from the 477 V of a conventional SOI with the same thicknesses of SOI layer and the buried oxide layer.Moreover,SBO CBL SOI can also reduce the self-heating effect.     

Investigation of laterally single-diffused metal oxide semiconductor (LSMOS) field effect transistor

We propose a distinct approach to implement a laterally single diffused metal-oxide-semiconductor (LSMOS) FET with only one impurity doped p-n junction. In the LSMOS, a single p-n junction is first created using lateral dopant diffusion. The channel is formed in the p region of the p-n junction and the n region acts as the drift region. Two distinct metals of different work function are used to form the “n⁺” source/drain regions and “p⁺” body contact using the charge plasma concept. We demonstrate that the LSMOS is similar in performance to a laterally double diffused metal-oxide-semiconductor (LDMOS) although it has only one impurity doped p-n junction. The LSMOS exhibits a breakdown voltage of ∼50.0 V, an average ON-resistance of 48.7 mΩ-mm² and a peak transconductance of 53.6 μS/μm similar to that of a comparable LDMOS.     

具有部分本征GaN帽层新型AlGaN/GaN高电子迁移率晶体管特性分析

为了优化传统Al GaN/GaN高电子迁移率晶体管(high electron mobility transistors,HEMTs)器件的表面电场,提高击穿电压,本文提出了一种具有部分本征GaN帽层的新型Al GaN/GaN HEMTs器件结构.新型结构通过在Al GaN势垒层顶部、栅电极到漏电极的漂移区之间引入部分本征GaN帽层,由于本征GaN帽层和Al GaN势垒层界面处的极化效应,降低了沟道二维电子气(two dimensional electron gas,2DEG)的浓度,形成了栅边缘低浓度2DEG区域,使得沟道2DEG浓度分区,由均匀分布变为阶梯分布.通过调制沟道2DEG的浓度分布,从而调制了Al GaN/GaN HEMTs器件的表面电场.利用电场调制效应,产生了新的电场峰,且有效降低了栅边缘的高峰电场,Al GaN/GaN HEMTs器件的表面电场分布更加均匀.利用ISE-TCAD软件仿真分析得出:通过设计一定厚度和长度的本征GaN帽层,Al GaN/GaN HEMTs器件的击穿电压从传统结构的427 V提高到新型结构的960 V.由于沟道2DEG浓度减小,沟道电阻增加,使得新型Al GaN/GaN HEMTs器件的最大输出电流减小了9.2%,截止频率几乎保持不变,而最大振荡频率提高了12%.     

Modeling of a triple reduced surface field silicon-on-insulator lateral double-diffused metal–oxide–semiconductor field-effect transistor with low on-state resistance

An analytical model for a novel triple reduced surface field(RESURF) silicon-on-insulator(SOI) lateral doublediffused metal–oxide–semiconductor(LDMOS) field effect transistor with n-type top(N-top) layer, which can obtain a low on-state resistance, is proposed in this paper. The analytical model for surface potential and electric field distributions of the novel triple RESURF SOI LDMOS is presented by solving the two-dimensional(2D) Poisson's equation, which can also be applied to single, double and conventional triple RESURF SOI structures. The breakdown voltage(BV) is formulized to quantify the breakdown characteristic. Besides, the optimal integrated charge of N-top layer(Q_(ntop)) is derived, which can give guidance for doping the N-top layer. All the analytical results are well verified by numerical simulation results,showing the validity of the presented model. Hence, the proposed model can be a good tool for the device designers to provide accurate first-order design schemes and physical insights into the high voltage triple RESURF SOI device with N-top layer.     

A novel partial SOI LDMOSFET with a trench and buried P layer for breakdown voltage improvement

In this paper for the first time, a partial silicon-on-insulator (PSOI) lateral double-diffused metal-oxide-semiconductor-field-effect-transistor (LDMOSFET) is proposed with a novel trench which improves breakdown voltage. The introduced trench in the partial buried oxide enhances peak of the electric field and is positioned in the drain side of the drift region to maximize breakdown voltage. We demonstrate that the electric field is modified by producing two additional electric field peaks, which decrease the common peaks near the drain and gate junctions in the trench-partial-silicon-on-insulator (T-PSOI) structure. Hence, a more uniform electric field is obtained. Two dimensional (2D) simulations show that the breakdown voltage of T-PSOI is nearly 64% higher in comparison with partial silicon on insulator (PSOI) structure and alleviate self heating effect approximately 9% and 15% in comparison with its conventional PSOI (C-PSOI) and conventional SOI (C-SOI) counterparts respectively. In addition the current of the T-PSOI, C-PSOI, conventional SOI (C-SOI), and fully depleted conventional SOI (FC-SOI) structures are 90, 82, 74, and 44 μA, respectively for a drain–source voltage V_DS = 30 V and gate–source voltage V_GS = 10 V.     

A 4H-SiC trench MOSFET structure with wrap N-type pillar for low oxide field and enhanced switching performance

An optimized silicon carbide (SiC) trench metal-oxide-semiconductor field-effect transistor (MOSFET) structure with side-wall p-type pillar (p-pillar) and wrap n-type pillar (n-pillar) in the n-drain was investigated by utilizing Silvaco TCAD simulations. The optimized structure mainly includes a p$+$ buried region, a light n-type current spreading layer (CSL), a p-type pillar region, and a wrapping n-type pillar region at the right and bottom of the p-pillar. The improved structure is named as SNPPT-MOS. The side-wall p-pillar region could better relieve the high electric field around the p$+$ shielding region and the gate oxide in the off-state mode. The wrapping n-pillar region and CSL can also effectively reduce the specific on-resistance ($R_{rm on,sp}$). As a result, the SNPPT-MOS structure exhibits that the figure of merit (FoM) related to the breakdown voltage ($V_{rm BR}$) and $R_{rm on,sp}$ ($V_{rm BR}^{2}R_{rm on,sp}$) of the SNPPT-MOS is improved by 44.5%, in comparison to that of the conventional trench gate SJ MOSFET (full-SJ-MOS). In addition, the SNPPT-MOS structure achieves a much faster-witching speed than the full-SJ-MOS, and the result indicates an appreciable reduction in the switching energy loss.