{"title":"Split-p-GaN Gate HEMT With Suppressed Negative Vth Shift and Enhanced Robustness Against False Turn-On","authors":"Yunhong Lao;Jin Wei;Maojun Wang;Jingjing Yu;Zetao Fan;Junjie Yang;Jiawei Cui;Teng Li;Han Yang;Muqin Nuo;Qimeng Jiang;Gaofei Tang;Bo Shen","doi":"10.1109/LED.2025.3535601","DOIUrl":null,"url":null,"abstract":"In the development of the Schottky-type p-GaN gate HEMT, the instable <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> is always a highlighted problem. Under high <inline-formula> <tex-math>${V}_{\\text {DS}}$ </tex-math></inline-formula> bias, the potential of the floating p-GaN can be raised by the gate/drain coupled barrier lowering (GDCBL) effect, inducing a noticeable negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift. During the fast switching operation, the negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift severely aggravates the false turn-on problem. In this work, a split-p-GaN gate HEMT (SPG-HEMT) is demonstrated to effectively suppress the drain-induced negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift, enhancing the robustness against false turn-on. At <inline-formula> <tex-math>${V}_{\\text {DS}} =100$ </tex-math></inline-formula> V, the conventional p-GaN gate HEMT (Conv-HEMT) suffers a negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift of −0.33 V, while the SPG-HEMT exhibits only a minimal <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift of −0.07 V. In the SPG-HEMT, the GDCBL effect takes place only for the p-GaN near the drain side (p<inline-formula> <tex-math>$_{{2}}\\text {)}$ </tex-math></inline-formula>; the p-GaN near the source (p<inline-formula> <tex-math>$_{{1}}\\text {)}$ </tex-math></inline-formula> is isolated from p2 via the gate/p-GaN Schottky junctions, and the influence of drain bias upon p1 is shielded by p2. Then, the impact of negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift on false turn-on is evaluated by a half-bridge switching circuit. Due to the obvious negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift, the Conv-HEMT is falsely turned on when the <inline-formula> <tex-math>${V}_{\\text {GS}}$ </tex-math></inline-formula> ringing peak is still much lower than the static threshold voltage (<inline-formula> <tex-math>${V}_{{\\mathrm {th0}}})$ </tex-math></inline-formula>. In contrast, the SPG-HEMT starts to show false turn-on signal only when the <inline-formula> <tex-math>${V}_{\\text {GS}}$ </tex-math></inline-formula> ringing peak is near <inline-formula> <tex-math>${V}_{{\\mathrm {th0}}}$ </tex-math></inline-formula>. Overall, the unique device structure of the SPG-HEMT leads to a negligible negative <inline-formula> <tex-math>${V}_{\\text {th}}$ </tex-math></inline-formula> shift and enhances the robustness against false turn-on.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"46 4","pages":"628-631"},"PeriodicalIF":4.1000,"publicationDate":"2025-01-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"IEEE Electron Device Letters","FirstCategoryId":"5","ListUrlMain":"https://ieeexplore.ieee.org/document/10856268/","RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"Q2","JCRName":"ENGINEERING, ELECTRICAL & ELECTRONIC","Score":null,"Total":0}
引用次数: 0
Abstract
In the development of the Schottky-type p-GaN gate HEMT, the instable ${V}_{\text {th}}$ is always a highlighted problem. Under high ${V}_{\text {DS}}$ bias, the potential of the floating p-GaN can be raised by the gate/drain coupled barrier lowering (GDCBL) effect, inducing a noticeable negative ${V}_{\text {th}}$ shift. During the fast switching operation, the negative ${V}_{\text {th}}$ shift severely aggravates the false turn-on problem. In this work, a split-p-GaN gate HEMT (SPG-HEMT) is demonstrated to effectively suppress the drain-induced negative ${V}_{\text {th}}$ shift, enhancing the robustness against false turn-on. At ${V}_{\text {DS}} =100$ V, the conventional p-GaN gate HEMT (Conv-HEMT) suffers a negative ${V}_{\text {th}}$ shift of −0.33 V, while the SPG-HEMT exhibits only a minimal ${V}_{\text {th}}$ shift of −0.07 V. In the SPG-HEMT, the GDCBL effect takes place only for the p-GaN near the drain side (p$_{{2}}\text {)}$ ; the p-GaN near the source (p$_{{1}}\text {)}$ is isolated from p2 via the gate/p-GaN Schottky junctions, and the influence of drain bias upon p1 is shielded by p2. Then, the impact of negative ${V}_{\text {th}}$ shift on false turn-on is evaluated by a half-bridge switching circuit. Due to the obvious negative ${V}_{\text {th}}$ shift, the Conv-HEMT is falsely turned on when the ${V}_{\text {GS}}$ ringing peak is still much lower than the static threshold voltage (${V}_{{\mathrm {th0}}})$ . In contrast, the SPG-HEMT starts to show false turn-on signal only when the ${V}_{\text {GS}}$ ringing peak is near ${V}_{{\mathrm {th0}}}$ . Overall, the unique device structure of the SPG-HEMT leads to a negligible negative ${V}_{\text {th}}$ shift and enhances the robustness against false turn-on.
期刊介绍:
IEEE Electron Device Letters publishes original and significant contributions relating to the theory, modeling, design, performance and reliability of electron and ion integrated circuit devices and interconnects, involving insulators, metals, organic materials, micro-plasmas, semiconductors, quantum-effect structures, vacuum devices, and emerging materials with applications in bioelectronics, biomedical electronics, computation, communications, displays, microelectromechanics, imaging, micro-actuators, nanoelectronics, optoelectronics, photovoltaics, power ICs and micro-sensors.