Wenhui Wang;Zelin Yuan;Haoran Peng;Panpan Zhang;Yida Li
{"title":"Quantifying the Contact Resistance Components in Oxide Thin-Film Transistor","authors":"Wenhui Wang;Zelin Yuan;Haoran Peng;Panpan Zhang;Yida Li","doi":"10.1109/LED.2026.3719158","DOIUrl":"https://doi.org/10.1109/LED.2026.3719158","url":null,"abstract":"Understanding the contact resistance (<inline-formula> <tex-math>${R}_{C}text {)}$ </tex-math></inline-formula> of back-end-of-line (BEOL) compatible oxide thin-film transistors (TFTs) is critical for drive current optimization especially in advanced technology node. Here, we elucidate the contributions of <inline-formula> <tex-math>${R}_{C}$ </tex-math></inline-formula> in an indium–gallium–zinc oxide (IGZO) TFT by integrating the transfer length method (TLM) and contact-end-resistance (CER) model, supported by physical and material characterization of the TFT, where <inline-formula> <tex-math>${R}_{C}$ </tex-math></inline-formula> is divided into the Schottky barrier resistance (<inline-formula> <tex-math>${R}_{textit {SC}}text {)}$ </tex-math></inline-formula>, the effective interlayer resistance (<inline-formula> <tex-math>${R}_{textit {Int}}text {)}$ </tex-math></inline-formula>, and the resistance of IGZO beneath the contacts (<inline-formula> <tex-math>${R}_{textit {IGZO}}text {)}$ </tex-math></inline-formula>. Using our fabricated IGZO TFT as a test vehicle, we show that the <inline-formula> <tex-math>${R}_{textit {IGZO}}$ </tex-math></inline-formula> represents around two-thirds of the total <inline-formula> <tex-math>${R}_{C}$ </tex-math></inline-formula> and a significant one-third contributed by the interfacial contact layer, with a negligible <inline-formula> <tex-math>${R}_{textit {SC}}$ </tex-math></inline-formula>. By decomposing the <inline-formula> <tex-math>${R}_{C}$ </tex-math></inline-formula> components, they can be separately addressed for device optimization, thus guiding device architecture or process design for future monolithic three-dimensional chip.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2055-2058"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072266","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Munhyeon Kim;Woohyun Lee;Junhyeok Kim;Jae-Joon Kim
{"title":"High-Density 3-D-DRAM Architecture With Folded Capacitor for Sub-10-nm Scaling","authors":"Munhyeon Kim;Woohyun Lee;Junhyeok Kim;Jae-Joon Kim","doi":"10.1109/LED.2026.3715518","DOIUrl":"https://doi.org/10.1109/LED.2026.3715518","url":null,"abstract":"In this letter, a novel 3D-DRAM process architecture based on a folded capacitor is proposed to enhance the bit-cell density of 3D-DRAM, one of the most promising candidates for sub-10 nm DRAM technology nodes. This work comprehensively introduces a manufacturable solution that includes bit-cell layout design, structural configuration, and a process integration scheme, ensuring design-to-fab applicability. To conduct a rigorous evaluation, structural characteristics of the proposed memory cell are precisely calibrated through Technology Computer-Aided Design (TCAD) simulations and BSIM-CMG modeling, using silicon-verified hardware data. As a result, the proposed cell exceeds a <inline-formula> <tex-math>${3}.{3}times $ </tex-math></inline-formula> increase in storage capacitance (<inline-formula> <tex-math>${C}_{text {S}}$ </tex-math></inline-formula>) within the same footprint compared to state-of-the-art 3D-DRAM with horizontal capacitor. Moreover, it secures over a 28% improvement in bit-cell density within the operational margin that guarantees reliable memory performance, highlighting its potential as a next-generation DRAM architecture.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2003-2006"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072273","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Duo Xu;Shaomeng Wang;Zhanliang Wang;Zhigang Lu;Zhaoyun Duan;Yubin Gong
{"title":"Emittance-Limited Beam Radius of Pencil Beams in Terahertz Vacuum Electron Devices","authors":"Duo Xu;Shaomeng Wang;Zhanliang Wang;Zhigang Lu;Zhaoyun Duan;Yubin Gong","doi":"10.1109/LED.2026.3719330","DOIUrl":"https://doi.org/10.1109/LED.2026.3719330","url":null,"abstract":"As vacuum electron devices (VEDs) push toward the terahertz band, the interaction-circuit beam tunnel must shrink with frequency, and the transverse dimension of the electron beam becomes increasingly affected by emittance. To estimate the minimum achievable beam radius (MABR) of pencil beams in terahertz VEDs, we perform numerical simulations of a 20-kV solenoid-confined pencil beam under idealized injection and focusing conditions, scanning magnetic field 0.3–0.8 T, normalized rms emittance 1–200 nm, and beam current 5–30 mA. Across the full scan, the MABR is a universal function of a single dimensionless space-charge-to-emittance ratio: it decreases from about 3.1 times the matched rms envelope radius in the emittance-dominated limit to about 2.2 times in the space-charge-dominated limit. In the emittance-dominated regime relevant to terahertz operation, the matched radius—and hence the MABR—is governed primarily by emittance and magnetic field rather than by beam current or voltage.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2103-2106"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072287","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Dong Min Kim;Yu Bin Kim;Sung Ho Kim;Shivam Kumar Gautam;Hi-Deok Lee
{"title":"Reliable Bi-Layer HfO2/Zr-Doped ZnO Memristive Synaptic Devices","authors":"Dong Min Kim;Yu Bin Kim;Sung Ho Kim;Shivam Kumar Gautam;Hi-Deok Lee","doi":"10.1109/LED.2026.3722740","DOIUrl":"https://doi.org/10.1109/LED.2026.3722740","url":null,"abstract":"Oxide-based memristive synaptic devices are promising hardware elements for neuromorphic computing, but stochastic resistive switching caused by uncontrolled defect distributions and localized conductive paths remains a critical challenge. Here, we demonstrate Zr-doped ZnO memristive synaptic devices fabricated using an atomic layer deposition (ALD) super-cycle process to regulate both defect states and surface morphology. X-ray photoelectron spectroscopy revealed a decrease in the V<sub>O</sub>-related O 1s component from 34.9% to 23.2%, while atomic force microscopy showed a reduction in RMS surface roughness from 0.7532 to 0.2603 nm with less distinguishable surface-grain features. These results suggest that Zr incorporation suppresses V<sub>O</sub>-related defects and reduces grain-boundary-assisted localized conduction. Compared with the undoped device, the Zr-doped device exhibited improved switching uniformity, reduced resistance-state variation, stable pulse endurance, and retention for over <inline-formula> <tex-math>${10}^{{4}}$ </tex-math></inline-formula> s at 25, 50, and <inline-formula> <tex-math>$75~^{circ }$ </tex-math></inline-formula>C. The regulated defect distribution and surface morphology enabled gradual and reproducible conductance modulation during long-term potentiation and depression, resulting in improved synaptic linearity. Neural network simulations using experimentally extracted LTP/LTD nonlinearity parameters further demonstrated enhanced recognition accuracy in ANN and CNN classification tasks.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2115-2118"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072297","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"4-Transistor IGZO Ternary Content Addressable Memory Enabling Large-Scale Array Integration for In-Memory Computing","authors":"Taewon Seo;Taejun Ha;Seunghyun Son;Sunmean Kim;Yoonyoung Chung","doi":"10.1109/LED.2026.3725692","DOIUrl":"https://doi.org/10.1109/LED.2026.3725692","url":null,"abstract":"We report a 4-transistor (4T) Ternary Content Addressable Memory (TCAM) that significantly reduces the physical footprint by employing dual-gate IGZO transistors. High-density TCAMs are essential components for memory augmented neural networks and advanced computing systems; however, the large physical footprint remains a significant limitation in conventional designs. The proposed TCAM unit cell adopts a simplified structure, reducing the transistor count to four, which is substantially lower than previous SRAM-based (16T) and oxide semiconductor-based (6T) counterparts. Moreover, connecting the search line directly to the gate electrode effectively mitigates IR drop, enhancing the design’s suitability for large-scale memory applications. Experimental results validate the proposed design, demonstrating accurate Hamming distance computations (155.9 nA/bit), high endurance (<inline-formula> <tex-math>$gt$ </tex-math></inline-formula><inline-formula> <tex-math>$10^{{10}}$ </tex-math></inline-formula> cycles), and fast operation with 350 ps search latency and 220 ns write time.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2015-2018"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072313","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Experimental Demonstration of Nonlinear Photoconductive Gain in N-Doped β-Ga2O3 Devices","authors":"Vikash K. Jangir;Sudip K. Mazumder","doi":"10.1109/LED.2026.3721486","DOIUrl":"https://doi.org/10.1109/LED.2026.3721486","url":null,"abstract":"In this Letter, we report field-tunable nonlinear photoconductive gain in vertical <inline-formula> <tex-math>$beta $ </tex-math></inline-formula>-Ga<sub>2</sub>O<sub>3</sub> photoconductive detectors under sub-bandgap visible-light excitation. Devices fabricated on a 5.6-<inline-formula> <tex-math>$mu $ </tex-math></inline-formula>m-thick nitrogen-doped semi-insulating <inline-formula> <tex-math>$beta $ </tex-math></inline-formula>-Ga<sub>2</sub>O<sub>3</sub> epilayer grown on a conductive Sn-doped substrate were characterized under 445-nm continuous-wave illumination. A distinct transition from linear to nonlinear photoconductive behavior was observed near 325–350 V, corresponding to a nominal average threshold electric field of <bold>~</b> 0.58-0.63 MV/cm, with the photocurrent subsequently increasing by more than 20-fold and reaching approximately <inline-formula> <tex-math>$475~mu $ </tex-math></inline-formula>A at 435–445 V. Complementary TCAD simulations reveal high local electric fields and a rapid increase in the impact-ionization generation rate at high bias, suggesting a possible contribution from impact-ionization-assisted carrier multiplication to the observed gain.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2083-2086"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072321","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Changes to the Editorial Board","authors":"Kelin J. Kuhn","doi":"10.1109/LED.2026.3707713","DOIUrl":"https://doi.org/10.1109/LED.2026.3707713","url":null,"abstract":"","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"1977-1977"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=11714240","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072265","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Changes to the Editorial Board","authors":"Kelin J. Kuhn","doi":"10.1109/LED.2026.3707711","DOIUrl":"https://doi.org/10.1109/LED.2026.3707711","url":null,"abstract":"","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"1975-1975"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=11714242","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072301","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"IEEE Transactions on Electron Devices Table of Contents","authors":"","doi":"10.1109/LED.2026.3731839","DOIUrl":"https://doi.org/10.1109/LED.2026.3731839","url":null,"abstract":"","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2129-C3"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://ieeexplore.ieee.org/stamp/stamp.jsp?tp=&arnumber=11714241","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072286","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
{"title":"Performance Enhancement of IGZO Thin-Film Transistors by Ultrathin Te Back-Channel Heterojunction Capping","authors":"Kai-Jhih Gan;Chong Ma;Zefu Zhao;Jialong Xiang;Tiaoyang Li;Shaohao Wang;Dun-Bao Ruan","doi":"10.1109/LED.2026.3724062","DOIUrl":"https://doi.org/10.1109/LED.2026.3724062","url":null,"abstract":"Ultrathin p-type capping layers were introduced to modulate the back-channel surface of IGZO thin-film transistors (TFTs). Among Te, NiO<sub>x</sub>, and SnO<sub>x</sub> capping layers, the Te-capped IGZO TFT exhibits the best balanced performance, with a subthreshold swing (SS) of 67.1 mV/dec, a field-effect mobility (<inline-formula> <tex-math>$mu _{text {FE}}text {)}$ </tex-math></inline-formula> of 25.6 cm<sup>2</sup>/V<inline-formula> <tex-math>$cdot $ </tex-math></inline-formula>s, an on/off current (I<sub>on</sub>/<inline-formula> <tex-math>$mathrm{I}_{text {off}}text {)}$ </tex-math></inline-formula> ratio of <inline-formula> <tex-math>${1}.{06}times {10} ^{{9}}$ </tex-math></inline-formula>, and a threshold voltage (<inline-formula> <tex-math>$mathrm{V}_{text {TH}}text {)}$ </tex-math></inline-formula> of −0.035 V. Compared with the control device, Te capping reduces SS by 63%, enhances <inline-formula> <tex-math>$mu _{text {FE}}$ </tex-math></inline-formula> by 43%, and shifts V<sub>TH</sub> positively by 0.945 V. The I<sub>on</sub>/I<sub>off</sub> ratio also increases by 49.3 times. The 2-nm Te layer therefore enables simultaneous improvement in switching steepness, carrier transport, and V<sub>TH</sub> control through back-channel modulation.","PeriodicalId":13198,"journal":{"name":"IEEE Electron Device Letters","volume":"47 10","pages":"2067-2070"},"PeriodicalIF":4.6,"publicationDate":"2026-10-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149072256","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"工程技术","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}