Shigetaka Kumashiro
Renesas Electronics
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Publication
Featured researches published by Shigetaka Kumashiro.
IEEE Transactions on Electron Devices | 2006
Mitiko Miura-Mattausch; Norio Sadachika; Dondee Navarro; G. Suzuki; Youichi Takeda; Masataka Miyake; Tomoyuki Warabino; Yoshio Mizukane; Ryosuke Inagaki; Tatsuya Ezaki; Hans Jürgen Mattausch; Tatsuya Ohguro; Takahiro Iizuka; Masahiko Taguchi; Shigetaka Kumashiro; S. Miyamoto
The compact MOSFET model development trend leads to models based on the channel surface potential, allowing higher accuracy and a reduced number of model parameters. Among these, the Hiroshima University Semiconductor Technology Academic Research Center IGFET Model (HiSIM) solves the surface potentials with an efficient physically correct iteration procedure, thus avoiding additional approximations without any computer run-time penalty. It is further demonstrated that excellent model accuracy for higher-order phenomena, which is a prerequisite for accurate RF circuit simulation, is achieved by HiSIM without any new model parameters in addition to those for describing the current-voltage characteristics
IEEE Transactions on Electron Devices | 1987
Mohammad Madihian; Kazuhiko Honjo; H. Toyoshima; Shigetaka Kumashiro
This paper establishes a systematic approach for the design, fabrication, and modeling of a newly proposed self, aligned Al-GaAs/GaAs heterojunction bipolar transistor (HBT) employing a two-dimensional heterostructure device simulator and a heterojunction bi-polar transistor circuit simulator. The developed HBT has an abrupt emitter-base heterojunction, and applies a novel structure in which a single base electrode is placed between two emitter electrodes. A fabricated 3 × 8 µm2two-emitter HBT exhibits a measured current gain cutoff frequency fT= 45 GHz and a maximum oscillation frequency fmax= 18.5 GHz. Results of frequency divider circuit Simulation indicate that the developed HBT would be 1.4 times faster than a conventional HBT in which one emitter electrode is located between two base electrodes.
symposium on vlsi circuits | 2006
Kenichi Inagaki; Danardono Dwi Antono; Makoto Takamiya; Shigetaka Kumashiro; Takayasu Sakurai
An on-chip sampling oscilloscope with lps timing resolution is realized in 90nm CMOS process based on a proposed ramp waveform division scheme for precise signal integrity and power-line integrity measurement. The resolution in time is variable from 1ps to 64ps in 64 steps. A novel on-chip inductance measurement procedure is also proposed
IEICE Transactions on Electronics | 2005
S. Matsumoto; Hiroaki Ueno; Satoshi Kure Hosokawa; Toshihiko Kitamura; Mitiko Miura-Mattausch; Hans Jürgen Mattausch; Tatsuya Ohguro; Shigetaka Kumashiro; Tetsuya Yamaguchi; Kyoji Yamashita; Noriaki Nakayama
SUMMARY A systematic experimental and modeling study is reported, which characterizes the low-frequency noise spectrum of 100 nmMOSFETs accurately. Two kinds of measured spectra are observed: 1/f and non-1/f spectra. The non-1/f spectrum is analysed by forward and backward measurements with exchanged source and drain, and shown to be due to a randomly distributed inhomogeneity of the trap density along the channel and within the gate oxide. By averaging the spectra of identical MOSFETs on a wafer the measured non-1/f noise spectra reduce to a 1/f characteristics. On the basis of these measurement data a noise model for circuit simulation is developed, which reproduces the low-frequency noise spectrum with a single model parameter for all gate lengths and under any bias conditions.
international reliability physics symposium | 2010
Hideyuki Nakamura; Katsuhiko Tanaka; Taiki Uemura; Kan Takeuchi; Toshikazu Fukuda; Shigetaka Kumashiro
A novel SET pulse measurement circuit is proposed which can detect pulses narrower than 100ps. Alternation of SET pulses during the propagation through the chain of target cells is minimized, which is attributed to small chain length (typically 20). This circuit configuration contributes to obtaining pulse distribution similar to that observed in actual circuit in use. Distribution of SET pulse width measured by our circuit through the white neutron beam testing agrees well with that estimated by computer simulation.
international reliability physics symposium | 2012
Hideyuki Nakamura; Taiki Uemura; Kan Takeuchi; Toshikazu Fukuda; Shigetaka Kumashiro; Tohru Mogami
Neutron induced single event transient (SET) has been measured on NAND and inverter (INV) chain with changing fan-out, drive strength, size of drain diffusion area, temperature and VDD on 40nm and 90nm bulk CMOS technology. As the pulse width distribution varies with the length of SET target chain as well, it is important to use the chain length similar with the actual logic circuits. Using tens of stages of target chain, pulses wider than 150ps have been rarely observed. The results of the measurement show that the SER of SET changes depending on the cell type and fan-out. SER of SET in combinational logic circuits decreases by half from 90nm to 40nm for the same gate count and the same clock frequency.
international conference on simulation of semiconductor processes and devices | 2008
Masami Hane; Hideyuki Nakamura; Katsuhiko Tanaka; Kentaro Watanabe; Yoshiharu Tosaka; Kiyoshi Ishikawa; Shigetaka Kumashiro
Soft error phenomena induced by the Sea-level cosmic neutron have been investigated by using a simulation system that covers from an individual MOSFET device level to an LSI-chip level. This system consists of the several kinds of simulation codes/tools, such as a mixed-mode 3D device simulator, SPICE circuit simulator, and analyzing tools of gate-level net-lists. A comprehensive practical simulation flow is demonstrated in this paper on commercial 90 nm generation logic devices and standard-cells.
IEICE Transactions on Electronics | 2008
K. Yamada; Takashi Sato; Shuhei Amakawa; Noriaki Nakayama; Kazuya Masu; Shigetaka Kumashiro
A compact model is proposed for accurately incorporating effects of STI (shallow trench isolation) stress into post-layout simulation by making layout-dependent corrections to SPICE model parameters. The model takes in-plane (longitudinal and transverse) and normal components of the layout-dependent stress into account, and model formulas are devised from physical considerations. Not only can the model handle the shape of the active-area of any MOSFET conforming to design rules, but also considers distances to neighboring active-areas. Extraction of geometrical parameters from the layout can be performed by standard LVS (layout versus schematic) tools, and the corrections can subsequently be back-annotated into the netlist. The paper spells out the complete formulation by presenting expressions for the mobility and the threshold voltage explicitly by way of example. The model is amply validated by comparisons with experimental data from 90 nm- and 65 nm-CMOS technologies having the channel orientations of, respectively, (110) and (100), both on a (100) surface. The worst-case standard errors turn out to be as small as 1.7% for the saturation current and 8 mV for the threshold voltage, as opposed to ∼20% and ∼50 mV without the model. Since device characteristics variations due to STI stress constitute a significant part of what have conventionally been treated as random variations, use of the proposed model could enable one to greatly narrow the guardbands required to guarantee a desired yield, thereby facilitating design closure.
international conference on simulation of semiconductor processes and devices | 2009
Katsuhiko Tanaka; Hideyuki Nakamura; Taiki Uemura; Kan Takeuchi; Toshikazu Fukuda; Shigetaka Kumashiro
Current responses due to the strike of ionized particle onto nMOS transistor of 90nm and 55nm generation have been analyzed through 3D device simulations. From the current response, duration of charge collection (tcc) is determined, which correlated strongly with the width of erroneous pulse (SET pulse). Causes of the difference between tcc values of 90nm and 55nm generation MOSFETs have been investigated and it is found that the difference in STI depth and width of p-well contact line between these two generations influences tcc mainly. This is because that the resistance below the p-well contact affects the ability to pull out the excess holes remaining in the channel region. It is also shown that there is room for reducing tcc and hence SET pulse width by well profile engineering. I. INTRODUCTION Neutron-induced soft error phenomena have received much attention since they are considered as one of the major ob- stacles to realize highly reliable LSIs. Although Single-Event- Upset observed in memory circuits such as SRAMs and flip- flops is still major concern, soft error phenomena occurring in combinational-logic circuits can be more serious in future technology node (1). In the logic circuits, propagation of erroneous signal, called Single-Event-Transient (SET), occurs and the erroneous signal might be finally stored, for instance, in a flip-flop as illustrated in Fig. 1. The wider the SET pulse is, the more probably the erroneous signal is stored. Such a SET pulse is initially caused by collection of generated charge due to the impact of the ionized particle. In this paper, duration of charge collection is evaluated which is related to SET pulse width strongly, and its dependence on device structure dimensions and profiles is investigated.
asian solid state circuits conference | 2010
Masaaki Soda; Yoji Bando; Satoshi Takaya; Toru Ohkawa; Toshiharu Takaramoto; Toshio Yamada; Shigetaka Kumashiro; Tohru Mogami; Makoto Nagata
A sine-wave noise generator with a harmonic-eliminated waveform is proposed for measuring the noise tolerance of analog IPs. In the waveform, harmonics up to the thirteenth harmonic are eliminated by combining seven rectangular waves with 22.5-degree spacing phases. This waveform includes only high-region frequency harmonic components which are easily suppressed by a low-order filter. In the circuit, the harmonic-eliminated waveform generator is combined with a current-controlled oscillator and a frequency-adjustment circuit. The sine-wave noise generator can generate power-line noise from 20 MHz to 220 MHz in 1 MHz steps. A spurious-free dynamic range (SFDR) of 45 dB is obtained at the 100 MHz noise frequency.