4H-SiC Lateral RESURF MOSFET with a Buried Channel Structure
4H-SiC Lateral RESURF MOSFET with a Buried Channel Structure
复制标题
具有埋沟道结构的 4H-SiC 横向 RESURF MOSFET
DOI:
10.4028/www.scientific.net/msf.433-436.753
复制
发表时间:
2003
期刊:
影响因子:
--
通讯作者:
K. Fukuda
中科院分区:
文献类型:
--
作者:
Seiji Suzuki;S. Harada;T. Yatsuo;R. Kosugi;J. Senzaki;K. Fukuda
This paper presents the static characteristics of 4H-SiC lateral R ESU F MOSFET with a buried channel structure. The MOSFET channel mobility was obtained to be as high as 80-90cm/Vs, resulting in the low channel resistance. The RESURF MOSFE T exhibited an on-resistance of 71m Ωcm and a breakdown voltage of 730V. A figure-of-merit ( Vbd / Ron) of this device was calculated to be 7.5MW/cm . Introduction SiC power MOSFET is a promising switching device for high-power el ctronics. Vertical MOSFETs using SiC are extensively investigated as iscrete devices [1-3]. On the other hand, lateral power MOSFET plays an important role in power IC a pplications. SiC RESURF (REduced SURface Field) MOSFETs have been demonstrated by several groups [4-6]. However, high channel resistance because of the poor channel mobility is a se rious problem for the low on-resistance of the SiC power MOSFET. Previously, we have repor ted the high channel mobility in 4H-SiC MOSFETs using the buried channel structure [7, 8]. In this paper, we present the static characteristics of 4H-SiC lateral RESURF MOSFET with a buried channe l structure. Device Design and Fabrication A schematic cross section of a lateral RESURF MOSFET fa bric ted in this study is shown in Fig.1. We adopted the RESURF, a gate field plate and the buried channe l structures in circular-geometric devices. Materials Science Forum Online: 2003-09-15 ISSN: 1662-9752, Vols. 433-436, pp 753-756 doi:10.4028/www.scientific.net/MSF.433-436.753 © 2003 Trans Tech Publications Ltd, Switzerland All rights reserved. No part of contents of this paper may be reproduced or transmitted in any form or by any means without the written permission of Trans Tech Publications Ltd, www.scientific.net. (Semanticscholar.org-12/03/20,10:57:01) A two-dimensional (2-D) simulation was carried out for the MOSFET design. The breakdown voltage and the maximum electric field in the field oxide Eox versus doping concentration of the RESURF region are shown in Fig.2. The channel and the RESURF length are 5 and 20 μm, respectively. Taking into account of the maximum Eox, the optimum dose for the RESURF region was 6-7x10 cm. The breakdown voltage of the MOSFET is designed to be 800-1000V. Maximum Eox decreased with the length of the RESURF layer. The RESURF length of 20μm was required for the maximum Eox below 3-4MV/cm. The devices were fabricated on p 4H-SiC substrates with a p-type homo-epitaxial layer (from CREE Research Inc.). The thickness and effective doping density ( NA-ND) of the epitaxial layer was 15μm and 5.0x10 /cm, respectively. Source and drain regions were formed by phosphorous ion implantation at 500°C. By using multiple implant energies and dose s, a box profile of about a 1x10cm and a junction depth of 0.3 μm was fabricated. The RESURF and buried channel region were implanted with nitrogen at room temperature. The tota l d se and the implanted depth of the each region were summarized in Table 1. The length of the RESURF layer was 20 μm. After all the ion implantation process was performed, activation anne ali g for the implanted impurities was performed at 1500°C for 5min in Ar. A field oxide was deposited by LPCVD with a thickness of 1 μm. After the channel area was opened by wet etching, a gate ox id was also deposited by LPCVD and reoxidized in dry O 2 at 1200°C for 140min followed by wet O 2 ambient at 950°C for 180min to densify the oxide film and improve the MO S interface quality. The final gate oxide thickness was 0.15 μm. Aluminum (Al) was used as both the gate metal and the contact metal for the source and drain. The gate field plate w as fabricated by extending the gate electrode on the field-oxide. Finally, the wafer surface wa s passivated with the polyimide film. Table1 Conditions of the ion implantations 140