A new SiGe Stepped Gate (SSG) Thin Film SOI LDMOS for enhanced breakdown voltage and reduced delay

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    ISDRS 2009, December 9-11, 2009, College Park, MD, USA

    ISDRS 2009 http://www.ece.umd.edu/ISDRS2009

    Student Paper

    A new SiGe Stepped Gate (SSG) Thin Film SOI LDMOS for enhanced

    breakdown voltage and reduced delay

    Radhakrishnan Sithanandam and M. Jagadesh Kumar

    Department of Electrical Engineering, Indian Institute of Technology Delhi, India, [email protected]

    This paper introduces a new SiGe Stepped Gate (SSG) thin film SOI LDMOS for enhanced

    performance. The proposed device eliminates the premature breakdown of the device due to

    floating body effects, which is one major problem of the thin film SOI LDMOS. The most

    common technique used to eliminate the floating body effects in SOI power device is the source

    tied body contact. Though this technique is successful in thick film devices, its effectiveness to

    thin film LDMOS is questionable, and also it imposes area penalty. Without a body contact, the

    floating body effects can be also reduced by decreasing the drift region doping [1]. But increased

    drift region resistance degrades the on-resistance of the device. The proposed device, SSG

    LDMOS circumvents the above challenges. It has a germanium implanted source and stepped fieldplate in the drift region. The SSG LDMOS reduces floating body effects in two ways. The SiGe

    source offers low potential to the excess holes generated due to the impact ionization [2]. The

    stepped gate reduces gate-drain capacitance improving the switching speed. The combined effect

    of (i) SiGe in the source and (ii) the stepped gate, improves the breakdown voltage and also allows

    us to increase the drift doping levels resulting in a reduced on-resistance.

    Using two dimensional device simulation [3], the proposed device is simulated and compared

    with the conventional thin film LDMOS. The cross-sectional view of both the devices is shown in

    Fig. 1. The conventional LDMOS has a uniform gate oxide thickness of 50 nm with a field plate.

    The drift region doping in both the devices is chosen for maximum breakdown voltage and is

    found to be 91016 cm-3 (which is higher than the conventional device doping 31016 cm-3). The

    germanium mole fraction in the SiGe source of the SSG LDMOS is chosen to be 0.2. The device

    parameters used in our simulation are given in Table 1. Figs. 2 and 3 show the breakdown

    characteristics and the on-resistance variation of the SSG LDMOS and the conventional LDMOS.The SSG LDMOS exhibits a 97% improvement in breakdown voltage and a 61% reduction in on-

    resistance compared to the convetional LDMOS. Figs. 4 and 5 show the switching delay and the

    gate-charge behaviour. We observe that the SSG LDMOS exhibits a 57% reduction in switching

    delay and a 50% reduction in gate-drain charge compared to the conventional LDMOS. This work

    clearly demonstrates the application of SiGe source and a stepped oxide gate in improving the

    performance of the LDMOS making this device more useful in both RF and wireless system-on-

    chip applications.

    References

    [1] M. Bawedin, C. Renaux and D. Flandre, LDMOS in SOI technology with very-thin silicon film,

    Solid State Electronics, vol. 48, pp. 2263-2270, Dec 2004.[2] M. J. Kumar and V. Verma, "Elimination of Bipolar Induced Drain Breakdown and Single Transistor

    Latch in Submicron PD SOI MOSFET,"IEEE Transactions on Reliability, vol. 51, no. 3, pp. 367-370,

    Sep. 2002.[3] ATLAS user's manual : Device simulation software. Santa Clara, CA: Silvaco International, 2007.

    978-1-4244-6031-1/09/$26.00 2009 IEEE

    Authorized licensed use limited to: INDIAN INSTITUTE OF TECHNOLOGY DELHI. Downloaded on January 31, 2010 at 04:39 from IEEE Xplore. Restrictions apply.

  • 8/14/2019 A new SiGe Stepped Gate (SSG) Thin Film SOI LDMOS for enhanced breakdown voltage and reduced delay

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    ISDRS 2009, December 9-11, 2009, College Park, MD, USA

    ISDRS 2009 http://www.ece.umd.edu/ISDRS2009

    Fig. 1 Cross sectional view of (a) the

    conventional LDMOS (b) the SSG LDMOS.

    Fig. 2 Breakdown voltage characteristics of

    the conventional and SSG LDMOS.

    Fig. 4 Switching characteristics of

    conventional and SSG LDMOS.

    Table. 1 Device parameters used in

    simulation.

    Gate oxide thickness,

    (tox1, tox2 and tox3)

    50 nm, 100 nm and300 nm

    Gate length,

    (LG1, LG2 and LG3)

    1 m, 0.5 m and0.5 m

    Channel length, L 0.5 m

    Source/Drain doping 11019 cm-3

    Channel doping 11017 cm-3

    Buried oxidethickness

    400 nm

    Silicon thickness 200 nm

    Drift region length 3.5 m

    Threshold voltage ofconventional and SSG

    LDMOS1.85 V

    Fig. 3 On-resistance of the conventional and

    SSG LDMOS.

    Fig. 5 Gate charging curve of conventional

    and SSG LDMOS.

    Authorized licensed use limited to: INDIAN INSTITUTE OF TECHNOLOGY DELHI. Downloaded on January 31, 2010 at 04:39 from IEEE Xplore. Restrictions apply.