4h-sic dmosfet and silicon carbide accumulation-mode laterally diffused mosfet archana n- 09mq01 -...

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4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics & Drives Dept. of EEE 1

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Page 1: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

4H-SIC DMOSFET AND

SILICON CARBIDE ACCUMULATION-MODE

LATERALLY DIFFUSED MOSFET

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 2: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

SiC

• excellent electrical and thermal properties.• only semiconductor material besides Si on

which a thermal oxide can be grown

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 3: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

Materials Property Si SiC-4H GaN

Band Gap (eV) 1.1 3.2 3.4

Critical Field 106 V/cm

0.3 3 3.5

Electron Mobility (cm2/V-sec)

1450 900 2000

Electron Saturation Velocity (106 cm/sec)

10 22 25

Thermal Conductivity (Watts/cm2 K)

1.5 5 1.3

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 4: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 5: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE OF POWER MOSFET:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 6: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE OF 4H-SIC DMOSFET :

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 7: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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• The MOS channel length is defined by the p-well and n+ implants, and can range from 0.5 μm to 1.5 μm.

• Electron flow : n+ source - inversion layer - implanted p-well

-JFET region - lightly doped n- drift region - drain.

Page 8: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE OF

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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• The blocking voltage of the MOSFET is determined by the doping concentration of the n- epilayer.

• For 1200 V devices, an epilayer with a doping concentration of 6x1015 cm-3 and a thickness of 12 μm can be used.

• A thermally grown oxide layer is typically used as gate dielectric due to its repeatability and stability.

Page 9: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

9

• Typically, the gate oxide is nitrided in NO or N2O to reduce MOS interface state density, which improves the transconductance of the

MOSFET.

Page 10: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

TRANSFER CHARACTERISTICS:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 11: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

OUTPUT CHARACTERISTICS:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 12: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE OFSiC AMLDM:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 13: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

• A thin n-channel region (accumulation-layer) below the gate oxide .

• Normally off device with the entire drain voltage supported by the p/n-drift region.

• Support high forward blocking voltages at zero gate bias with low leakage currents.

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Page 14: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

STRUCTURE:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

• A low resistance path for the electron current flow from the source to the drain can be achieved.

• This structure utilizes the buried p-well region as a shield to the influence of a high SiC bulk electric filed on the gate oxide.

• Removes the effect of interface quality on the channel mobility.

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Page 15: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

EFECT OF ACCUMULATION LAYER THICKNESS ON OPERATING VOLTAGE AND SPECIFIC ON RESISTANCE:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 16: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

TRANSFER

CHARACTERISTICS:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 17: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

OUTPUT CHARACTERISTICS:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 18: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

OFF STATE CHARCATERISTICS:

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

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Page 19: 4H-SIC DMOSFET AND SILICON CARBIDE ACCUMULATION-MODE LATERALLY DIFFUSED MOSFET Archana N- 09MQ01 - 15/10/2010 PSG COLLEGE OF TECHNOLOGY ME – Power Electronics

Archana N- 09MQ01 - 15/10/2010

PSG COLLEGE OF TECHNOLOGYME – Power Electronics & Drives

Dept. of EEE

THANK YOU

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