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MOS capacitor before joining The metallic gate may be replaced with a heavily doped p+ polysilicon gate. The Fermi energy levels are approximately at.

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Presentation on theme: "MOS capacitor before joining The metallic gate may be replaced with a heavily doped p+ polysilicon gate. The Fermi energy levels are approximately at."— Presentation transcript:

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2 MOS capacitor before joining The metallic gate may be replaced with a heavily doped p+ polysilicon gate. The Fermi energy levels are approximately at the same level.

3 Positive electron energy

4 MOS capacitor after joining Assume that there is no charge in the oxide layer

5 MOS capacitor energy levels

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7 MOS capacitor p type semiconductor voltage bias effects E G V

8 MOS capacitor p type semiconductor voltage bias effects –battery switched G V E

9 MOS capacitor n type semiconductor voltage bias effects G V E

10 MOS capacitor n type semiconductor voltage bias effects –battery switched E G V

11 MOS capacitor after joining Assume that there is charge in the oxide layer

12 G V MOS capacitor p type semiconductor gate voltage V G = V Flatband

13 MOS capacitor p type semiconductor gate voltage V G = V T “threshold” G V

14 MOS capacitor –charge distribution..

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16 Problem 6.1 Charge distributions are depicted in an MOS capacitor. 1) Is the semiconductor n or p type? 2) Does the bias make it an accumulation mode, depletion mode or an inversion mode?

17 Problem 6.1 Charge distributions are depicted in an MOS capacitor. 1) Is the semiconductor n or p type? 2) Does the bias make it an accumulation mode, depletion mode or an inversion mode?

18 Electric field due to charges

19 . MOS capacitor – changing charge distribution with changing voltage accumulation mode.

20 . MOS capacitor – changing charge distribution with changing voltage depletion mode.

21 MOS capacitor – changing charge distribution with changing voltage

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23 definition Approximate proportion of charge located at x

24 Problem 6.22 Using superposition, find the dependence of the “flat bad voltage” as the charge density changes. Nonuniform charge density @ x Change of flat band voltage Superimposition applies

25 Problem 6.23 Using superposition, find the dependence of the “flat bad voltage” for a particular charge density profiles.. Charges located just at the interface

26 Charge density is nonuniform

27 Problem 6.28 Consider the high-frequency capacitance- voltage relationship. Locate the inversion; threshold; depletion; flat band, and accumulation points.

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