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ECE 875: Electronic Devices

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Presentation on theme: "ECE 875: Electronic Devices"— Presentation transcript:

1 ECE 875: Electronic Devices
Prof. Virginia Ayres Electrical & Computer Engineering Michigan State University

2 Lecture 31, 28 Mar 14 Chp 04: metal-insulator-semiconductor junction: GATES Capacitances: Low frequency voltage sweep: 1 Hz to 1KHz High frequency voltage sweep: > 1Mz - slow ramp: Pr. 4.06 - fast ramp VM Ayres, ECE875, S14

3 C-V curves and Frequencies:
Use Gate voltage: Sweeping Vgate for example ± 4 Volts over and over to turn the channel OFF and ON: binary logic Low: 1- 1 kHz Intermediate: 1 kHz - 1 MHz High: > 1 MHz Vgate: Slow ramp Vgate: Fast ramp ON/OFF cycles per sec “counting” charge per sec applied to gate VM Ayres, ECE875, S14

4 OFF ON C / Ci C-V curves for n-channel in p-substrate: Low
Intermediate C / Ci High + slow ramp High + fast ramp VM Ayres, ECE875, S14

5 OFF ON C / Ci C’min V’min = VT
What looks different in the readout: flat line in Vfor and Cmin shift OFF ON Low C / Ci Cmin High + slow ramp C’min V’min = VT Vmin VM Ayres, ECE875, S14

6 Cmin = Ci CDmin CDmin = CminCi Ci + Cmin Ci + CDmin Low frequency C-V:
You know the experimental values in the circles. Therefore it’s easy to get a number for Cdmin Cmin = Ci CDmin CDmin = CminCi Ci + Cmin Ci + CDmin VM Ayres, ECE875, S14

7 Low frequency C-V: Low: 1- 1 kHz: develop (ON) and later remove (=> OFF) a full inversion layer and a full depletion region VM Ayres, ECE875, S14

8 High frequency + slow ramp:
> 1 MHz: develop and later remove a full depletion region charge qNAWD. But e-’s don’t have time to form a full inversion layer at the surface Fig. 8, (b) VM Ayres, ECE875, S14

9 High frequency + slow ramp: simpler:
C’Dmin = es /WDmax So total capacitance C’min is: C’min = Ci C’Dmin Ci + C’Dmin VM Ayres, ECE875, S14

10 Low frequency High frequency, Slow ramp WDmax is bigger Qn smaller
VM Ayres, ECE875, S14

11 High frequency + slow ramp: WDmax
From strong inversion up to thermal energy Have been finding WD = WDm at the start of inversion with ys = 2 kT/q ln (NA/ni). But (Qs, ys) can be bigger VM Ayres, ECE875, S14

12 High frequency + slow ramp: WDmax:
VM Ayres, ECE875, S14

13 Assume that Pr. 4.06  the high frequency- slow ramp condition
VM Ayres, ECE875, S14

14 Qn layer; no time to form at all
Low frequency High frequency, Slow ramp High frequency, Fast ramp WDmax is bigger WDmax is biggest Qn layer; no time to form at all Qn smaller Qn biggest VM Ayres, ECE875, S14

15 High frequency + fast ramp: during ON:
No Qn and big WDmax: “driven into deep depletion” VM Ayres, ECE875, S14

16 across insulator region
CD  Qs region ys = 0) Ci  across insulator region VM Ayres, ECE875, S14

17 VM Ayres, ECE875, S14

18 ys VGate

19 Iterate Pr. 3. 9 until donor concentration ND-nth – ND-(nth+1) = 0
Iterate Pr. 3.9 until donor concentration ND-nth – ND-(nth+1) = 0.01 x 1016 cm-3


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