Why does Efm shift in MOSFETs?

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Discussion Overview

The discussion centers on the behavior of the Fermi level (Efm) in MOSFETs in response to varying gate voltages, particularly focusing on the shifts in energy band diagrams when applying positive or negative gate voltages. Participants explore the implications of these shifts in the context of thermal equilibrium, work function differences, and the concept of flat band voltage (Vfb).

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant questions why Efm shifts upwards with negative gate voltage and how it behaves with positive voltage, expressing confusion about the relationship between Efm and Efp.
  • Another participant clarifies that the Fermi level is constant only at thermal equilibrium with no external bias, suggesting that shifts occur due to applied voltages.
  • A participant references the alignment of Fermi levels in PN junctions, questioning the consistency of Efm and Efp levels in MOSFETs.
  • Discussion includes the concept that when no external voltage is applied, Efm and Efp are aligned at the same height, but shifts occur under bias conditions.
  • One participant describes the effects of applying positive gate potential, detailing how it attracts electrons and causes shifts in the Fermi levels of both metal and semiconductor, leading to band bending.
  • A reference to work function differences is made, explaining that these differences lead to band bending in equilibrium conditions and the significance of flat band voltage (Vfb) in determining further gate voltage effects.

Areas of Agreement / Disagreement

Participants express varying levels of understanding regarding the shifts in Efm and Efp, with some agreeing on the principles of thermal equilibrium and work function differences, while others remain uncertain about the implications of Vfb and its role in the discussion.

Contextual Notes

Participants mention the need for assumptions regarding Vfb and its implications on the behavior of the MOSFET, indicating that the discussion relies on specific definitions and conditions that may not be universally agreed upon.

jaus tail
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Hi,
I'm studying MOSFET and the book says that when N-channel mosfet has negative or positive gate voltage, the energy band diagram will shift. I don't understand why Efm shifts.
upload_2018-9-15_14-35-31.png

Now when Vg is negative the Efm shifts upwards, Why? And when later when Vf is positive the Efm also shifts again? I don't understand this. Shouldn't Efm and Efp be at same level?

upload_2018-9-15_14-34-57.png
 

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The Fermi level (or electrochemical potential of the electrons) is only constant throughout a MOS device when thermal equilibrium is reached and no external bias is applied to the device..
 
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Thanks for the reply. Shouldn't Efm and Efp be at same level. At junction of PN diode, we shift bands after aligning the Ef of both doped regions together.
 
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Thanks. This helped clear some things up. Just to be sure. Let's assume Vfb = 0 for now. initially mosfet fermi and Si fermi are at same level.
upload_2018-9-17_22-25-12.png

I got the above pic from the pdf link you gave.
Now if I apply positive Gate potential, then the positive terminal will attract electrons from Gate (metal). So the surface junction between Metal and Oxide will be devoid of electrons and so fermi level of metal will shift downwards.
Likewise the positive terminal will attract electrons from P-silicon body and fermi level of Semiconductor shifts up toward Ec at surface. Thus we bend Ec and Ev of Semiconductor so that Ec is closer to Ef at junction.

This pic helped a lot:
upload_2018-9-17_22-27-40.png

But I don't understand How Vfb helps. I assumed Vfb = 0 and was able to figure out how bands shift. But can you elaborate as to how Vfb comes in the picture?
When Vg is less than Vfb as in accumulation case, is Vg also less than zero? That would explain why negative Q accumulates at junction. Cause negative Vg repels electrons to junction.
 

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From “Physics and Technology of Semiconductor Devices” by Andrew S. Grove:

The electron energies at the Fermi level in the metal and in the semiconductor of an MOS structure will, in general, be different. Such an energy difference is usually expressed as a difference in work functions, which is the energy required to remove an electron from the Fermi level in a given material to vacuum. When the metal of an MOS structure is shorted to the semiconductor, electrons will flow from the metal to the semiconductor or vice versa until a potential will be built up between the two which will counterbalance the difference in work functions. When equilibrium is reached, the Fermi level in the metal is lined up with the Fermi level in the semiconductor. Therefore, there will be an electrostatic potential variation from one region to the other, as illustrated in….

Thus, when there is a difference in work function between the metal and the semiconductor, one has band bending within the semiconductor in the equilibrium case with gate voltage VG = 0. You can now apply just enough gate voltage VG to counterbalance the work function difference and to maintain a flat band condition in the semiconductor. The gate voltage required to bring about the flat band condition is called the flat band voltage VFB. VFB is - so to speak - the reference point for the gate voltage VG for further considerations.
 
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