What is the significance of the contact potential in metal-metal interfaces?

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Discussion Overview

The discussion centers on the significance of contact potential in metal-metal interfaces, particularly in the context of calculating expected results when two metals with different work functions are in contact. Participants explore theoretical frameworks, measurement techniques, and implications for circuit behavior.

Discussion Character

  • Exploratory
  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • One participant seeks resources for calculating interface behavior between two metals, referencing Anderson's Rule and the Schottky-Mott Rule, while expressing uncertainty about their applicability to metal-metal interfaces.
  • Another participant suggests limiting the discussion to metal-metal interactions and considers the implications of differing crystal structures and microscopic gaps.
  • A different viewpoint emphasizes the fundamental differences between metals and semiconductors, questioning the simplification of applying semiconductor theories to metals, particularly regarding band gaps and charge flow.
  • Concerns are raised about the behavior of charge flow when connecting two different metals, specifically whether a measurable voltage exists without continuous current flow due to the contact potential.
  • Participants mention the Kelvin probe method as a relevant technique for measuring work function and surface potential, noting its connection to the physics of metal-metal interfaces and potential gradients.
  • There is a request for clarification on the significance of contact potential in practical circuit applications, indicating ongoing uncertainty about its effects.

Areas of Agreement / Disagreement

Participants express a range of views on the applicability of semiconductor theories to metals, the nature of charge flow at metal-metal interfaces, and the significance of contact potential. No consensus is reached on these issues.

Contextual Notes

Participants highlight limitations in existing theories and models, particularly regarding their applicability to metal-metal interfaces. There is also mention of unresolved questions about the behavior of charge flow and the implications of contact potential in circuits.

Who May Find This Useful

This discussion may be of interest to those studying materials science, electrical engineering, or surface physics, particularly in relation to metal interfaces and their applications in electronic devices.

VortexLattice
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Hi all,

I'm trying to find resources for how to calculate and find what I should expect as the result of the interface between two metals with different work functions.

Anderson's[/PLAIN] Rule tells us how to do this for two semiconductors and the Schottky-Mott Rule tells us how to do it for a metal-semiconductor interface (and those articles both mention that in reality those rules rarely actually predict something close to reality).

All I can find for a metal-metal interface (assuming there are no oxide layers between them or anything) is this article, but it's not clear to me if that's a very oversimplified model or not.

Does anyone have any suggestions, or know of any programs that could calculate this?

Thank you!
 
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For starters, can you limit these theories to the metal-metal case? Maybe make the gap go to zero?

Definitely you expect impedance from the differing crystal structures and gap between the materials (although it may be microscopic).
 
Well, maybe that would work, but metals are fundamentally different from semiconductors... For example, if the top of the valence band is now 5eV above the bottom of the conduction band (so they overlap), would you say that the band gap is now 0, or maybe -5eV? I kind of suspect you can't naively just apply a simplified version of these.

But I think what I'm looking for is this. However, I'm still unsure about a bunch of stuff about it. So the basic idea is, when you connect two different metals with a conducting wire, a tiny bit of charge flows from one to another until the Fermi levels (not equal to the chemical potentials!) are equal.

So, is it true that you have this strange situation where there is a measurable voltage across the two metals, but charge isn't constantly flowing (obviously) due to that?

So, what happens if you just apply an exterior voltage to this setup? Because there is a voltage by default across the metals, would you see no current until you got to some threshold voltage?
 
In the Kelvin probe method, the physics of metal-metal interface is central to the ability to measure the work function/surface potential. So maybe you might want to try looking into that technique, because it tends to cover the physics of metal-metal interface.

The brief summary of it here is that, similar to the PN junction case, the Fermi levels of the two metals will align themselves, creating a potential gradient across the metal-metal junction.

You may try looking at this paper for a start.

http://kummelgroup.ucsd.edu/pubs/paper/110.pdf

Zz.
 
ZapperZ said:
In the Kelvin probe method, the physics of metal-metal interface is central to the ability to measure the work function/surface potential. So maybe you might want to try looking into that technique, because it tends to cover the physics of metal-metal interface.

The brief summary of it here is that, similar to the PN junction case, the Fermi levels of the two metals will align themselves, creating a potential gradient across the metal-metal junction.

You may try looking at this paper for a start.

http://kummelgroup.ucsd.edu/pubs/paper/110.pdf

Zz.

Hi, thank you for the reply, I read the relevant part of that. But there's still something I don't really understand, what is the significance of that contact potential, even if you can measure it? Does it affect the two metals if they are part of a circuit?
 

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