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A Schottky diode is constructed with two metal conductors bonded to a doped semiconductor. One of the metal-semiconductor junctions is a Schottky contact, and the other metal-semiconductor junction is an Ohmic contact. If the doping in the semiconductor is uniform, and the two metalic contacts are made of the same metal, I would presume the device would be symmetric, and would not be useful as a diode. If it had two Schottky contacts, they would be in opposing orientations. If it had two Ohmic contacts, it would just be a resistor composed of doped semiconductor.

My question is, how it the asymmetry between the two contacts achieved? Is there a doping gradient in the semiconductor? Are the two metal conductors composed of different metals? Is there some third alternative that I am missing?

(The common internet literature on Schottky diodes explains why the Schottky metal-semiconductor junction acts as a diode, but I have not seen an explanation of how the Ohmic contact in the same device is made to be different).

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    \$\begingroup\$ I think it's typically done by doping -- but if I were sure, this would be an answer, not a comment! I just read the Wikipedia article on ohmic contacts and came away with the impression that it's much easier to make a Schottky contact than an ohmic one. \$\endgroup\$ – TimWescott Feb 20 at 17:25
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    \$\begingroup\$ The key search phrase you may need is "ideal nonrectifying barrier". Check this out: eng.libretexts.org/Bookshelves/Materials_Science/… It boils down to mating the right metal with the right semiconductor so their work functions (or maybe their energy bands?) transition smoothly into one another. You sometimes need a third intermediary material to do this. If you make it discontinuous, you get a Schottky junction. If you make it smooth, you get an Ohmic junction. \$\endgroup\$ – DKNguyen Feb 20 at 18:02
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    \$\begingroup\$ I have always been surprised that explanations about the rectifying effect of a junction doesn't even mention that there should be the opposite effect on the other side of the material. In fact, the other side is manufactured as a ohmic junction, but as the understanding of the ohmic junction needs Quantum mechanics, this subject is hidden under the carpet (sometime : Physics = Magic). To be confirmed. \$\endgroup\$ – andre314 Feb 20 at 19:01
  • \$\begingroup\$ @andre314 I know, right? I would understand it if it was an electronics course where you only use components and never have to design them. But even in undergrad electronics engineering where they're teaching you the internal workings of semiconductors it isn't even mentioned. Just mentioning it would be enough. \$\endgroup\$ – DKNguyen Feb 20 at 19:06
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    \$\begingroup\$ @andre314 I agree to a point... that explanation only really applies if you're talking about a discrete Schottky diode. In the case of e.g. a PN diode, both M-S junctions are ohmic and the rectification comes from the P-N semiconductor junction, of course. The Schottky barriers I work with on a day-to-day are actually a parasitic (formed by the gate contact of a HEMT), so there's not exactly an "other side of the material" to consider. We never even talked metal-semiconductor junctions in my undergrad semiconductors course, or if we did it was so far over our heads we didn't retain any of it! \$\endgroup\$ – Shamtam Feb 20 at 23:16
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As alluded to by DKNguyen in the comments, the "asymmetry" appears because the contacts on either side of the diode are formed with different metals. A given semiconductor has a given workfunction, as does any given metal. The difference in the workfunction of the semiconductor and the contact metals determines how the interface between the two behaves.

There are two broad classes of metal-semiconductor junction: rectifying (i.e. Schottky junction) and non-rectifying (i.e. Ohmic junction). More info on the Wikipedia page, of course..

In addition, doping can also come into play. It's often impossible to find a metal that will form a desired contact for a given intrinsic semiconductor, but doping can adjust the workfunction of the semiconductor to make this possible. Often times, the region used to form a metal-semiconductor junction will be doped to adjust the junction properties. For example, ohmic contacts often are heavily doped to lower contact resistance. Another example would be adjusting the doping level of the semiconductor to precisely control the Schottky barrier height (which would adjust the forward voltage of the diode).

The following diagrams are taken from here, where a more complete explanation can be found: https://eng.libretexts.org/Bookshelves/Materials_Science/Supplemental_Modules_(Materials_Science)/Semiconductors/Metal-Semiconductors_Contacts

If you select the appropriate a metal and semiconductor, each with their own energy bands, that is appropriate to make a Schottky diode it ends up looking like this when unbiased:

The energy bands of a Schottky diode look like this when forward biased:
[![enter image description here][1]][1]

Then when you forward bias it it looks like this and electrons can easily make it up the energy slop roll off the energy cliff and move from one side to the other in the forward direction. The cliff prevents electrons from traversing in the reverse direction.

enter image description here

If you reverse bias it, the cliff is still there preventing electrons from moving in the reverse direction, but now the energy slope that must be overcome in the forward direction is also steeper preventing electrons from flowing in either direction.

enter image description here

But if you choose the energy bands of the material so that when they mate together, the energy bands transition smoothly without a cliff then you get an ohmic contact where the electrons can traverse in either direction with minimal biasing:

enter image description here

Apparently you don't need to actually make it be smooth. You just need the semiconductor energy bands to be lower than the metal which causes the electrons in the metal valence band to spill out into the semiconductor which pushes up the semiconductor energy bands until they are level.

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  • \$\begingroup\$ Feel free to link eng.libretexts.org/Bookshelves/Materials_Science/… and reference images from it. It makes it clear as day compared to the Wiki page. \$\endgroup\$ – DKNguyen Feb 20 at 18:12
  • \$\begingroup\$ @DKNguyen I'd be happy to community wiki this answer if you'd like to improve on it! \$\endgroup\$ – Shamtam Feb 20 at 18:19
  • \$\begingroup\$ Or that. Doesn't matter to me. But I can only regurgitate what that link says. I also have the permissions to just add it into your post without making it community. \$\endgroup\$ – DKNguyen Feb 20 at 18:24

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