Conversation started Aug 20, 2019 at 15:44.
Aug 20, 2019 15:44
@Aladdin A $p$-type dopant has an outer electron state just above the valence band so an electron in the valence band can jump up to it leaving behind a hole.
Again the negative acceptor dopant ion can't move, but the hole can. So $p$-type doping produces lots of mobile holes.
Aug 20, 2019 16:00
@JohnRennie ifthe electron jumps from valence band to the outer electronics state, it will leave a hole
But I don't get why the acceptor ion is negative.... Maybe because electrons are going into it?
Yes. The acceptor starts off neutral and it accepts an electron from the valence band to form a negative ion.
Okay and also hole is the majority carrier here
Ah got it. Now I can understand biasing properly
A typical $p$-type dopant would be boron with 3 electrons in its outer shell. It accepts a fourth electron so it can form four bonds just like the silicon atoms around it.
Aug 20, 2019 16:05
But that would create a hole on the other site if it accepts electron
@Aladdin I think we might be talking at cross purposes ...
What is cross purpose
If you start with pure silicon and add a $p$-type dopant like boron then it creates holes in the valence band and negative B- ions in the band gap just above the valence band.
Yea. I got till here
The electrons in the B- ions can't move, so conduction is due to the holes created in the valence band.
 
Conversation ended Aug 20, 2019 at 16:08.