- #1
transmini
- 81
- 1
For a lab I just finished this past week, we were working with the hall effect and finding hall voltages. The metals used were p-germanium and n-germanium semi-conductors. I understand why in n-germanium the hall voltage is positive and p-germanium is negative assuming negative charge carriers for n-type and positive holes as carriers for p-type.
What I don't get is why we are treating positive holes as the carriers. Even though it looks like a positive hole is moving through as a current, the electrons are still what's moving, creating the movement of the holes. So the ##\vec{F}=q(\vec{v}\times \vec{B})## would still be in the same direction as for negative charge carriers, since it is still technically the electrons that are movin, causing the voltages to be the same, since ##\vec{v}## and ##\vec{B}## are in the same direction still and ##q## is still the same sign. Why does the Hall effect behave as if the holes are actually a moving mass instead in p-type, like electrons for n-type?
What I don't get is why we are treating positive holes as the carriers. Even though it looks like a positive hole is moving through as a current, the electrons are still what's moving, creating the movement of the holes. So the ##\vec{F}=q(\vec{v}\times \vec{B})## would still be in the same direction as for negative charge carriers, since it is still technically the electrons that are movin, causing the voltages to be the same, since ##\vec{v}## and ##\vec{B}## are in the same direction still and ##q## is still the same sign. Why does the Hall effect behave as if the holes are actually a moving mass instead in p-type, like electrons for n-type?