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Per Oni said:My idea is this: the Lorenz force causes slightly more electrons to flow along the left of the conductor (ref post # 6). This would mean that more “holes” are formed at the left side, where now the probability of an electron knocking other electrons is higher. This way the fields of the static +ve holes at the left will dominate the Hall field generated by the electron current.
Can I understand what you said like this:
Considering figure post #6, right; Yes the current moves upwards, so due to Lorentz force/field more electrons flows in the left hand side than on the right. However for the more electrons to flow there must be more available holes (since in p-type materials the only way electrons move is my jumping from one hole to the other). So, in addition to more electrons on the left side there is also more holes.
But due to some * reasons, the holes dominate and hence we get the positive polarity!
If this summary is incorrect, you can entirely skip, what I have written below!
However one question has struck to me. Does the existence of hole makes the region spontaneously +ve? I mean to ask, suppose there are two blocks of silicon wafer. One is heavily doped with holes. One isn't doped. Is there a Voltage Deference between them? I guess no, because both are electrically neutral, although the p-type wafer has tendency to accept electrons in expense of its neutrality!
So, I think I got the answer, a Voltage develops after sometime if we connect them with a wire but not initially, is this correct?
If that's correct, then in above scenario, how can holes dominate and give positive polarity? Having holes in a region doesn't spontaneously makes that region +ve!