SUVAM ROY
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Why is it opposite to that of an electron?
SUVAM ROY said:Why is it opposite to that of an electron?
Well I know what is effective mass, how it's expression is obtained, how it varies for electron with wavenumber 'k' (m* vs k graph). But can't understand why for hole the m* vs k graph is opposite to the graph of electron.ZapperZ said:Back up a bit. You haven't told us what you already know.
For instance, do you know how we obtain the 'effective mass' of anything in a solid? For example, the "electron" that is in a metal or semiconductor also has an effective mass. Do you know how that is obtained?
In the future, unless you want your question to drag on for people to figure out what exactly you are asking, you must put SOME effort in elaborating your question, but also what you already know and tried to find out. It is required in the PF Rules.
Zz.
SUVAM ROY said:Well I know what is effective mass, how it's expression is obtained, how it varies for electron with wavenumber 'k' (m* vs k graph). But can't understand why for hole the m* vs k graph is opposite to the graph of electron.
Thanks. It's just my conception was not that clear. Will you check if I am right or not.ZapperZ said:Then I don't understand why you have your problem.
For example, look at Page 1 of this link at the top figure of a generic band structure of a semiconductor:
http://users.physik.fu-berlin.de/~pascual/Vorlesung/WS05/Slides/WS05-06%20AdMat%20IT%20-%20L1b.PDF
The bottom of the conduction band (energy band 1), the second derivative of E vs k is positive, and thus, m* is positive. The top of the valence band (energy band 2) has a negative curvature, and thus, the second derivative is negative, giving a negative m*.
Thus, knowing how m* is derived, and knowing the band structure, you get what m* is. If you know these, why are you still having a problem in understanding it?
Zz.