- #1
roam
- 1,271
- 12
I am trying to find the effective mass of the electron within the first Brillouin zone in a particular direction in a crystal where the energy of the electron varies with some wave vector ##E(k)=Ak^2+Bk^4##. But I need to express this as a fraction of the electron rest mass.
I know that the effective mass (from Newton's 2nd law) is given by:
At the first Brillouin zone boundary we have ##k =\pi / a##. Also the second derivative of the E(k) is ##\frac{d^2E}{dk^2}=2A+12Bk^2##.
Substituting these in I think the effective mass is:
Now, how does one express this as a fraction of the electron rest mass m (511 KeV)?
Any suggestion or correction is appreciated.
I know that the effective mass (from Newton's 2nd law) is given by:
##m^* = \frac{\hbar^2}{d^2E/dk^2}##
At the first Brillouin zone boundary we have ##k =\pi / a##. Also the second derivative of the E(k) is ##\frac{d^2E}{dk^2}=2A+12Bk^2##.
Substituting these in I think the effective mass is:
##m^* = \frac{\hbar^2}{2A+12B (\frac{\pi}{a})^2}##
Now, how does one express this as a fraction of the electron rest mass m (511 KeV)?
Any suggestion or correction is appreciated.