Psinter
- 278
- 785
In metals, there is a concept called the Fermi energy which you can calculate with the following:
Electron concentration in the solid:
<br /> n = (valency)*\frac{N_{A}D}{M_{AT}}\\<br />
Where:
n = electron concentration
valency = number of valency electrons in the atom
N_{A} = Avogadro constant
D = element density
M_{AT} = atomic mass
Energy of Fermi at absolute zero (0K):
E_{F0} = (\frac{h^2}{2m_e})(\frac{3n}{\pi})^{\frac{2}{3}}(\frac{1}{q})
Where:
E_{F0} = energy of Fermi at absolute zero (0K)
h = Plank's constant
m_e = effective electron mass at rest
n = electron concentration
\frac{1}{q} = reciprocal of electron charge (to convert energy units to electron volts)
However, the math above is for a single element. Is there any quantum mechanical approach for the same concept, but in alloys where you have a metallic bonding and the same crystalline structure?
I want to know if there is such a thing as Fermi energy in such structures (alloys) that can be tackled mathematically in a quantum mechanical way. Such that one could describe conductivity properties of an alloy. Or if there are other models for that.
Electron concentration in the solid:
<br /> n = (valency)*\frac{N_{A}D}{M_{AT}}\\<br />
Where:
n = electron concentration
valency = number of valency electrons in the atom
N_{A} = Avogadro constant
D = element density
M_{AT} = atomic mass
Energy of Fermi at absolute zero (0K):
E_{F0} = (\frac{h^2}{2m_e})(\frac{3n}{\pi})^{\frac{2}{3}}(\frac{1}{q})
Where:
E_{F0} = energy of Fermi at absolute zero (0K)
h = Plank's constant
m_e = effective electron mass at rest
n = electron concentration
\frac{1}{q} = reciprocal of electron charge (to convert energy units to electron volts)
However, the math above is for a single element. Is there any quantum mechanical approach for the same concept, but in alloys where you have a metallic bonding and the same crystalline structure?
I want to know if there is such a thing as Fermi energy in such structures (alloys) that can be tackled mathematically in a quantum mechanical way. Such that one could describe conductivity properties of an alloy. Or if there are other models for that.