Free Electron Model of Metals Flashcards

1
Q

What is the equation for N(E) in the 3D box problem?

A

N(E) = Vk^2/3π^2 = V/3π^2 *(2mE/ћ^2)^3/2

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2
Q

What is the equation for the density of states n(E) in the 3D box problem?

A

n(E) = dN/dE = V/2π^2 *(2m/ћ^2)^3/2 *E^1/2

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3
Q

What do we get a picture of from n(E) and N(E) in the 3D problem?

A

A picture of a “Fermi Sphere” of radius k(F) filled up with gas of N electrons.

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4
Q

How can we use the density of states to calculate the total energy in the 3D problem?

A

Etot = integral from 0 to E(F) of E*n(E) dE = V/5π^2 *(2m/ћ^2)^3/2 *E(F)^5/2

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5
Q

How do we get the average energy per electron in the 3D problem?

A

Etot/N = 3/5 *E(F)

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6
Q

What is the equation for the Fermi velocity?

A

v(F) = ћ*k(F)/m

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7
Q

What is the equation for the fermi energy in terms of temperature?

A

E(F) = k(B)*T(F)

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8
Q

For a gas of free electrons at T=0K, what does the graph of f(E) against E look like?

A

Straight line up to E(F) where it cuts down to 0, creating a square.

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9
Q

What is the equation for the Fermi-Dirac function?

A

f(E, μ, T) = 1/(exp((E-μ)/k(B)T)+1)

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10
Q

What does the graph f the Fermi-Dirac function look like for T2? How does it differ for T1

A

Starts off flat then curves own and tends to zero. FOr T1

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11
Q

What is the equation for N including the fermi-dirac function?

A

N = integral from 0 to inf of f(E, μ, T)*n(E) dE

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12
Q

What is the equation for the total energy in terms of the Fermi-dirac function?

A

Etot = integral from 0 to inf of f(E, μ, T)En(E) dE

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13
Q

What is the total energy change proportional to?

A

Total energy change proportional to n(E(F))*k(B)T

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14
Q

How is the specific heat Cv related to the temperature and energy?

A

Cv = dEtot/dT which is proportional to T.

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15
Q

What is magnetic susceptibility?

A

If a material is placed in a magnetic field with spin up, it will be affected differently from those with spin down.

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16
Q

What is the equation for up spin states for energy including μ(B)?

A

E = ћ^2 k^2/2m + Begћ/4m = ћ^2 k^2/2m + μ(B)B

17
Q

What is the equation for down spin states for energy including μ(B)?

A

E = ћ^2 k^2/2m - μ(B)B

18
Q

What do we find from these energies for up and down spin states?

A

That the total number of up electron states occupied is not equal to the total number of down spin states.

19
Q

What is the equation for the magnetisation M?

A

M = μ(B)(N(down)-N(up)) ~ μ(B)B*n(E(F))

20
Q

What is the equation for the susceptibility χ?

A

χ = dM/dB = μ(B)*n(E(F))

21
Q

For conduction, what analogy can we look at?

A

Conservation of mass flow in a fluid: flow through surface = rate of decrease of mass inside.

22
Q

What is the equation for the conservation of mass flow in a fluid (integrals)?

A

Closed double integral over S of j.dS = - triple integral over V of dρ/dt dV, so ∇.j = -dρ/dt

23
Q

Looking at the probability current in QM, what do we do to the Schrodinger equation and why?

A

We want the density ρ = Ψ* Ψ, so multiply the Schrodinger equation through by Ψ, and we look at the complex conjugate of the Schrodinger equation separately and multiply through by Ψ. Then subtract these 2 equations from eachother and rearrange for d(Ψ* *Ψ)/dt

24
Q

What do we do with the equation for d(Ψ* *Ψ)/dt? What happens in 2D and 3D?

A

Use ρ = Ψ* *Ψ, so this equation equals -∇.j, so we can find j from this. In 2D its just d/dx in bracket, but in 3D can replace with ∇.

25
Q

How can we check the equation for j?

A

Check for a plane wave description Ψ = exp(ik.r), and sub this into the equation for j.

26
Q

Thinking of lattice vectors R(n1,n2,n3) = n1a+n2b+n3c, what does each unit cell go between?

A

-a2 <= x <= a/2

27
Q

Thinking of the reciprocal lattice G(h,k,l) = hA+kB+lC, what is the spacing between each unit cell?

A

2π/a, so Brillouin zone is -π/a <= k <= π/a