Calculate the ratio of the Fermi wavevector to the radius of the largest sphere

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SUMMARY

This discussion focuses on calculating the ratio of the Fermi wavevector to the radius of the largest sphere inscribed in the first Brillouin zone for sodium, a monovalent free-electron metal with a body-centered cubic structure. The ratio is determined to be √(2/π):1. Additionally, the Fermi energy is calculated to be 5.09 × 10-19 J, and the change in Fermi energy per degree of temperature rise is found to be -1.81 × 10-23 JK-1, based on a linear thermal expansion coefficient of α = 7 × 10-5 K-1.

PREREQUISITES
  • Understanding of Fermi wavevector calculations
  • Knowledge of Brillouin zones in solid-state physics
  • Familiarity with the properties of body-centered cubic (bcc) structures
  • Basic principles of thermal expansion and its effects on material properties
NEXT STEPS
  • Study the derivation of Fermi energy in metals
  • Explore the concept of Brillouin zones and their significance in solid-state physics
  • Investigate the relationship between thermal expansion and electronic properties in metals
  • Learn about the implications of Fermi wavevector in quantum mechanics
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Students and researchers in condensed matter physics, materials science, and anyone interested in the electronic properties of metals, particularly those studying sodium and similar materials.

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Homework Statement



Sodium is, to a good approximation, a monovalent free-electron metal which has the
body-centred cubic structure.
(a) Calculate the ratio of the Fermi wavevector to the radius of the largest sphere that
can be inscribed in the first Brillouin zone. Remember that the reciprocal lattice of bcc
is fcc, and that the Brillouin zone is the cell formed in reciprocal space by the bisector
planes of the vectors from the origin to every reciprocal lattice point.
(b) If the cubic cell side of Sodium is 0.4225 nm, calculate its Fermi energy.
(c) Calculate the change in the Fermi energy of Sodium per degree temperature rise if
its linear thermal expansion coefficient is \alpha= 7 × 10^{-5} K^{-1}.
(The linear thermal expansion coefficient is related to the lattice parameter, a, by
\frac{da}{dT}=\alphaa)

The Attempt at a Solution



a) Fermi wavevector:
k_{F}=\sqrt{\frac{2}{\pi}}(\frac{\pi}{a})

r=\frac{\pi}{a}

so the ratio is \sqrt{\frac{2}{\pi}}:1

Is it really as simple as that or have I done something wrong?
 
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b) Fermi energy:E_{F}=\frac{h^{2}}{2m}k_{F}^{2}k_{F}=\sqrt{\frac{2}{\pi}}(\frac{\pi}{a})E_{F}=\frac{h^{2}}{2m}(\sqrt{\frac{2}{\pi}}(\frac{\pi}{a}))^{2}E_{F}=\frac{h^{2}}{2m}\frac{4}{\pi a^{2}}a=0.4225 nmE_{F}=\frac{h^{2}}{2m}\frac{4}{\pi(0.4225nm)^{2}}E_{F}= 5.09 × 10^{-19} Jc) \frac{dE_{F}}{dT}=\frac{\partial E_{F}}{\partial a}\frac{da}{dT}\frac{\partial E_{F}}{\partial a}= -\frac{8h^{2}}{\pi m a^{3}}\frac{da}{dT}= \alpha aso \frac{dE_{F}}{dT}= -\frac{8h^{2} \alpha a^{2}}{\pi m a^{3}}dE_{F}= -\frac{8h^{2} \alpha a^{2}}{\pi m a^{3}} dTdE_{F}= -\frac{8h^{2} \alpha a}{\pi m } dTdE_{F}= -1.81 × 10^{-23} JK^{-1} dT
 

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