Conduction and valence band for metals

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SUMMARY

In metals, the conduction and valence bands overlap, making it challenging to distinguish between them. The conduction band extends from a lower limit of E=-k eV to infinity eV, but this representation oversimplifies the nature of these bands. Each band consists of distinct electron wavefunctions associated with different wave vectors (k), despite their overlapping energy levels. The transition between wavefunctions within the valence band is continuous, while a transition to the conduction band is not possible without a significant energy input.

PREREQUISITES
  • Understanding of electron wavefunctions in solid-state physics
  • Familiarity with band theory of solids
  • Knowledge of wave vector (k) in quantum mechanics
  • Basic concepts of energy bands in metals
NEXT STEPS
  • Study the principles of band theory in semiconductors and insulators
  • Explore the mathematical representation of wavefunctions in quantum mechanics
  • Investigate the implications of overlapping bands on electrical conductivity in metals
  • Learn about the role of temperature in band structure and electron mobility
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Physicists, materials scientists, and electrical engineers interested in solid-state physics and the electronic properties of metals.

thinktank1985
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for metals the conduction and valence bands overlap. So how do you distinguish between the conduction and valence bands? How do you find out the lower limit of the conduction band and the higher limit of the valence band?

Or is it the case that the highest conduction band in a metal goes from a value of E=-k eV to infinity eV?
 
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It sounds as though you're thinking of a band only as a range of energy values, which is not accurate. Each band basically consists an electron wavefunction for each value of the wave vector k. If the valence band and conduction band overlap, then there is a valence band wavefunction and a conduction band wavefunction with the same energy, but they're still going to be different wavefunctions. Also, you can get from any wavefunction in the valence band to another continuously by varying k, but you can never get to the conduction band this way.

(As an analogy, you could think about sound waves and electromagnetic waves. They could both exist at the same frequency, but we think of them as distinct because: 1. they are clearly oscillating in a different way, and 2. there's no way you can transform one continuously into the other)
 

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