Valley degeneracy in tunneling current

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SUMMARY

The discussion focuses on valley degeneracy in the context of calculating tunneling current, specifically using the equation $$I_T=q\frac {g_sg_v} {L} \sum_{k} v_g(k)(f_v-f_c)T$$. The valley degeneracy factor, g_v, quantifies the number of distinct energy minima in a material's band structure, which is influenced by the symmetry of the crystal lattice. For instance, in a two-dimensional honeycomb lattice, g_v equals 2 due to the presence of two valleys at the corners of the Brillouin zone. Understanding how to count valley degeneracy is crucial for accurate tunneling current calculations.

PREREQUISITES
  • Understanding of tunneling current equations, specifically $$I_T=q\frac {g_sg_v} {L} \sum_{k} v_g(k)(f_v-f_c)T$$
  • Knowledge of band structure and energy minima in solid-state physics
  • Familiarity with crystal lattice symmetry and its impact on electronic properties
  • Basic concepts of the Brillouin zone in condensed matter physics
NEXT STEPS
  • Research the calculation methods for valley degeneracy in various materials
  • Study the implications of crystal lattice symmetry on electronic band structures
  • Explore the role of the Brillouin zone in determining electronic properties
  • Learn about advanced tunneling current models in two-dimensional materials
USEFUL FOR

Physicists, materials scientists, and electrical engineers interested in semiconductor physics, particularly those focused on tunneling phenomena and valley degeneracy in two-dimensional materials.

Noki Lee
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I'm trying to understand the valley degeneracy to calculate the tunneling current.

Here is the equation of tunneling current.$$I_T=q\frac {g_sg_v} {L} \sum_{k} v_g(k)(f_v-f_c)T$$

##g_v## is valley degeneracy. I thought it comes from the symmetry of structures, depending on a certain point in k-space like below

$$I_T=q\frac {g_s} {L} \sum_{k} g_v(k)v_g(k)(f_v-f_c)T$$

How can I count the number of valley degeneracy?
And what I'm misunderstanding?
 
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The valley degeneracy factor, g_v, is a measure of the number of valleys, or distinct energy minima, in the band structure of the material. It is related to the symmetry of the crystal lattice and the number of distinct energy minima that exist in the Brillouin zone. In general, it is determined by counting the number of distinct points in the Brillouin zone where the band has a minimum energy. This number may be equal to 1, 2, 3, or more, depending on the material and its lattice structure. For example, in a two-dimensional honeycomb lattice, the band structure includes two distinct valleys at the corners of the Brillouin zone (K and K'), so the valley degeneracy factor, g_v, would be equal to 2.
 

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