For nonrelativistic electrons in a solid, different energy dispersion relations (with effective masses $m_a^*$, $m_b^*$, and $m_c^*$) are schematically shown in the plots. Which one of the following options is CORRECT?
To determine the correct option, we need to analyze the energy dispersion relations for nonrelativistic electrons in a solid and find how they relate to the effective masses \(m_a^*\), \(m_b^*\), and \(m_c^*\).
The energy dispersion relation for an electron is given by:
\(E = \frac{\hbar^2 k^2}{2m^*}\)
where \(E\) is the energy, \(k\) is the wave vector, \(\hbar\) is the reduced Planck's constant, and \(m^*\) is the effective mass of the electron.
From the equation, it is clear that the curvature of the dispersion relation in the \(E\) vs. \(k\) plot is inversely related to the effective mass:
Looking at the given plot:
From this analysis, we conclude:
Therefore, the correct option is:
The dispersion ($E(k)$) of the conduction band (CB) and valence band (VB) for a semiconductor are shown schematically in the figure. Considering the possibility of an electron making a transition from the bottom of the CB to the top of the VB, which of the following options is/are correct?
The temperature dependence of the electrical conductivity ($\sigma$) of three intrinsic semiconductors A, B and C is shown in figure. 
Let $E_A$, $E_B$ and $E_C$ be the bandgaps of A, B and C, respectively. Which one of the following relations is correct?