Step 1: Understanding the Question:
The effective mass ($m^*$) of an electron in a crystal lattice accounts for the internal forces exerted on the electron by the periodic potential of the lattice.
This question relates effective mass to the curvature of the Energy-wavevector ($E-k$) diagram and the energy band bandwidth.
Step 2: Key Formula or Approach:
The effective mass $m^*$ of an electron in a crystal band is defined as:
\[ m^* = \frac{\hbar^2}{\frac{d^2E}{dk^2}} \]
where $\frac{d^2E}{dk^2}$ represents the curvature of the $E-k$ relationship.
Step 3: Detailed Explanation:
• From the definition, $m^*$ is inversely proportional to the second derivative of energy with respect to the wavevector, which is the curvature of the $E-k$ curve.
• A higher curvature means a smaller effective mass, and vice versa.
• In solid-state physics, a wider energy band (higher bandwidth) corresponds to stronger overlap of atomic wavefunctions, which leads to a more dispersive curve (larger curvature).
• Thus, larger bandwidth leads to smaller effective mass, meaning $m^*$ is also inversely proportional to the bandwidth.
Step 4: Final Answer:
The effective mass is inversely related to both the curvature of the E-k diagram and the bandwidth, corresponding to Option (B).