
The density of states, $N(E)$, represents the number of electronic states per unit energy interval. For a free electron gas in $d$ dimensions, the density of states is generally given by the proportionality:
$N(E) \propto E^{(d/2 - 1)}$
In the specific case of two dimensions ($d=2$), the formula becomes:
$N(E) \propto E^{(2/2 - 1)} = E^{(1 - 1)} = E^0$
This implies that $N(E)$ is a constant value, independent of the energy $E$. Therefore, the graph representing the density of states as a function of energy should be a horizontal line.
The graph representing a constant density of states, independent of energy, corresponds to the correct relationship for a 2D free electron gas.
Crystal structures of two metals A and B are two-dimensional square lattices with same lattice constant $a$. Electrons in metals behave as free electrons. The Fermi surfaces corresponding to A and B are shown by solid circles in figures. 
The electron concentrations in A and B are $n_A$ and $n_B$, respectively. The value of $(\frac{n_B}{n_A})$ is
If $X$ is the dimensionality of a free electron gas, the energy ($E$) dependence of density of states is given by $E^{½X-Y}$, where $Y$ is ________.