Step 1: Recall specific heat dependence in metals.
At low temperatures, the heat capacity of a metal has two contributions:
\[
C_v = \gamma T + \beta T^3
\]
where
- $\gamma T$ = electronic contribution (linear in $T$),
- $\beta T^3$ = lattice contribution (phonons, Debye $T^3$ law).
Step 2: Rearrange to given form.
Dividing by $T$:
\[
\frac{C_v}{T} = \gamma + \beta T^2
\]
This is a straight line in $\frac{C_v}{T}$ vs $T^2$ plot, with
- Intercept = $\gamma$ (electronic term),
- Slope = $\beta$ (phonon contribution).
Step 3: Interpret the graph.
- The graph matches exactly the expected linear form.
- This confirms the presence of both electronic and lattice contributions $\Rightarrow$ material is a **metal**.
Step 4: Dimensionality check.
- Debye’s $T^3$ law is valid for **three-dimensional solids**.
- For 1D or 2D materials, phonon contributions follow different power laws ($T$ for 1D, $T^2$ for 2D).
- Since the data shows $T^3$ dependence $\Rightarrow$ it must be **3D**.
Step 5: Evaluate options.
(A) Metallic → Correct.
(B) Insulating → Wrong, because intercept $\gamma \neq 0$ shows metallic behavior.
(C) Three dimensional → Correct (phonon $T^3$ law).
(D) One dimensional → Wrong.
Final Answer:
\[
\boxed{\text{(A) and (C)}}
\]