
Paramagnetic substances are characterized by their magnetic susceptibility ($\chi$) at temperatures above any ordering transition (like the ferromagnetic Curie temperature, $T_C$). Their behavior is typically described by the Curie's Law.
Curie's Law states that the magnetic susceptibility ($\chi$) of a paramagnetic material is inversely proportional to the absolute temperature ($T$) in Kelvin:
$ \chi = \frac{C}{T} $
Here, $C$ is the Curie constant, a material-specific positive constant.
To find the relationship for reciprocal susceptibility ($\frac{1}{\chi}$), we can rearrange Curie's Law:
$ \frac{1}{\chi} = \frac{T}{C} $
This equation shows a direct linear relationship between $\frac{1}{\chi}$ and $T$. The plot of $\frac{1}{\chi}$ versus $T$ should be a straight line.
The plot matching this description is shown in Option 3:

| List - I | List - II |
|---|---|
| A. Bloch wall | I. Directs the magnetisation along directions of easy magnetisaton |
| B. Anisotropy energy | II. Above which the susceptibility of a ferromagnetic material obeys Curie-Weiss Law |
| C. Magnon | III. Separates domains magnetised in different directions |
| D. Curie Temperature | IV. Quantised spin wave |
Match List - I with List - II.
| List - I (System) | List - II (Density of States) |
|---|---|
| A. Bulk semiconductor | I. ![]() |
| B. Quantum well | II. ![]() |
| C. Quantum wire | III. ![]() |
| D. Quantum dot | IV. ![]() |
Choose the correct answer from the options given below :
| List - I (Type) | List - II (Examples) |
|---|---|
| A. Diamagnetic Materials | I. Aluminium, Sodium, Calcium |
| B. Paramagnetic Materials | II. $\text{SrTiO}_{3-x}$, $\text{LiTi}_{2}\text{O}_{4}$, $\text{Ba}(\text{Pb, Bi})\text{O}_{3}$ |
| C. Ferromagnetic Materials | III. Bismuth, Copper, lead |
| D. High temperature superconductors | IV. Alnico |
| List - I | List - II |
|---|---|
| A. Young's Modulus | I. $\frac{-\text{V}\text{d}\text{P}}{\text{d}\text{V}}$ |
| B. Bulk Modulus | II. $\frac{-\Delta\text{d}/\text{d}}{\Delta\text{L}/\text{L}}$ |
| C. Modulus of Rigidity | III. $\frac{\text{FL}}{\text{A}\Delta\text{L}}$ |
| D. Poisson Ratio | IV. $\frac{\text{F}/\text{A}}{x/h}$ |