Step 1: Identify the physical quantities. Here \(n\) is the number density of atoms/molecules, \(\alpha\) is the atomic (electronic) polarizability, \(\epsilon_0\) is the permittivity of free space, and \(\epsilon_r\) is the relative permittivity (dielectric constant).
Step 2: The relation links the macroscopic dielectric constant \(\epsilon_r\) to the microscopic polarizability \(\alpha\) by accounting for the local (Lorentz) field inside the dielectric: \[\frac{\epsilon_r - 1}{\epsilon_r + 2} = \frac{n\alpha}{3\epsilon_0}.\]
Step 3: This bridge between micro and macro properties is the Clausius-Mossotti relation. (Its optical form, using refractive index \(n_r^2 = \epsilon_r\), is the Lorentz-Lorenz equation.)
Step 4: The other names refer to unrelated results (Debye relaxation, Einstein-Debye specific heat, Bose-Einstein statistics), so they are ruled out.\[\boxed{\text{Clausius-Mossotti relation}}\]