Bose-Einstein statistics describes one of the two possible ways in which a collection of indistinguishable particles can be distributed over various energy states in thermal equilibrium. These particles, known as bosons, do not obey the Pauli Exclusion Principle, which means that multiple bosons can occupy the same quantum state. This is fundamentally different from fermions, which adhere to the Fermi-Dirac statistics and cannot share the same state.
