In this paper we study the number of states with given spin for identical particles, denoted as
DIn(l) for bosons and as
DIn(j) for fermions, where
I is the total angular momentum of the system,
n is the particle number,
l is the spin of a single boson, and
j is the spin of a single fermion. We derive relations of
DIn(l) and
DIn(j); in particular, we obtain recursive and explicit formulas of
DIn(l) and
DIn(j) in terms of those for $n\ensuremath{-}1$ particles and apply them to systems of two, three, and five identical particles.
In quantum mechanics, elementary particles of the same type are considered identical. For example, an electron in an atom could be replaced by another electron and the atom would behave in exactly the same way. Nature has taken particular advantage of this, allowing only two types of elementary particles: bosons and fermions. They differ fundamentally in how a collection of identical particles interact. Identical fermions cannot occupy the same quantum state (only one per state!). Identical bosons can occupy the same quantum state. The statistics of identical particles (how they act in groups) has profound affects. For example, the rich and complex structure of the periodic table arises from the principle that only one electron can occupy each quantum state. The spin and the statistics of particles are closely connected: (fermions) bosons have (half-)integer spin. (Spin is an internal angular momentum measured in units of Planck’s constant.)