Suppose now that the energy of state | 1 ⟩ ⟩ is slightly greater than the energy of state | 0 ⟩ ⟩ by an amount E. At temperature T, a particle will have a lesser probability to be in state | 1 ⟩ ⟩ by e − − E / k T . In the distinguishable case, the particle distribution will be biased slightly towards state | 0 ⟩ ⟩ . But in the indistinguishable case, since there is no statistical pressure toward equal numbers, the most-likely outcome is that most of the particles will collapse into state | 0 ⟩ ⟩ .