So, if T ≪ ≪ T c , the fraction ⟨ ⟨ n 0 ⟩ ⟩ N ≈ ≈ 1 , and if T ≫ ≫ T c , the fraction ⟨ ⟨ n 0 ⟩ ⟩ N ≈ ≈ 0 . At temperatures near to absolute 0, particles tend to condense in the fundamental state, which is the state with momentum p → → = 0 .