“…Then φ o (x) := |ν x | is an eigenfunction of ∆ in C ∞ (Γ(q)\H 2 ) with eigenvalue δ(1 − δ) [31], and φ o ∈ L 2 (Γ(q)\H 2 ) if and only if δ Γ > 1/2. If we identity H 2 = SL 2 (R)/ SO (2), and ψ ∈ C c (Γ(q)\G) is SO (2) [8] established a uniform spectral gap for the smallest two Laplace eigenvalues on L 2 (Γ(q)\H 2 ) for all square-free q ∈ N with no small prime divisors; for some ǫ > 0, there are no eigenvalues between δ(1 − δ), which is known to be the smallest one, and δ(1 − δ) + ǫ. When δ ≤ 1 2 , the L 2 -spectrum of ∆ is known to be purely continuous [23], and the relevant spectral quantities are the resonances.…”