[en] The q-analogue coherent states |z >_q are used to identify physical signatures for the presence of a q-analogue quantized radiation field in the | >_q classical limit where |z| is large. In this quantum-optics-like limit, the fractional uncertainties of most physical quantities (momentum, position, amplitude, phase) which characterize the quantum field are O(1). They only vanish as O(1/|z|) when q = 1. However, for the number operator, N, and the N-Hamiltonian for a free q-boson gas, H_N = ℎω(N + 1/2), the fractional uncertainties do still approach zero. A signature for q-boson counting statistics is that (ΔN)²/< N> → 0 as |z| → ∞. Except for its O(1) fractional uncertainty, the q-generalization of the Hermitian phase operator of Pegg and Barnett, φ_q, still exhibits normal classical behavior. The standard number-phase uncertainty-relation, ΔN Δφ_q = 1/2, and the approximate commutation relation, [N,φ_q] = i, still hold for the single-mode q-analogue quantized field. So, N and φ_q are almost canonically conjugate operators in the |z >_q classical limit. The |z >_q CS's minimize this uncertainty relation for moderate |z|²