Step 1: When an atom emits a photon, momentum conservation gives the atom a recoil momentum equal in magnitude to the photon momentum. A photon of wavelength \(\lambda\) carries momentum \[p = \frac{h}{\lambda}.\]
Step 2: Write both recoil momenta: \[p_A = \frac{h}{\lambda_A} = \frac{h}{1500\ \text{nm}}, \qquad p_B = \frac{h}{\lambda_B} = \frac{h}{500\ \text{nm}}.\]
Step 3: Take the ratio; the constant \(h\) cancels: \[\frac{p_A}{p_B} = \frac{\lambda_B}{\lambda_A} = \frac{500}{1500} = \frac{1}{3}.\]
Step 4: Hence \(p_A:p_B = 1:3\).\[\boxed{p_A:p_B = 1:3}\]