Resonance Fluorescence Intensity Research Articles

Determination of atomic oscillator strengths using resonance absorption with a Döppler line source: transitions of Br and I (n+ 1)s–np5

A new general method is described for the determination of atomic transition probabilities using measurements of absorption intensity as a function of ground state atom concentration. The source for absorption measurements is resonance fluorescence emitted under optically thin conditions. The emission (and absorption) line profiles approximate closely to those for a Doppler line at 300 K under the conditions used. Known concentrations of Br 4p52P atoms for these (and fluorescence) studies, were produced by the two rapid reactions, O 3PJ+ Br2→ BrO + Br, O 3PJ+ BrO → O2+ Br.Values for the oscillator strengths, ƒ(λ nm), of various transitions of Br 4p52P are reported: ƒ(157.7)=(1.16 ± 0.08)× 10–3; ƒ(154.1)=(4.88 ± 0.59)× 10–2; ƒ(148.9)=(4.13 ± 0.39)× 10–2. These data were combined with resonance fluorescence intensity ratio measurements to give ƒ values for the corresponding transitions to the 4p52P½ state of Br: ƒ(163.4)=(6.4 ± 1.2)× 10–3; ƒ(157.5)=(1.5 ± 0.5)× 10–2. The experimental results confirm theoretical determinations by Lawrence of the ƒ values for the 5s– 4p5 multiplet of Br.For I atom resonance, the source of radiation was I atom fluorescence (6s– 5p5) from the photolysis of ICl (X17 Σ+, v″= 0) with H λ 121.6 nm radiation. Absorption measurements were performed with known I atom concentrations generated by the rapid reaction, Cl + ICl → I + Cl2. ƒ values for two transitions to I 5p52P were determined: ƒ(178.3)=(4.52 ± 0.42)× 10–2; ƒ(183.0)=(1.67 ± 0.23)× 10–3. These results are in less good agreement, than those for Br, with the work of Lawrence.Investigations of Br atom resonance fluorescence have been made in a flow system at 300 K and near 200 N m–2 total pressure. For kinetic studies of ground state 4p52P bromine atoms using resonance fluorescence, the most useful transitions are the λ 157.7 nm 5s4P5/2– 4p52P and the λ 154.1 nm 5s4P– 4p52P lines. Use of certain lines which connect with the 4p52P½ state also has potential value because of the high oscillator strength of these lines combined with the absence of self-reversal of fluorescence in a system consisting of 4p52P atoms.

A `Level Crossing' Experiment in Mercury

A change of the intensity of resonance fluorescence may take place when Zeeman states of the excited level have the same energy. The fields at which these `level crossings' occur in 199Hg and 201Hg have been measured. Combined with recent determinations of the hyperfine coupling constants, the results yield values for gJ of the 3P1 states: gJ (199)=1.48634±0.00005, gJ (201)=1.48606±0.00015.