1992
DOI: 10.1088/0953-4075/25/22/018
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Energy pooling reactions between two Na* (3p) atoms specified according to magnetic substate combinations

Abstract: In a beam experiment the authors have studied the energy pooling reaction between two laser excited Na* (3p) atoms, where in the final state one of the sodium atoms is in the 5s or 4d state and the other in the ground state. They have determined all eight independent partial cross sections and coherence terms, specified according to the various magnetic substate combinations of the colliding Na* (3p) atoms, as a function of the collision velocity. This is the maximum information that can be extracted from the … Show more

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Cited by 9 publications
(4 citation statements)
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“…In our experiment the Na + 2 ions are produced via associative ionization in so-called headtail collisions between two Na(3 2 P 3/2 , F = 3) atoms in a single thermal Na beam. Our atomic beam configuration is based upon the experimental apparatus described by Meijer et al [13] and Nijland et al [14]. The associative ionization volume with dimensions x × y × z = 5 × 0.7 × 8 mm 3 is located between the grids G1 and G2 of the electrode system, displayed schematically in figure 4.…”
Section: Experimental Set-upmentioning
confidence: 99%
See 1 more Smart Citation
“…In our experiment the Na + 2 ions are produced via associative ionization in so-called headtail collisions between two Na(3 2 P 3/2 , F = 3) atoms in a single thermal Na beam. Our atomic beam configuration is based upon the experimental apparatus described by Meijer et al [13] and Nijland et al [14]. The associative ionization volume with dimensions x × y × z = 5 × 0.7 × 8 mm 3 is located between the grids G1 and G2 of the electrode system, displayed schematically in figure 4.…”
Section: Experimental Set-upmentioning
confidence: 99%
“…For a → transition the angular fragment distribution is given by Yang et al [16] G(θ) ∝ 1 + βP 2 (cos θ) (14) with θ the angle between the laser polarization axis and the recoil direction, β the socalled asymmetry parameter and P 2 the second Legendre polynomial. Kortyna et al [5] find experimentally β = 1.83 ± 0.17, in agreement with the theoretical value of 2.0 for low rotational temperatures.…”
Section: Recoilmentioning
confidence: 99%
“…The experimental set-up is shown schematically in figure 2. The apparatus has been described previously in [7,15] and has been used in beam experiments on associative ionization and energy pooling, respectively, in collisions between Na * (3p; 2 P 3/2 ) atoms. In the experiment discussed in this paper a single sodium beam is used, which intersects the exciting laser beams at right angles.…”
Section: Experimental Set-upmentioning
confidence: 99%
“…In principle, a complete analysis in the J -picture involves a very large set of partial cross sections and coherence terms. For a detailed discussion on these cross sections and coherence terms we refer to [15,18]. This set has already been reduced considerably by the transformation from the F -to the J-picture, using the reasonable assumption that the nuclear spin (I = 3…”
Section: Partial Cross Sectionsmentioning
confidence: 99%