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EGAS41 - Swansea University

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41 st EGAS CP 190 Gdańsk 2009<br />

Reorientation, alignment and coherence effects in Ca-RG<br />

collisions<br />

E. Paul-Kwiek<br />

Institute of Physics, Pomeranian <strong>University</strong> in S̷lupsk, ul. Arciszewskiego 22,<br />

76-200 S̷lupsk, Poland<br />

∗ Corresponding author: ewa@.apsl.edu.pl,<br />

The main purpose of the present work is to perform a detailed analysis of the alignment,<br />

orientation and coherence effects in Ca(4s4p, 3 P j ) colliding with rare gas (RG) atoms.<br />

The calculations are based on the standard close-coupling formalism (used for example<br />

in [1,2]) with application the relevant pseudopotential curves of Czuchaj, Krośnicki, Stoll<br />

[3].<br />

σ ( 3 P j1 -> 3 P j2 ) [10 -16 cm 2 ]<br />

40<br />

Ca-He 1->2<br />

0->2<br />

30<br />

2->1<br />

20<br />

0->1<br />

10<br />

2->0<br />

1->0<br />

0<br />

0 .2 .4 .6 .8<br />

σ ( 3 P j1<br />

-> 3 P j2<br />

) [10 -16 cm 2 ]<br />

40<br />

30<br />

20<br />

10<br />

0<br />

Ca-Xe<br />

1->0<br />

1->2<br />

2->1<br />

0->2<br />

0->1<br />

2->0<br />

0 .2 .4 .6 .8<br />

Ek[eV]<br />

Ek[eV]<br />

Figure 1: Total integral cross-section for the Ca(4s4p, 3 P j1 − > 3 P j2 ) spin changing transitions<br />

induced by He and Xe as a function of translational energy.<br />

The reorientation effect and angular distribution of scattered calcium atoms associated<br />

with the inelastic transition j 1 m 1 → j 2 m 2 are discussed via multi-structure differential<br />

cross-sections<br />

dσ m1 →m 2<br />

(j 1 → j 2 ;k j1 ,R))<br />

dΩ<br />

= k j 2<br />

k j1<br />

| f j1 m 1 →j 2 m 2<br />

(k j1 ,R) | 2 , (1)<br />

where f j1 m 1 →j 2 m 2<br />

is the scattering amplitude and the vectors k j1 and R define the incident<br />

velocity and the scattering directions, respectively. The alignment effects are described<br />

by means of the conventional and coherence cross-sections<br />

σ m1 m ′ 1 →m 2m ′ 2 (j 1 → j 2 ;k j1 ) = k j 2<br />

k j1<br />

∫<br />

dˆRf j1 m 1 →j 2 m 2<br />

(k j1 ,R) · f ∗ j 1 m ′ 1 →j 2m ′ 2 (k j 1<br />

,R). (2)<br />

References<br />

[1] E. Paul-Kwiek, J. Phys. B At. Mol. Opt. Phys. 34, 285, (2001)<br />

[2] E. Paul-Kwiek, J. Phys. B At. Mol. Opt. Phys. 35, 175, (2002)<br />

[3] E. Czuchaj, M. Krośnicki, H. Stoll, Chemical Physics 292, 101 (2003)<br />

250

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