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Physics of Electronic and Atomic Collisions: ICPEAC XI

Depolarization of 4 2 P potassium atoms induced in resonant collisions

P. Skalinski, L. Krause

Published Jan 1, 1979• 0 citations
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The mj mixing cross section for disorientation of magnetically 2 oriented potassium atoms in the 4 ^2/2 state» induced by collisions with ground state helium atoms, was measured using a modified Zeeman scanning technique.The mj substates of potassium atoms, situated in a strong magnetic field, were selectively excited and the collisionally induced mixing manifested itself by the depolarization of the potassium resonance fluorescence.The depolarization measurements yielded mixing cross -14 2 -14 2 sections ranging from 0.77 x 10 cm to 1.4 x 10 cm .It is felt that this discrepancy may be due to a selection rule for transitions between the fine structure states such that £nij = 0 is preferred.

•Jan 1, 1967•0 citations
A modified Zeeman scanning method was used to excite selectively the magnetic substates of the 42P124^{2}P_{\frac{1}{2}}42P21​​ potassium atoms mixed with inert gases and placed in a strong magnetic field. The resulting potassium-inert-gas atomic collisions induced mJ{m}_{J}mJ​ mixing in potassium, which manifested itself by the depolarization of the potassium resonance fluorescence. The polarization measurements yielded the following disorientation cross sections: K-He: 46 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-Ne: 39 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-A: 52 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-Kr: 80 A˚2{\mathrm{\AA{}}}^{2}A˚2; K-Xe: 107 A˚2{\mathrm{\AA{}}}^{2}A˚2.
The mj mixing cross section for disorientation of magnetically 2 oriented potassium atoms in the 4 ^2/2 state» induced by collisions with ground state helium atoms, was measured using a modified Zeeman scanning technique.The mj substates of potassium atoms, situated in a strong magnetic field, were selectively excited and the collisionally induced mixing manifested itself by the depolarization of the potassium resonance fluorescence.The depolarization measurements yielded mixing cross -14 2 -14 2 sections ranging from 0.77 x 10 cm to 1.4 x 10 cm .It is felt that this discrepancy may be due to a selection rule for transitions between the fine structure states such that £nij = 0 is preferred.