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The classical dynamics of Rydberg Stark atoms in momentum space
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10.1119/1.2961081
/content/aapt/journal/ajp/76/11/10.1119/1.2961081
http://aip.metastore.ingenta.com/content/aapt/journal/ajp/76/11/10.1119/1.2961081
View: Figures

Figures

Image of Fig. 1.
Fig. 1.

(a) Heavy solid line: as a function of from Eq. (9b). Dashed line: as a function of from Eq. (9a). The electron’s motion is confined to the area defined by these parabolas. The light solid lines are numerical solutions of the classical equations of motion. (b) Heavy solid lines are as determined from Eqs. (10) and (11). The dashed lines (not visible on the scale of this plot) are as determined from Eq. (12) and differentiation of Eq. (9a). The parameters are , , and energy level . Light solid lines are numerical solutions to the classical equations of motion from which we find and ; these coordinates are defined in the text.

Image of Fig. 2.
Fig. 2.

The parameters are , , and . We find from the trajectory calculations that and . The different line styles are defined in Fig. 1.

Image of Fig. 3.
Fig. 3.

The parameters are , , and . We find from the trajectory calculations that and . The different line styles are defined in Fig. 1.

Image of Fig. 4.
Fig. 4.

Schematic of an electron’s trajectory and while precessing about the static electric field axis in (a) position space and (b) momentum space.

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/content/aapt/journal/ajp/76/11/10.1119/1.2961081
2008-11-01
2014-04-17
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: The classical dynamics of Rydberg Stark atoms in momentum space
http://aip.metastore.ingenta.com/content/aapt/journal/ajp/76/11/10.1119/1.2961081
10.1119/1.2961081
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