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Production of a single spin-rotational state selected molecular oxygen beam by a hexapole magnet
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10.1063/1.3206299
/content/aip/journal/rsi/80/8/10.1063/1.3206299
http://aip.metastore.ingenta.com/content/aip/journal/rsi/80/8/10.1063/1.3206299
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) The SG spectra measured for supersonic seeded beams at the stagnation pressures shown. The solid (broken) lines correspond to the nonflip (flip) modes of the flipper. The velocity distributions of the corresponding beam are shown in (b). The dashed lines in (a) and (b) are drawn to guide the eyes. The SG deflection spectra and the velocity distribution measured for the beam are shown in (c) and (d), respectively.

Image of FIG. 2.
FIG. 2.

The trajectories of the molecules from the beam source to the defining aperture (A1) simulated for the spin-rotational states shown. The beam velocity is 900 m/s. The solid and dashed lines correspond to the cases in which the beam enters the hexapole magnet with different angles.

Image of FIG. 3.
FIG. 3.

The SG spectra of (a) and (b) at the transverse coil current shown.

Image of FIG. 4.
FIG. 4.

The intensity of the , 0, peaks (a) and the peaks (b) as a function of . The solid lines correspond to those derived from the Majorana’s formula [Eqs. (1) and (2)]. See text for details.

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/content/aip/journal/rsi/80/8/10.1063/1.3206299
2009-08-24
2014-04-18
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752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Production of a single spin-rotational state [(J,M)=(2,2)] selected molecular oxygen (Σ3g−) beam by a hexapole magnet
http://aip.metastore.ingenta.com/content/aip/journal/rsi/80/8/10.1063/1.3206299
10.1063/1.3206299
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