TY - JOUR
T1 - Transverse stability in a Stark decelerator
AU - van de Meerakker, S.Y.T.
AU - Vanhaecke, N.
AU - Bethlem, H.L.
AU - Meijer, G.
PY - 2006
Y1 - 2006
N2 - The concept of phase stability in a Stark decelerator ensures that polar molecules can be accelerated, guided, or decelerated without loss; molecules within a certain position and velocity interval are kept together throughout the deceleration process. In this paper the influence of the transverse motion on phase stability in a Stark decelerator is investigated. For typical deceleration experiments-i.e., for high values of the phase angle phi(0)-the transverse motion considerably enhances the region in phase space for which phase stable deceleration occurs. For low values of phi(0), however, the transverse motion reduces the acceptance of a Stark decelerator and unstable regions in phase space appear. These effects are quantitatively explained in terms of a coupling between the longitudinal and transverse motion. The predicted longitudinal acceptance of a Stark decelerator is verified by measurements on a beam of OH (X (2)Pi(3/2),J=3/2) radicals passing through a Stark decelerator.
AB - The concept of phase stability in a Stark decelerator ensures that polar molecules can be accelerated, guided, or decelerated without loss; molecules within a certain position and velocity interval are kept together throughout the deceleration process. In this paper the influence of the transverse motion on phase stability in a Stark decelerator is investigated. For typical deceleration experiments-i.e., for high values of the phase angle phi(0)-the transverse motion considerably enhances the region in phase space for which phase stable deceleration occurs. For low values of phi(0), however, the transverse motion reduces the acceptance of a Stark decelerator and unstable regions in phase space appear. These effects are quantitatively explained in terms of a coupling between the longitudinal and transverse motion. The predicted longitudinal acceptance of a Stark decelerator is verified by measurements on a beam of OH (X (2)Pi(3/2),J=3/2) radicals passing through a Stark decelerator.
U2 - 10.1103/PhysRevA.73.023401
DO - 10.1103/PhysRevA.73.023401
M3 - Article
SN - 1050-2947
VL - 73
JO - Physical Review A. Atomic, Molecular and Optical Physics
JF - Physical Review A. Atomic, Molecular and Optical Physics
IS - 2
ER -