Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Log inSign up
Challenges
Datasets
Workspaces
Papers
Discussions
Leaderboard
Blog
Job Board
Q3AS

© 2026 Aqora Quantum S.A.S.

TermsPrivacyLegal Notice

Role of the collision induced transitions between electronic states for the surface ionisation of the Xe Rydberg atoms

Jelena Sjakste, Andrei G. Borisov, J.P. Gauyacq

Published Jan 1, 2005• 0 citations
OpenAlex

Related papers

Ionisation of Rydberg atoms colliding on metal surfaces

J.P. Gauyacq, Jelena Sjakste, Andrei G. Borisov

•Jan 1, 2006•0 citations

Ionization of Xe(nf) Rydberg Atoms at Surfaces: Effect of Stray Fields

Dennis Neufeld, Hardin Dunham, S. Wethekam +2 more

Bulletin of the American Physical Society•May 29, 2008•0 citations

Collisions of Xe(nf) Rydberg atoms with ammonia

F. G. Kellert, Greg W. Foltz, K. A. Smith +3 more

peac•Jan 1, 1979•0 citations

A study of n changing, l changing and ionisation in collisions of Xe(nf) Rydberg atoms with HF

C Higgs, K. A. Smith, G. B. McMillian +2 more

Thermal collisions between Xe(nf) Rydberg atoms and HF molecules have been investigated. The highly excited collision products were detected using selective field ionisation (SFI). Both n-changing and l-changing collisions were identified and the absolute rate constants for these processes, and for collisional ionisation, have been measured for n=26, 27. In addition, the first evidence of molecular rotational excitation through the transfer of energy of electronic excitation from a Rydberg atom is presented.

Journal of Physics B Atomic and Molecular Physics•Apr 28, 1981•22 citations

Collisional Ionization of Xe Atoms in Single High Rydberg States

W.P. West, Terri Cook, Colin J. Latimer +2 more

peac•Jan 1, 1975•0 citations

Fluorescence-lifetime-limited trapping of Rydberg helium atoms on a chip

Valentina Zhelyazkova, M. Žeško*, Hansjürg Schmutz +2 more

Metastable (1s)(2s) 3S1 helium atoms produced in a supersonic beam were excited to Rydberg-Stark states (with n in the 27–30 range) in a cryogenic environment and subsequently decelerated by, and trapped above, a surface-electrode decelerator. In the trapping experiments, the Rydberg atoms were brought to rest in 75 μs and over a distance of 33 mm and kept stationary for times ttrap in the 0–525 μs range, before being re-accelerated for detection by pulsed field ionisation. The use of a home-built valve producing short gas pulses with a duration of about 20 μs enabled the reduction of losses arising from collisions with atoms in the trailing part of the gas pulses. Cooling the decelerator to 4.7 K further suppressed losses by transitions induced by blackbody radiation and by collisions with atoms desorbing from the decelerator surface. The main contribution (60%) to the atom loss during deceleration is attributed to the escape out of the decelerator moving traps of atoms having energies higher than the trap saddle point, spontaneous emission and collisions with atoms in the trailing part of the gas pulses causing each only about 20% of the atom loss. At 4.7 K, the atom losses in the trapping phase of the experiments were found to be almost exclusively caused by spontaneous emission and the trap lifetimes were found to correspond to the natural lifetimes of the Rydberg-Stark states. Increasing the temperature to 100 K enhanced the trap losses by transitions stimulated by blackbody radiation.

arXiv:1904.07628•Molecular Physics•Apr 5, 2019•19 citations
Thermal collisions between Xe(nf) Rydberg atoms and HF molecules have been investigated. The highly excited collision products were detected using selective field ionisation (SFI). Both n-changing and l-changing collisions were identified and the absolute rate constants for these processes, and for collisional ionisation, have been measured for n=26, 27. In addition, the first evidence of molecular rotational excitation through the transfer of energy of electronic excitation from a Rydberg atom is presented.
Metastable (1s)(2s) 3S1 helium atoms produced in a supersonic beam were excited to Rydberg-Stark states (with n in the 27–30 range) in a cryogenic environment and subsequently decelerated by, and trapped above, a surface-electrode decelerator. In the trapping experiments, the Rydberg atoms were brought to rest in 75 μs and over a distance of 33 mm and kept stationary for times ttrap in the 0–525 μs range, before being re-accelerated for detection by pulsed field ionisation. The use of a home-built valve producing short gas pulses with a duration of about 20 μs enabled the reduction of losses arising from collisions with atoms in the trailing part of the gas pulses. Cooling the decelerator to 4.7 K further suppressed losses by transitions induced by blackbody radiation and by collisions with atoms desorbing from the decelerator surface. The main contribution (60%) to the atom loss during deceleration is attributed to the escape out of the decelerator moving traps of atoms having energies higher than the trap saddle point, spontaneous emission and collisions with atoms in the trailing part of the gas pulses causing each only about 20% of the atom loss. At 4.7 K, the atom losses in the trapping phase of the experiments were found to be almost exclusively caused by spontaneous emission and the trap lifetimes were found to correspond to the natural lifetimes of the Rydberg-Stark states. Increasing the temperature to 100 K enhanced the trap losses by transitions stimulated by blackbody radiation.