Optimization of Raman Cooling of 25Mg+ Ion to Ground Vibrational State in Linear Paul Trap

2019 ◽  
Vol 46 (4) ◽  
pp. 138-142
Author(s):  
P. L. Sidorov ◽  
K. Yu. Khabarova ◽  
I. V. Zalivako ◽  
A. S. Borisenko ◽  
I. A. Semerikov
Keyword(s):  
Vibrational State ◽  
Paul Trap ◽  
Linear Paul Trap ◽  
Ground Vibrational State ◽  
Raman Cooling

scholarly journals Transport of ions in a segmented linear Paul trap in printed-circuit-board technology

2008 ◽  
Vol 10 (1) ◽  
pp. 013004 ◽  
Author(s):  
G Huber ◽  
T Deuschle ◽  
W Schnitzler ◽  
R Reichle ◽  
K Singer ◽  
...  
Keyword(s):  
Printed Circuit Board ◽  
Paul Trap ◽  
Circuit Board ◽  
Linear Paul Trap ◽  
Printed Circuit ◽  
Transport Of Ions

Excitation of transverse dipole and quadrupole modes in a pure ion plasma in a linear Paul trap to study collective processes in intense beams

2013 ◽  
Vol 20 (5) ◽  
pp. 055706 ◽  
Author(s):  
Erik P. Gilson ◽  
Ronald C. Davidson ◽  
Philip C. Efthimion ◽  
Richard Majeski ◽  
Edward A. Startsev ◽  
...  
Keyword(s):  
Paul Trap ◽  
Linear Paul Trap ◽  
Ion Plasma ◽  
Collective Processes

Speed dependence of collisional relaxation in ground vibrational state of OCS: Rotational behaviour

2012 ◽  
Vol 136 (12) ◽  
pp. 124316 ◽  
Author(s):  
Maxim A. Koshelev ◽  
Mikhail Yu. Tretyakov ◽  
François Rohart ◽  
Jean-Pierre Bouanich
Keyword(s):  
Vibrational State ◽  
Rotational Behaviour ◽  
Collisional Relaxation ◽  
Ground Vibrational State ◽  
Speed Dependence

scholarly journals Nonlinear Resonances of Laser Cooled Ions in a Linear Paul Trap due to the Anharmonicity of the Trap Potential

2003 ◽  
Vol 31 (7) ◽  
pp. 477-481 ◽  
Author(s):  
Toshihiko MORI ◽  
Kenji TOYODA ◽  
Masayoshi WATANABE ◽  
Shinji URABE
Keyword(s):  
Paul Trap ◽  
Linear Paul Trap ◽  
Nonlinear Resonances ◽  
Trap Potential

scholarly journals Double-well trap for charged microparticles

2021 ◽  
Vol 2103 (1) ◽  
pp. 012222
Author(s):  
Olga Kokorina ◽  
Vadim Rybin ◽  
Semyon Rudyi
Keyword(s):  
Experimental Data ◽  
Numerical Simulation ◽  
Strong Correlation ◽  
Paul Trap ◽  
Axial Position ◽  
Experimental Setup ◽  
Mass Ratio ◽  
Linear Paul Trap ◽  
Spatial Selection ◽  
Axial Density

Abstract We propose a double-well linear Paul trap for particle’s spatial selection according to the charge-to-mass ratio. To perform spatial selection we implemented an experimental setup that permits to detect particles’ positions in the double-well trap from three different view-points: top, front left, and front right. The setup gives an opportunity to monitor the particles’ axial density distribution in real-time. We have shown a strong correlation between axial position of separated localization areas and the DC voltages applied to the rod and end-cap electrodes. We have experimentally determined the critical localization parameters where double-well mode acquires for all the trapped charged microparticles. According to the experimental data and a numerical simulation a upper value of charge-to-mass ratio of the trapped microparticles was estimated.

scholarly journals Charged particle capturing in air flow by linear Paul trap

2018 ◽  
Vol 946 ◽  
pp. 012152
Author(s):  
D S Lapitsky ◽  
V S Filinov ◽  
V I Vladimirov ◽  
R A Syrovatka ◽  
L M Vasilyak ◽  
...  
Keyword(s):  
Charged Particle ◽  
Air Flow ◽  
Paul Trap ◽  
Linear Paul Trap

Millimeter Wave Rotational Transitions of 16O12C32S and 16O13C32S

1974 ◽  
Vol 29 (8) ◽  
pp. 1213-1215 ◽  
Author(s):  
N. W. Larsen ◽  
B. P. Winnewisser
Keyword(s):  
Excited States ◽  
Millimeter Wave ◽  
Vibrational Spectra ◽  
Vibrational State ◽  
Vibrational States ◽  
Ground Vibrational State ◽  
Wave Region ◽  
Rotational Transitions ◽  
Good Agreement

Rotational transitions of 16012C32S and 16013C32S in the ground vibrational state and of 16012C32S in several excited states have been accurately measured in the millimeter wave region for a minimum of four different J values. The analysis of the measured frequencies leads to rotational constants for the following vibrational states: 0 00 0 of 16O13C32S and 0 00 0, 0 1 1c 0, 0 1 1d 0, 0 20 0, 0 22c 0, 0 22d 0, 0 00 1 of 16O12C32S. Since the two components of the 0 22 0 transitions were resolved, an analysis of the l-type resonance was carried out and the interval 0 22 0 - 0 20 0 has been determined to be -4.63(10) cm-1. The result is in good agreement with the presently available determination of this level from vibrational spectra.

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