Coulomb Crystals in a Cryogenic Paul Trap for Sympathetic Cooling of Molecular Ions and Highly Charged Ions

被引:2
作者
Windberger, A. [1 ]
Schwarz, M. [1 ]
Versolato, O. O. [1 ]
Baumann, T. [1 ]
Bekker, H. [1 ]
Schmoeger, L. [1 ]
Hansen, A. K. [2 ]
Gingell, A. D. [2 ]
Klosowski, L. [2 ]
Kristensen, S. [2 ]
Schmidt, P. O. [3 ]
Ullrich, J. [1 ,3 ]
Drewsen, M. [2 ]
Lopez-Urrutia, J. R. Crespo [1 ]
机构
[1] Max Planck Inst Kernphys, Saupfercheckweg 1, D-69117 Heidelberg, Germany
[2] Aarhus Univ, Dept Phys & Astron, Ion Trap Grp, DK-8000 Aarhus, Denmark
[3] Physikal Tech Bundesanstalt, D-38116 Braunschweig, Germany
来源
NON-NEUTRAL PLASMA PHYSICS VIII | 2013年 / 1521卷
关键词
Coulomb crystal; highly charged ion; alpha variation; ion clock; ion trap; spectroscopy; cryogenic; Paul trap; EBIT; sympathetic cooling; laser cooling; MgH ion; rotational cooling; STRONGLY COUPLED PLASMAS;
D O I
10.1063/1.4796081
中图分类号
O59 [应用物理学];
学科分类号
摘要
Electron beam ion traps used for spectroscopy of highly charged ions (HCI) produce a deep trapping potential leading to high temperatures of the stored ions, and thus limiting the achievable spectral resolution. A novel device at the Max-Planck-Institut fur Kernphysik, the Cryogenic linear Paul Trap Experiment (CryPTEx), attached to an electron beam ion trap, provides a new experimental platform to overcome these limitations. The trap assembly operates at a temperature of 4 K and offers optical access for quantum manipulation and imaging of the trapped ions. Since forbidden optical transitions in HCI do not support direct laser cooling, sympathetic cooling with Coulomb crystals of singly charged ions such as Be+ or Mg+ will be applied in order to reach the natural linewidth of optical forbidden transitions in HCI of interest. With the added advantage of long ion trapping times resulting from residual gas pressures of H-2 at 4 K below 10(-15) mbar, CryPTEx has been commissioned in collaboration with the Ion Trap Group in angstrom rhus using rovibrationally cooled MgH+ ions. Strong suppression of the black body radiation at the trap center, ion storage times of about 28 hours, and largely enhanced population of the rovibrational ground state were achieved.
引用
收藏
页码:250 / 256
页数:7
相关论文
共 19 条
[1]  
Baumann T M, 2012, THESIS
[2]   Highly charged ions with E1, M1, and E2 transitions within laser range [J].
Berengut, J. C. ;
Dzuba, V. A. ;
Flambaum, V. V. ;
Ong, A. .
PHYSICAL REVIEW A, 2012, 86 (02)
[3]   Transitions in Zr, Hf, Ta, W, Re, Hg, Ac, and U ions with high sensitivity to variation of the fine-structure constant [J].
Berengut, J. C. ;
Dzuba, V. A. ;
Flambaum, V. V. .
PHYSICAL REVIEW A, 2011, 84 (05)
[4]   Electron-Hole Transitions in Multiply Charged Ions for Precision Laser Spectroscopy and Searching for Variations in α [J].
Berengut, J. C. ;
Dzuba, V. A. ;
Flambaum, V. V. ;
Ong, A. .
PHYSICAL REVIEW LETTERS, 2011, 106 (21)
[5]   Towards sympathetic cooling of trapped ions with laser-cooled Mg+ ions for mass spectrometry and laser spectroscopy [J].
Cazan, Radu ;
Geppert, Christopher ;
Noertershaeuser, Wilfried ;
Sanchez, Rodolfo .
HYPERFINE INTERACTIONS, 2010, 196 (1-3) :177-189
[6]   Frequency Comparison of Two High-Accuracy Al+ Optical Clocks [J].
Chou, C. W. ;
Hume, D. B. ;
Koelemeij, J. C. J. ;
Wineland, D. J. ;
Rosenband, T. .
PHYSICAL REVIEW LETTERS, 2010, 104 (07)
[7]   Highly charged ions [J].
Gillaspy, JD .
JOURNAL OF PHYSICS B-ATOMIC MOLECULAR AND OPTICAL PHYSICS, 2001, 34 (19) :R93-R130
[8]   Formation of strongly coupled plasmas from multi-component ions in a penning trap [J].
Gruber, L ;
Holder, JP ;
Schneider, D .
PHYSICA SCRIPTA, 2005, 71 (01) :60-107
[9]   Evidence for highly charged ion Coulomb crystallization in multicomponent strongly coupled plasmas [J].
Gruber, L ;
Holder, JP ;
Steiger, J ;
Beck, BR ;
DeWitt, HE ;
Glassman, J ;
McDonald, JW ;
Church, DA ;
Schneider, D .
PHYSICAL REVIEW LETTERS, 2001, 86 (04) :636-639
[10]   THE LAMB SHIFT IN HYDROGEN-LIKE ATOMS, 1 LESS-THAN-OR-EQUAL-TO Z LESS-THAN-OR-EQUAL-TO 110 [J].
JOHNSON, WR ;
SOFF, G .
ATOMIC DATA AND NUCLEAR DATA TABLES, 1985, 33 (03) :405-446