Thermalization of199Hg ion macromotion by a light background gas in an RF quadrupole trap

The largest systematic uncertainty in the performance of atomic frequency standards using a cloud of ions stored in an rf quadrupole trap is the second-order Doppler shift which depends on ion temperature and trapping parameters. This paper presents evidence that cooling the ions by collisions with atoms of a background gas light compared to the ions results in the condensation of the ions into a cloud of almost uniform density determined by space charge versus potential well forces. In this condition the second-order Doppler shift is simple to calculate and is found to depend only on readily measured characteristics of the ion cloud. This along with already observed good signal-to-noise ratio shows that the frequency standard we have constructed using the hyperfine splitting of singly ionized199Hg, with helium cooling can have an order of magnitude better performance in accuracy, stability, and reproducibility than presently available commercial cesium beam standards.

[1]  F. G. Major,et al.  Absolute measurement of the total number of ions stored in an RF quadrupole trap , 1981 .

[2]  R. F. Wuerker,et al.  Electrodynamic Containment of Charged Particles , 1959 .

[3]  D. Church Storage‐Ring Ion Trap Derived from the Linear Quadrupole Radio‐Frequency Mass Filter , 1969 .

[4]  M. Hohenstatt,et al.  "Optical-sideband Cooling of Visible Atom Cloud Confined in Parabolic Well" , 1978 .

[5]  J. Todd,et al.  The quadrupole ion store (QUISTOR). Part XI. The model of ion motion in a pseudo-potential well: An appraisal in terms of phase-space dynamics , 1980 .

[6]  R. Petsch,et al.  Precision determination of the ground-state hyperfine separation inHg+199using the ion-storage technique , 1978 .

[7]  R. Iffländer,et al.  Optical Detection of Ions Confined in a rf Quadrupole Trap , 1977 .

[8]  H. Schuessler,et al.  Investigation of the production of singly charged ions in a rf quadrupole ion trap , 1979 .

[9]  F. G. Major,et al.  High-Resolution Magnetic Hyperfine Resonance in Harmonically Bound Ground-State Hg 199 Ions , 1973 .

[10]  H. Dehmelt,et al.  Radiative Cooling of an Electrodynamically Contained Proton Gas , 1969 .

[11]  R. Dicke The effect of collisions upon the Doppler width of spectral lines , 1953 .

[12]  M. A. Biondi,et al.  Mobilities of Mercury Ions in Helium, Neon, and Argon , 1957 .

[13]  E. W. McDaniel,et al.  Collision phenomena in ionized gases , 1964 .

[14]  H. Dehmelt,et al.  Radiofrequency Spectroscopy of Stored Ions I: Storage , 1968 .

[15]  J. R. Pierce,et al.  Scientific foundations of vacuum technique , 1949 .

[16]  G. Werth,et al.  Trapped ion density distribution in the presence of He-buffer gas , 1981 .

[17]  M. Mcguire,et al.  Penning-trap technique for studying electron-atom collisions at low energy , 1974 .

[18]  Robin P. Giffard,et al.  Mercury-199 Trapped Ion Frequency Standard: Recent Theoretical Progress and Experimental Results , 1983 .

[19]  M. Stuke,et al.  Hyperfine density shifts of137Ba+ ions in noble gas buffers , 1975 .

[20]  Claude Audoin,et al.  Frequency stability of a mercury ion frequency standard , 1981 .

[21]  R. D. Knight,et al.  Laser scanning measurement of the density distribution of confined 6Li+ ions , 1979 .

[22]  F. G. Major,et al.  Exchange-Collision Technique for the rf Spectroscopy of Stored Ions , 1968 .