Principles of the stored ion calorimeter

Journal of Applied Physics

Volumn 46, Issue 2, 1975, Pages 919-930

  Wineland, D J ^a   Dehmelt, H G ^a  

^a UNIVERSITY OF WASHINGTON   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

ION CALORIMETERS;

IONS;

EID: 0016470933     PISSN: 00218979     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.321602     Document Type: Article

References (37)

1. The total magnetron energy is dominantly potential energy and is negative if we choose the potential at the center of the trap to be zero.
2. Actually a less restrictive criterion is needed; see, for example
3. See also
4. One can examine a simpler problem which illustrates the general features discussed here. Consider two electrons which are confined to move along the z axis by spring constants which may be different.
5. Collisions and inhomogeneous field excitation could play a role but for the conditions achieved here these effects were negligible.
6. Cyclotron transitions were induced by microwave radiation from a resonant slot in the ring electrode which terminates a section of K-band wave guide (not shown in Fig. 1).
7. It is important that we do not excite the CM directly by parametric drive.
8. See, for example