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Thermal ionization cavity source

Schematic representation of a thermal ionization cavity source. Schematic representation of a thermal ionization cavity source.
Wayne DM, Hang W, McDaniel DK, Fields RE, Rios E, Majidi V (2002) The thermal ionization cavity (TIC) source elucidation of possible mechanisms for enhanced ionization efficiency. Inti J Mass Spectrom 216 41-57... [Pg.59]

Buerger, S., et al. (2007) A high efficiency cavity ion source using thermal ionization mass spectrometry (TIMS) for nuclear forensic analysis. Journal of Alloys and Compounds, 444-445, 660-662. [Pg.472]

Fig. 10.2 Major components of a thermal atomic beam apparatus for microwave ionization experiments,the atomic source, the microwave cavity, and the electron multiplier. The microwave cavity is shown sliced in half. The Cu septum bisects the height of the cavity. Two holes of diameter 1.3 mm are drilled in the side walls to admit the collinear laser and Na atomic beams, and a 1 mm hole in the top of the cavity allows Na+ resulting from a field ionization of Na to be extracted. Note the slots for pumping (from ref. 4). Fig. 10.2 Major components of a thermal atomic beam apparatus for microwave ionization experiments,the atomic source, the microwave cavity, and the electron multiplier. The microwave cavity is shown sliced in half. The Cu septum bisects the height of the cavity. Two holes of diameter 1.3 mm are drilled in the side walls to admit the collinear laser and Na atomic beams, and a 1 mm hole in the top of the cavity allows Na+ resulting from a field ionization of Na to be extracted. Note the slots for pumping (from ref. 4).
See other pages where Thermal ionization cavity source is mentioned: [Pg.11]    [Pg.67]    [Pg.35]    [Pg.178]    [Pg.14]    [Pg.1152]    [Pg.174]   
See also in sourсe #XX -- [ Pg.11 ]



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