Features
Typical SHRIMP IIe flat-bottomed sample pit
Features
Small size of standard SHRIMP Samples
Features
Ion Beam Path for SHRIMP IIe
Features
SHRIMP IIe Single Collector, with electron multiplier and Faraday cup
Features
SHRIMP IIe Multicollector - completely reconfigurable under vacuum

Features

Primary Ion Beam



  • Independent control of primary and extracted beam energies and polarities.
  • 45 degree angle primary beam incident angle for efficient Sputtering of sample.
  • Hollow cathode duoplasmatron ion source designed at Cambridge University (UK) especially for ion probe applications - dual polarity - exceptionally bright and stable.
  • Option of Cesium gun for analysis of oxygen and electron gun for source neutralisation.
  • Wien filter for mass filtering of primary ion beam - adjustable resolution - may be turned off to maximize sputtering rates.
  • Kohler focussing provides radially ion flux on the primary beam.
  • Beam diameter variable from 5µm to 30µm.
  • Beam diameter and brightness adjusted independently.
  • Sharply defined, flat-bottomed pits.

Sample Stage



  • Standard 25mm diameter sample mounts - Thin section holder or large diameter mega-mount options.
  • Fully automated sample transfer.
  • Total computer control of sample stage movements - Multiple sample coordinates can be stored and revisited.
  • Visual optics permit viewing of sample stage during analysis - Variable magnification - Colour CCD camera/video monitor.
  • Up to three samples at one time can be stored in the vacuum lock In addition, two more samples can be placed in the specimen chamber, allowing for the easy comparison of a standard with an unknown.

Seconday Ion Beam



  • 90 degree angle extraction of the secondary beam to minimise instrumental discrimination.
  • Large apeture eliminates sample-to-sample memory Low field gradient extraction minimizes inter-element discrimination.
  • Triple quadrupole lens matching of secondary beam for maximum transmission.
  • Simultaneous collection of secondary and mass analysed beams for maximum precision of analysis.
  • Large (1272 mm) radius electrostatic analyser.
  • Rotatable source slit, width continuously variable from 5µm to 150µm.
  • Isotopic mapping of samples accomplished by rastering sample beneath primary beam.
  • Elegant, simple integrated ion lens system minimizes beam abberations and simplifies operation.
  • High mass dispersion achieved with large (1000mm) radius sector electromagnet.
  • Very stable, high speed laminated electromagnet controlled by multiple Hall Effect probes
  • Resolution > 5000 (1% definition) with flat-tops for 80µm source slit and 100µm collector slit.
  • Sensitivity better than 18cps/ppm/206Pb/nA 02- under above conditions

Single Collector



  • Rotatable collector slit, width continuously variable from ~5µm to 300µm.
  • Ion counting with robust, high gain, high speed electron multiplier, or
  • Ion current measurement via Faraday cup and electrometer.
  • Advanced, low-noise electrometers, with computer-configurable gain and settling time.


Multi-Collector (option)



  • Five channels of Faraday cups or electron multipliers.
  • Fully reconfigurable under vacuum; no lost time in re-pumping.
  • Most variables adjustable under computer control (slit size, head spacing, focus).


Instrument Control



  • PC platform standard.
  • Entire vacuum system under microprocessor control.
  • Highly intuitive, easy-to-use graphically orientated operation of entire machine.
  • Remote operation via the web, allowing monitoring or real-time control.
  • Optional Automated operation for unattended operation and sample pre-screening.