Typical SHRIMP IIe flat-bottomed sample pit
Small size of standard SHRIMP Samples
Ion Beam Path for SHRIMP IIe
SHRIMP IIe Single Collector, with electron multiplier and Faraday cup
SHRIMP IIe Multicollector - completely reconfigurable under vacuum
Features
Primary Ion Beam
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Independent control of primary and extracted beam energies and
polarities.
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45 degree angle primary beam incident angle for efficient Sputtering of
sample.
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Hollow cathode duoplasmatron ion source designed at Cambridge
University (UK) especially for ion probe applications - dual polarity -
exceptionally bright and stable.
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Option of Cesium gun for analysis of oxygen and electron gun for source
neutralisation.
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Wien filter for mass filtering of primary ion beam - adjustable
resolution - may be turned off to maximize sputtering rates.
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Kohler focussing provides radially ion flux on the primary beam.
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Beam diameter variable from 5µm to 30µm.
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Beam diameter and brightness adjusted independently.
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Sharply defined, flat-bottomed pits.
Sample Stage
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Standard 25mm diameter sample mounts - Thin section holder or large
diameter mega-mount options.
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Fully automated sample transfer.
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Total computer control of sample stage movements - Multiple sample
coordinates can be stored and revisited.
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Visual optics permit viewing of sample stage during analysis - Variable
magnification - Colour CCD camera/video monitor.
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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
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90 degree angle extraction of the secondary beam to minimise
instrumental discrimination.
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Large apeture eliminates sample-to-sample memory Low field gradient
extraction minimizes inter-element discrimination.
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Triple quadrupole lens matching of secondary beam for maximum
transmission.
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Simultaneous collection of secondary and mass analysed beams for
maximum precision of analysis.
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Large (1272 mm) radius electrostatic analyser.
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Rotatable source slit, width continuously variable from 5µm to 150µm.
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Isotopic mapping of samples accomplished by rastering sample beneath
primary beam.
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Elegant, simple integrated ion lens system minimizes beam abberations
and simplifies operation.
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High mass dispersion achieved with large (1000mm) radius sector
electromagnet.
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Very stable, high speed laminated electromagnet controlled by multiple
Hall Effect probes
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Resolution > 5000 (1% definition) with flat-tops for 80µm source
slit and 100µm collector slit.
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Sensitivity better than 18cps/ppm/206Pb/nA
02- under above conditions
Single Collector
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Rotatable collector slit, width continuously variable from ~5µm to
300µm.
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Ion counting with robust, high gain, high speed electron multiplier, or
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Ion current measurement via Faraday cup and electrometer.
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Advanced, low-noise electrometers, with computer-configurable gain and
settling time.
Multi-Collector (option)
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Five channels of Faraday cups or electron multipliers.
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Fully reconfigurable under vacuum; no lost time in re-pumping.
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Most variables adjustable under computer control (slit size, head
spacing, focus).
Instrument Control
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PC platform standard.
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Entire vacuum system under microprocessor control.
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Highly intuitive, easy-to-use graphically orientated operation of
entire machine.
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Remote operation via the web, allowing monitoring or real-time control.
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Optional Automated operation for unattended operation and sample
pre-screening.