What is Secondary Ion Mass Spectrometer (SIMS) ?
As a class, SIMS instruments (aka ion microprobes) use an internally generated beam of either positive (e.g., Cs) or negative (e.g., O) ions (primary beam) focused on a sample surface to generate ions that are then transferred into a mass spectrometer across a high electrostatic potential, and are referred to as secondary ions. In a similar technique, a beam of high-speed neutral atoms (e.g., Ar) can substitute for the primary ion beam, an approach used primarily for surface analysis of organic compounds that has few applications in the geosciences and is not discussed here.
Fundamental Principles of Secondary Ion Mass Spectrometer (SIMS)
The interaction of the primary ion beam with the sample (under vacuum) provides sufficient energy to ionize many elements. If the primary beam is composed of positively charged ions, the resultant ionization favors production of negative ions; primary beams of negative ions favor generation of positive ions. Although most atoms and molecules removed from the sample by the interaction of the primary beam and the sample surface (referred to as sputtering) are neutral, a percentage of these are ionized. These ions are then accelerated, focused, and analyzed by a mass spectrometer.
In “dynamic SIMS” mode the primary ion beam exceeds the “static limit” (~1E12 ions/cm2) producing a high yield of secondary ions. This technique is used for “bulk” analysis of elementsand isotopes, and is particularly well-suited for analysis of isotopes and trace elements in minerals (e.g. REE in garnet). Alternatively, “static SIMS” uses a much lower energy primary ion beam (usually Ga or Cs). This technique is typically used for analysis of atomic monolayers on material surfaces to obtain information about molecular species on material surfaces (e.g. organic compounds; see module on Time-of-Flight SIMS).
How Does It Work ?
There are several different designs of SIMS currently being manufactured commercially that have applications in the geosciences (e.g., Cameca’s 1280, 7f, and NanoSIMS, ASI’s SHRIMP and SHRIMP RG, EAG’s ToF SIMS). Most of these instruments are characterized by a source region in which the intensity, energy, and orientation of the primary beam (relative to the sample) are controlled. Ions generated by this process form the secondary beam and are subsequently transmitted within a continuous high vacuum environment to a mass spectrometer. Most SIMS instruments used for elemental and isotopic analyses function by accelerating ions produced in the source along a potential gradient, typically 10 KV, and then transferring these ions into the mass spectrometer. Details of the configuration of the mass spectrometer vary from one application to another, but all utilize both magnetic and electrostatic analyzers, commonly referred to as sectors. If the electrostatic analyzer (sector) precedes the magnetic sector, the design is referred to as forward geometry. The advantage of this configuration is that the electrostatic filter reduces the energy range of the secondary ions so that they can then be separated into independent ion beams (based on the charge/mass ratio) by passing them through a magnetic field (magnetic sector). In this configuration, multiple ion beams can be measured simultaneously. If the magnetic sector precedes the electrostatic sector (reverse geometry), then mass resolution is improved at the cost of losing the ability to measure multiple ion beams simultaneously. Other types of mass spectrometers can be coupled to the SIMS source, including quadrupole and time-of-flight analyzers. These latter configurations have fewer applications in the geosciences.
In geochemistry SIMS is the instrumentation of choice for several analytical tasks, most noteworthy are:
- Large radius forward and reverse geometry instruments have been developed that can measure trace elemental and isotopic compositions in individual minerals with a spatial resolution down to roughly 10 microns. These applications include U-Th-Pb geochronology of zircon and other accessory minerals (e.g., SHRIMP).
- Large radius, double focusing instruments are also capable of measuring the isotopic composition of low atomic number elements such as O with similar spatial resolution (e.g., Cameca 1280) or even less for major constituents (e.g., 50 nanometers; NanoSIMS by Cameca Instruments)
- Smaller radius, double focusing instruments offer very high sensitivity (detection limits) for trace element analyses, roughly 10x the sensitivity of microprobes that utilize beams of electrons (e.g., Cameca IM 7f). These instruments can also used to “map” the distribution of individual elements in a sample.
- Some SIMS utilize other types of mass spectrometers (e.g., time-of-flight, quadrupole) and are used primarily for surface characterization, molecular analysis, and depth profiling.
For more information about Secondary Ion Mass Spectrometer (SIMS) follow the links below.
- SIMS Theory Tutorial — from Evans Analytical Group
- SIMS Tutorials — Dept. of Geosciences, University of Edinburgh
- SIMS Facility — Sandia National Laboratory and University of New Mexico; Basics explained and Trace Element Analysis.
- The Wisconsin Secondary Ion Mass Spectrometry Lab–includes Powerpoint and PDF files on instrumentation and applications
- UCLA SIMS Facility — including information about sample preparation, U-Pb tutorial.
- USGS- Stanfard SHRIMP-RG Facility — sample preparation, applications, research results.
- Australian National University SHRIMP page
- Geological Survey of Canada SHRIMP II Facility
Teaching Activities and Resources
Teaching activities, labs, and resources pertaining to Secondary Ion Mass Spectrometer (SIMS):