Multi-Cathode Source of Negative Ions by Cesium Sputtering (MC-SNICS)


Product Features
  • The MC-SNICS is capable of creating all negative ions across the periodic table except noble gases.
  • Sources typically function on the order of 1,000 before requiring maintenance, except for cathode wheel change.
  • Cathode wheel change time is within one hour from beam on target to beam on target.
  • Indexing system is capable of reproducing cathode position to within 0.05 mm of original position.
  • Allows repeat measurements within a batch of cathodes in any sequence.

The NEC MC-SNICS (Multi-Cathode Source of Negative Ions by Cesium Sputtering) is most commonly used in Accelerator Mass Spectrometry (AMS) systems to generate negative ions. Contact us to learn more.

Applications

NEC manufactures negative ion sources for a variety of applications. The Multi-Cathode Source of Negative Ions by Cesium Sputtering (MC-SNICS) was originally developed as a reliable sputter source for applications that required rapid cathode change and precise, repeatable positioning without cathode exposure to air. This source is most commonly used in AMS systems for the production of beams such as C, Be, I, Ca, Cl, and the actinides. Like the SNICS, it can create ion beams from all elements that form a stable negative ion.

 

How It Works

The MC-SNICS principle of operation is very similar to the single cathode SNICS source, with the exception of using a spherical ionizer instead of a conically shaped ionizer. Here’s how it works.

Diagram of operation of the SNICS source  

  • Cesium vapor flows from the cesium oven into an enclosed area between the cooled cathode and the heated spherical ionizing surface.
  • Most of the cesium is ionized by the hot surface, while some of the cesium condenses on the front of the cathode.
  • The ionized cesium sputters particles from the cathode through a condensed cesium layer on the cathode face.
  • Negative ions are propelled near the cathode surface and then accelerated back toward the ionizer.

MC-SNICS Design

The MC-SNICS uses the basic elements from the SNICS II ion source, with the addition of cathode indexing system that allows the change of cathodes without breaking vacuum. The indexing system features:

 

Options

There are two models of the MC-SNICS:

40 MC-SNICS

134 MC-SNICS

Though the MC-SNICS source is primarily designed for the use of solid samples, NEC offers a gas option that allows the input of carbon dioxide behind a hollow titanium cathode assembly. This is available for both the 40 MC-SNICS and 134 MC-SNICS models.

 

Configurations

A typical MC-SNICS system includes:

NEC can provide just the source, a complete injector system, or anything in-between. Contact NEC for more information on MC-SNICS injector systems.

Accessories

NEC also offers manual and electric cathode presses to pack powdered elemental samples into cathodes suitable to generate negative ion beams. Contact NEC for more information.

MC-SNICS Performance

The beam emittance is on the order of 5 πmm mR (MeV)1/2 for optimum transmission through a tandem electrostatic accelerator with proper optics.

Examples of Negative Ion Beams Produced by the MC-SNICS

Negative Ion Current after analysis
Carbon >100μA
Aluminum >200nA
Beryllium >1.5μA
Iodine ~1μA
Chlorine 30μA
Calcium 80nA

This list is based on data from the NEC factory and contributing laboratories. All ion beam currents listed are measured after 30° or 45° mass analysis.

This is not a complete list of beams that can be produced by the MC-SNICS source. For beam current information for other elements, please contact NEC.


Related Documents
MC-SNICS v1
ECP-890 v1