SIMS Measurements of Silicon Carbide

Silicon Carbide is a very important material for high-power, high-temperature, high-frequency and high-radiation devices due to its superior electronic and thermal properties. Dramatic progress in SiC-based power transistors, LEDs, and sensors have made it imperative to accurately control dopant and impurity levels.

Secondary Ion Mass Spectrometry (SIMS) has very high detection sensitivity for a variety of elements. Its unique profiling capability can provide quick and precise feedback in dopant level, junction depth, and impurity distribution in SiC sample, including patterned device structures. It is an essential tool for process control and problem solving in wafer growth and device manufacturing.

Silicon Carbide SIMS Measurements
Detection of Secondary Ions

BASICS OF SIMS ANALYSIS OF SiC

Primary Beam

Either oxygen (O2+) or cesium (Cs+) primary ion beams are used for SIMS analysis. The spot size of a focused primary ion beam is typically 2 to 20 μm. This primary beam is rastered over a square area, usually on the scale of up to several hundred microns on a side.

Detection of Secondary Ions

Secondary ions generated from the central portion of the rastered area are measured after being mass separated in a mass spectrometer. In magnetic sector SIMS instruments secondary ions can be detected using electron multipliers, Faraday cups or ion imaging detectors.

SIMS DETECTION LIMITS (at/cm3) IN DEPTH PROFILING MODE*

Silicon Carbide SIMS Measurements, SIMS Detection Limits
*Detection limits in semi-bulk or bulk mode may be significantly lower than those obtained in depth profiling mode.

QUANTIFICATION OF SiC

Concentration Calibration

Concentrations are calibrated based on ion implant standards into clean SiC.

Depth Calibration

The acquisition time of a depth profile is converted to depth using the measured analytical crater depth (using a stylus profilometer).

IMPROVEMENT OF SIMS DETECTION LIMITS IN SiC

Improvement of detection limits of N

Improved vacuum and a modified Cs+ source that provides high beam current density, has led to improved detection limits for N.

Improvement of detection limits for B, Al, and other metal elements

The instrument used is limited to the measurement of Si, C, and SiC material to reduce potential contamination from other materials. A larger Field Aperture and a non-standard Contrast Diaphragm are used to increase the detection area and collection angle, thus increasing our sensitivity for these elements.

Detection limits under profiling condition in SiC

N: 2-5E15 atoms/cm3

B: 2E13 atoms/cm3

Al: 2E13 atoms/cm3

Silicon Carbide SIMS Measurements, Detection limits under profiling condition in SiC

TYPICAL SiC ANALYSES

  • Depth profiling of dopants and impurities, including in small devices
  • Semi-bulk mode analysis of metallic impurities
  • SurfaceSIMS for surface contamination measurement on SiC surfaces
  • SIMS analysis with sample polishing to access deeper or buried layers (frontside or backside)
  • Extremely low concentration nitrogen analysis
  • SiO2/SiC interface analysis
Silicon Carbide SIMS Measurements, Semi-bulk mode analysis of metal impurities
Silicon Carbide SIMS Measurements, SIMS analysis of back-polished Sample Ni on SIC
Silicon Carbide SIMS Measurements, Raster Change Technique for Extremely Low Level N Analysis
Raster change during N profile. The N shown is quantified for the 50×50μm raster

RASTER CHANGE TECHNIQUE FOR LOW N CONCENTRATION MEASUREMENT

The “raster change” method provides an accurate way to determine and remove the contribution of background nitrogen to the measured signal, because both nitrogen and matrix ion intensities can be analyzed at the same location of the sample by changing the primary ion beam raster size during a profile.

In this technique, the sample is initially sputtered by the primary beam using a large raster. After the profile reaches a constant level, the primary raster size is reduced, while the collection area for secondary ions stays the same. This increases the current density of primary ions within the collection area.

A disadvantage of this technique is that it can be used only on uniformly doped samples or in a thick enough layer that concentration is uniform.

SiC 4-INCH WHOLE WAFER ANALYSIS

SIMS profile of Al and N from a 2” SiC wafer. The Al profile was acquired using oxygen beam sputtering, and N profile was acquired using Cs beam sputtering. The whole wafer capability provides doping concentration and thickness of each epi layer without breaking the wafer. A N detection limit of ~2e16 atoms/cc can be achieved after ~2 hours of pumping.

Silicon Carbide SIMS Measurements, Modified Cameca 4f Sample Intro System
Modified Cameca 4f with 4” Sample Intro System
Silicon Carbide SIMS Measurements, SIMS Analysis of Individual SiC Particles for Accurate Bulk Concentration Measurement

SIMS ANALYSIS OF INDIVIDUAL SiC PARTICLES FOR ACCURATE BULK CONCENTRATION MEASUREMENT

Using a special sample preparation technique and a new SIMS analytical protocol, individual SiC particles with a size ranging from 100 μm to 500 μm in a SiC powder sample can be analyzed. This innovative approach eliminates contributions from surface contamination to bulk concentration.

Silicon Carbide SIMS Measurements

N profiles for two different SiC particles from the same batch of powder samples. The SIMS results for these two particles show good batch bulk concentration consistency.

N profiles for two different SiC particles from the same batch of powder samples. The SIMS results for these two particles show good batch bulk concentration consistency.

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