Secondary Ion Mass Spectrometry (SIMS)
LaboratoryNational Renewable Energy Laboratory (NREL)
Capability ExpertSteven Harvey
Node Readiness Category2: High-Temperature Electrolysis (HTE)
2: Low-Temperature Electrolysis (LTE)
2: Photoelectrochemical (PEC)
2: Solar Thermochemical (STCH)
Secondary ion mass spectrometry (SIMS) is a powerful analytical technique useful for measurements of organic surfaces, dopants and impurities in solids, and diffusion across interfaces.
Time of Flight SIMS (TOF-SIMS) provides surface spectroscopy of both inorganic and organic materials, and is capable of detection limits in the sub-ppm range. High-lateral-resolution (>80 nm) chemical imaging is also possible; recent TOF-SIMS work at NREL has focused on understanding grain-boundary segregation effects in materials such as thin-film polycrystalline CdTe via high-resolution 3-D tomography.
Dynamic SIMS excels at measuring dopant concentrations at extremely low levels in solid materials. Dopants are routinely measured in the parts-per-billion (ppb) and sub-ppb levels.
The largest sample which can fit into the NREL system is 3x5 inches in size; the smallest samples we can measure are a few square millimeters. While TOF-SIMS can investigate organics and organic coatings, dynamic SIMS is only capable of investigating inorganic materials. Materials must be stable in vacuum at room temperature.
The NREL TOF-SIMS is a near state-of-the art ION-TOF TOF-SIMS V. The primary operator at NREL has extensive and varied experience utilizing TOF-SIMS to investigate a variety of materials including oxides, organics, and semiconductors. The NREL dynamic SIMS is a CAMECA 7F spectrometer capable of routinely measuring dopants in the ppb concentration range.
These capabilities are available for use within the HydroGEN consortium effort with no significant restrictions. NRELs staff are available to perform measurements, and can also host visitors to NREL.
TOF-SIMS is an extremely versatile technique capable of non-destructive investigation of surface coatings, as well as high-resolution imaging and tomography. Dynamic SIMS can measure dopants with sensitivity unmatched by most other methods.
Figure 1. A. 50x50µm image of the Ni signal in a composite NiO/Ba(1-x)YxCe(1-Y)ZryO3. B. 50x50µm image of the Ba signal in a composite NiO/Ba(1-x)YxCe(1-Y)ZryO3. C. 3-D rendering of both the Ba (blue) and Ni (yellow)signal in a composite NiO/Ba(1-x)YxCe(1-Y)ZryO3.
Figure 2. 3-D rendering of phosphorous dopant distribution in polycrystalline CdTe. High signal is red, at the grain-boundaries, and low signal is black, in the grain interiors.
Figure 3. Top: Structural rendering of the hybrid organic-inorganic perovskite photovoltaic material. Bottom: A series of regions from the TOF-SIMS mass spectra showing peaks related to the hybrid organic-inorganic perovskite material.
Figure 4. A. Standard depth profile of a completed perovskite photovoltaic device. B. 3-D tomography rendering of a completed perovskite PV device.
Colegrove, E., S. P. Harvey, et al. (2016). "Phosphorus Diffusion Mechanisms and Deep Incorporation in Polycrystalline and Single-Crystalline CdTe." Physical Review Applied 5(5): 054014; Harvey, S. P., G. Teeter, et al. (2015). Progress in Photovoltaics 23(7): 838-846.