Secondary ion mass spectrometry for quantitative surface and in-depth analysis of materials

被引:14
作者
Chakraborty, P [1 ]
机构
[1] Saha Inst Nucl Phys, Calcutta 700064, W Bengal, India
来源
PRAMANA-JOURNAL OF PHYSICS | 1998年 / 50卷 / 06期
关键词
sputtering; secondary ion emission; compositional profile; thin films;
D O I
10.1007/BF02846051
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
Secondary ion mass spectrometry (SIMS) is a technique based on the sputtering of material surfaces under primary ion bombardment. A fraction of the sputtered ions which largely originate from the top one or two atomic layers of the solid is extracted and passed into a mass spectrometer where they are separated according to their mass-to-charge ratios and subsequently detected. Because the sputter-yields of the individual species, coupled with their ionization probabilities, can be quite high and the mass spectrometers can be built with high efficiencies, the SIMS technique can provide an extremely high degree of surface sensitivity. Using a particular mode like static SIMS where a primary ion current is as low as 10(-11) amp, the erosion rate of the surface can be kept as low as 1 Angstrom per hour and one can obtain the chemical information of the uppermost atomic layer of the target. The other mode Like dynamic SIMS where the primary ion current is much higher can be employed for depth profiling of any chemical species within the target matrix, providing a very sensitive tool (similar to 1 ppm down to ppb) for quantitative characterization of surfaces, thin films, superlattices, etc. The presence of molecular ions amongst the sputtered species makes this method particularly valuable in the study of molecular surfaces and molecular adsorbates. The range of peak-intensities in a typical SIMS spectrum spans about seven to eight orders of magnitude, showing its enormously high dynamic range; an advantage in addition to high sensitivity and high depth-resolution. Furthermore, the high sensitivity of SIMS to a very small amount of material implies that this technique is adaptable to microscopy, offering its imaging possibilities. By using this possibility in static SIMS or dynamic SIMS mode of analysis, one can obtain a two-dimensional (2D) surface mapping or;a three-dimensional. (3D) reconstruction of the elemental distribution, respectively within the target matrix. Secondary ion yields for elements can differ from matrix to matrix. These sensitivity variations pose serious limitations in quantifying SIMS data. Various methods like calibration curve approach, implantation standard method, use of relative sensitivity factor, etc. are presently employed for making quantitative SIMS analysis. The formation of Secondary ions by ion bombardment of solids, is relatively a complex process and theoretical research in this direction continues in understanding this process in general. The present paper briefly reviews the perspective of this subject in the field of materials analysis.
引用
收藏
页码:617 / 640
页数:24
相关论文
共 40 条
[1]   CHROMIUM DIFFUSION IN LITHIUM-NIOBATE FOR ACTIVE OPTICAL WAVE-GUIDES [J].
ALMEIDA, JM ;
BOYLE, G ;
LEITE, AP ;
DELARUE, RM ;
IRONSIDE, CN ;
CACCAVALE, F ;
CHAKRABORTY, P ;
MANSOUR, I .
JOURNAL OF APPLIED PHYSICS, 1995, 78 (04) :2193-2197
[2]   NONLINEAR EFFECTS IN HEAVY-ION SPUTTERING [J].
ANDERSEN, HH ;
BAY, HL .
JOURNAL OF APPLIED PHYSICS, 1974, 45 (02) :953-954
[3]  
ANDERSON CA, 1973, ANAL CHEM, V45, P142
[4]   SURFACE-ANALYSIS BY SECONDARY-ION MASS-SPECTROMETRY (SIMS) [J].
BENNINGHOVEN, A .
SURFACE SCIENCE, 1994, 299 (1-3) :246-260
[5]   OBSERVATION ON SURFACE-REACTIONS WITH STATIC METHOD OF SECONDARY ION MASS-SPECTROMETRY .1. METHOD [J].
BENNINGHOVEN, A .
SURFACE SCIENCE, 1971, 28 (02) :541-+
[6]  
BENNINGHOVEN A, 1987, SECONDARY ION MASS S, P765
[7]  
BENNINGHOVEN A, 1983, SPRINGER SERIES CHEM, V25, P640
[8]  
BENNINGHOVEN A, 1987, SECONDARY ION MASS S, P296
[9]   COMPARATIVE EFFECTS OF OXYGEN ON ION EMISSION AND SURFACE POTENTIAL OF METALS [J].
BLAISE, G ;
SLODZIAN, G .
SURFACE SCIENCE, 1973, 40 (03) :708-714
[10]  
BLATTNER RJ, 1980, SCANNING ELECT MICRO