For two-dimensional x-ray imaging of thin films, the technique of scanning
transmission x-ray microscopy (STXM) has achieved images with feature sizes
as small as 40 nm in recent years. However, calibration of three-dimension
al tomographic images that are produced with STXM data at this scale has no
t yet been described in the scientific literature, and the calibration proc
edure has novel problems that have not been encountered by x-ray tomography
carried out at a larger scale. In x-ray microtomography, for example, one
always has the option of using optical imaging on a section of the object t
o verify the x-ray projection measurements. with STXM, on the other hand, t
he sample Features are too small to be resolved by light at optical wavelen
gths. This fact implies that one must rely on procedures with higher resolu
tion, such as atomic force microscopy (AFM), for the calibration. Such proc
edures, however, generally depend on a highly destructive sectioning of the
sample, and are difficult to interpret because they give surface informati
on rather than depth information. In this article, a procedure for calibrat
ion is described that overcomes these limitations and achieves a calibratio
n of an STXM tomography image with an AFM image and a scanning electron mic
roscopy image of the same object.
A Ge star-shaped pattern was imaged at a synchrotron with a scanning transm
ission x-ray microscope. Nineteen high-resolution projection images of 200x
200 pixels were tomographically reconstructed into a three-dimensional imag
e. Features in two-dimensional images as small as 40 nm and features as sma
ll as 80 nm in the three-dimensional reconstruction were resolved. Transver
se length scales based on atomic force microscopy, scanning electron micros
copy, x-ray transmission and tomographic reconstruction agreed to within 10
nm. Toward the center of the sample, the pattern thickness calculated from
projection images was (51 +/- 15) nm vs (80 +/- 52) nm for tomographic rec
onstruction, where the uncertainties are evaluated at the level of two stan
dard deviations.