Computer-assisted method for determining an element fraction of a determination element having a small atomic number, in particular a Li fraction, and corresponding device for processing data
12553840 · 2026-02-17
Assignee
Inventors
Cpc classification
G01N23/2206
PHYSICS
G01N2223/072
PHYSICS
G01N23/2208
PHYSICS
G01N23/2252
PHYSICS
International classification
G01N23/2206
PHYSICS
Abstract
A computer-assisted method for determining an element fraction of a determination element, in particular with a small atomic number, especially lithium, of an examination region of a sample bombarded with primary electrons, wherein a backscattered electron signal, preferably a backscattered electron image, captured using a backscattered electron detector and a spectroscopy element composition of the examination region determined using an X-ray spectroscopy detector, such as an EDX detector, are obtained. A practicable quantitative determination can be achieved if a measured gray value SM determined from the backscattered electron signal is combined with element fractions of the spectroscopy element composition in order to determine a fraction of the determination element. A device for processing data and to a computer product for carrying out the method is also disclosed.
Claims
1. A computer-assisted method for determining an element fraction of a determination element of an examination region of a sample bombarded with primary electrons, comprising the steps of: capturing a backscattered electron signal using a backscattered electron detector, obtaining using an X-ray spectroscopy detector a spectroscopy element composition of the examination region, combining a measured gray value SM determined from the backscattered electron signal with element fractions of the spectroscopy element composition in order to determine a fraction of the determination element, calculating a reference gray value SV using the element fractions of the spectroscopy element composition, and determining the fraction of the determination element using a comparison of the measured gray value SM and reference gray value SV.
2. The method according to claim 1, wherein combining the measured gray value SM and the element fractions of the spectroscopy element composition occurs using backscatter coefficients of the element fractions.
3. The method according to claim 1, wherein one or more calibration samples are measured using the backscattered electron detector, in order to assign specific gray values to specific elements or element compositions.
4. The method according to claim 1, wherein a calibration sample formed with or from the determination element is measured using the backscattered electron detector, in order to assign a gray value to the determination element.
5. The method according to claim 1, wherein the examination region of the sample is bombarded with a primary electron beam and electrons backscattered from the examination region are detected using the backscattered electron detector in order to capture the backscattered electron signal, and X-rays emitted from the examination region are detected using the X-ray spectroscopy detector in order to determine the spectroscopy element composition.
6. The method according to claim 1, wherein the determination element has a small atomic number.
7. The method according to claim 6, wherein the determination element is lithium.
8. The method according to claim 1, wherein the captured backscattered electron signal is a backscattered electron image.
9. The method according to claim 1, wherein the X-ray spectroscopy detector is an EDX detector.
10. The method according to claim 1, wherein the comparison is based on a difference between the measured gray value SM and reference gray value SV.
11. The method according to claim 5, wherein the X-ray spectroscopy detector is an EDX detector.
12. An electron microscope, comprising: a device having at least one processor for processing data; a backscattered electron detector; an X-ray spectroscopy detector; and wherein the electron microscope is configured to carry out the method according to claim 1.
13. A non-transitory computer-readable recording medium for use in a computer, the recording medium having a computer program recorded thereon for causing the computer in combination with a backscattered electron detector, and an X-ray spectroscopy detector to carry out the method according to claim 1.
Description
(1) Additional features, advantages, and effects follow from the exemplary embodiments described below. In the drawings which are thereby referenced:
(2)
(3)
(4)
(5)
(6) A gray value of a backscattered electron image, referred to as the measured gray value S.sub.M, of a surface of a sample is a function of a mean atomic element of the surface of the sample. Elements having a low atomic number, such as lithium for example, decrease the gray value. By calculating a reference gray value S.sub.V based on an element composition of the surface determined by means of X-ray spectroscopy, in which composition lithium is not represented due to inadequate sensitivity of X-ray spectroscopy to lithium, the Li content of the surface of the sample can be determined by combining the measured gray value S.sub.M of the backscattered electron image with the reference gray value S.sub.V. Typically, the measured gray value S.sub.M and reference gray value S.sub.V are thereby respectively stated as an averaged value. The backscattered electron image, customarily referred to in the art as a BSE image, is typically captured using a backscattered electron detector, or BSE detector. The element composition of the surface is normally determined by means of energy-dispersive X-ray spectroscopy, referred to as EDX.
(7)
(8) As a result, x.sub.Li can be calculated, and a fraction of Li in the examined sample surface can thus be determined.
(9) A determination of a fraction of lithium as a determination element is described below by way of example with the aid of two MgLi-based alloys LAX410 and LSX2021. For this purpose, one backscattered electron image each of an examination region, customarily referred to in the art as ROI or region of interest, of alloy samples of the respective alloy is determined, and one spectroscopy element composition of the respective examination region is determined by means of energy-dispersive X-ray spectroscopy, or EDX. The nominal compositions of LAX410 and LSX2021 are shown in wt % in Table 1. The alloy samples were produced using an electric induction furnace under argon protective gas atmosphere. To distinguish the alloy samples, a field-emission scanning electron microscope was used, wherein a silicon drift detector was used for EDX and a four-quadrant semiconductor detector was used to capture the backscattered electron image.
(10) TABLE-US-00001 TABLE 1 Nominal composition of LAX410 and LSX2021 in wt %. Mg Li Al Si Ca LAX410 Remainder 4.0 0.8 0.3 LSX2021 Remainder 20.0 2.0 1.0
(11)
(12) In order to calculate a respective mean reference gray value
(13) Based on the formula
(14)
the fraction x of Li in the respective examination region was thus calculated, wherein
(15) TABLE-US-00002 TABLE 2 For LAX410: Fractions of Mg, Al, and Ca in wt % determined by means of X-ray spectroscopy; mean measured gray value
(16) TABLE-US-00003 TABLE 3 For LSX2021: Fractions of Mg, Si, and Ca in wt % determined by means of X-ray spectroscopy; mean measured gray value
(17) As can be seen in Table 2 and Table 3, an Li fraction of 2.8 wt % and 17.5 wt %, respectively, was determined for the ROI 1 of the alloy samples. For both the LAX410 alloy sample and the LSX2021 alloy sample, the ROI 1 relates to a matrix region of the respective alloy morphology. The Li fractions determined for the ROI 1 are somewhat lower than, but very close to, the nominal Li fractions according to Table 1. As can be seen in Table 2 and Table 3, the ROI 2 of the LAX410 alloy sample and LSX2O2I alloy sample have slightly higher calculated mean reference gray values
(18) It is thus shown that, with the method according to the invention, a quantitative determination of elements having a smaller atomic number, in particular lithium, is enabled with high accuracy in that backscattered electron signals, in particular backscattered electron images, and X-ray spectroscopy measurement results are synergistically combined. A bonding state of the determination element thereby advantageously plays a secondary role, since a backscattering or a backscatter coefficient of backscattered electrons is typically dominated by the nucleus of the respective element.