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@@ -110,13 +110,13 @@ | |
offers the edge positions plus 50 eV. You are free to specify any energy | ||
within the range of the selected tabulation. | ||
A typical application is the calculation of the mass for a powder sample. The | ||
optimal *optical* sample thickness μd depends on the absorption levels selected | ||
for the ionization chambers (see below). Typically, μd is between 2 and 3 (e.g. | ||
for a 17.4% absorption level for the 1st chamber and a 50% level for the 2nd | ||
chamber, the optimal thickness is 2.42). However, if you get the absorption | ||
step more that 1.5 (reported by the drop-down list "absorptance step = "), it | ||
is recommended to reduce the sample mass to avoid the potential thickness | ||
The most typical application is the calculation of the mass of a powder sample. | ||
The optimal *optical* sample thickness μd depends on the absorption levels | ||
selected for the ionization chambers (see below). Typically, μd is between 2 | ||
and 3 (e.g. for a 17.4% absorption level for the 1st chamber and a 50% level | ||
for the 2nd chamber, the optimal thickness is 2.42). However, if you get the | ||
absorption step > 1.5 (reported by the drop-down list "absorptance step = "), | ||
it is recommended to reduce the sample mass to avoid the potential thickness | ||
effect due to possible inhomogeneity in the wafer. If your sample is diluted | ||
and you get a very low absorption step, do not try to make the wafer thicker | ||
hoping that you will get better spectra -- you will not: the optimal thickness | ||
|
@@ -195,12 +195,12 @@ | |
""" | ||
__module__ = "XAFSmass" | ||
__versioninfo__ = (1, 3, 9) | ||
__versioninfo__ = (1, 4, 2) | ||
__version__ = '.'.join(map(str, __versioninfo__)) | ||
__author__ = \ | ||
"Konstantin Klementiev (MAX IV Laboratory), " +\ | ||
"Roman Chernikov (Canadian Light Source)" | ||
__email__ = \ | ||
"[email protected], [email protected]" | ||
__date__ = "09 Jul 2019" | ||
__date__ = "20 Feb 2023" | ||
__license__ = "MIT license" |
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