Hello,
the difference in these configurations lies in the Debye-Waller factors you have specified. The file you generated from the CIF file has no Debye-Waller factors at all. This tells you that HAADF-STEM imaging is very sensitive to the Debye-Waller factors of the different Atom species.
With best regards,
Christoph Koch.
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Hello ?,
Let me try to answer your different questions one by one:
1. (Q1) If you generate a .cfg file from a .cif file and want to simulate HAADF-STEM images you should try to search the literature (or the .cif file you have used as input – if the structure stems from X-ray diffraction, then the DW-factors are often fitted and provided as well) for suitable Debye-Waller factors. Otherwise both qstem and qmb will insert default Debye-Waller factors.
Having written this, Ruben Bjorge from Trondheim, Norway and Florian Krause from Bremen, Germany have recently discovered that qstem is currently erroneously dividing the Debye-Waller factor by 3 when doing TDS calculations, so with the current version of qstem, one should specify a temperature that is 3 times higher than the actual specimen temperature (i.e. typically 900 K), IF YOU WANT TO DO A TDS CALCULATION. This is a serious bug, and I will fix it as soon as possible. Setting the temperature to 900 K will rescale all the mean squared atomic displacements by the necessary factor of 3.
2. (Q5) Both, the TDS multislice calculation, as well as the calculation without TDS rely on the very same Debye-Waller factor B. If TDS is turned off, then the atomic potentials will be smoothed by exp(-B*s^2). If TDS is turned on, then this smoothing will not be done, but instead the atoms will be displaced randomly with a displacement amplitude u=sqrt[B/(8pi^2)]. So in either case the value of B is highly relevant. In the kinematic approximation, both treatments should result in exactly the same change in the diffracted intensities – only the diffuse scattering between the Bragg beams will be different (no diffuse scattering, if TDS = off). Since Thermal diffuse scattering occurs predominantly at high scattering angles, this is more important in HAADF-STEM imaging, than in HRTEM or BF-STEM imaging.
3. (Q2,Q3) I do not remember where I have taken the Debye-Waller factors for SrTiO3 from. It was probably some article in the literature. L.M. Peng has also once computed a number of DW factors (see attached paper). But please keep in mind that in each crystal the same atom type may be bonded more or less rigidly, and thus the vibrational amplitudes may also differ.
4. (Q4) The difference between the simulated HAADF-STEM image and the experimental image can be due to several factors (different thickness, tilt, temperature, effective source size, etc.) but it might also be due to the factor 3 that I have mentioned above.
With best regards,
Christoph.