Comment on “Grazing incidence X-ray fluorescence of periodic structures – a comparison between X-ray standing waves and geometrical optics calculations” by F. Reinhardt, S. H. Nowak, B. Beckhoff, J-C. Dousse and M. Schoengen, JAAS, 2014, 29, 1778

2015 ◽  
Vol 30 (12) ◽  
pp. 2548-2550
Author(s):  
W. Jark ◽  
D. Eichert

The data interpretation in the recently published paper with the above title is criticized and it is shown that an alternative more physical model based on diffraction in periodic structures can explain the data better and more consistently.

2015 ◽  
Vol 30 (12) ◽  
pp. 2551-2553
Author(s):  
Stanisław H. Nowak ◽  
Burkhard Beckhoff ◽  
Falk Reinhardt ◽  
Jean-Claude Dousse

We respond to the comment by W. Jark and D. Eichert on our earlier article concerning geometrical optics based data interpretation of grazing incidence X-ray fluorescence experiments.


2014 ◽  
Vol 29 (10) ◽  
pp. 1778-1784 ◽  
Author(s):  
Falk Reinhardt ◽  
Stanisław H. Nowak ◽  
Burkhard Beckhoff ◽  
Jean-Claude Dousse ◽  
Max Schoengen

Geometrical optics calculations are able to reproduce experimentally found modulations in GIXRF which are beyond the potential of the XSW model.


10.14311/1787 ◽  
2013 ◽  
Vol 53 (2) ◽  
Author(s):  
Jakub Hübner ◽  
Pavel Vrba

Feasible soft-X-ray amplification in the CVI and NVII Balmer transition is investigated in a capillary discharge. The best conditions and parameters for the experimental set-up are found for an ablative capillary. The most optimistic results have shown that the gain would be greater than one, which is the condition for successful ASE (Amplified spontaneous emission) in capillary discharges. The capillary discharge evolution is modeled using the NPINCH program, employing a one-dimensional physical model based on MHD equations. The information about the capillary discharge evolution is processed in the FLY, FLYPAPER, FLYSPEC programs, enabling the population to be modeled on specific levels during capillary discharge.


2021 ◽  
Vol 54 (5) ◽  
pp. 1530-1534
Author(s):  
Sergey Stepanov

X-ray Server (https://x-server.gmca.aps.anl.gov) is a collection of programs for online modelling of X-ray diffraction and scattering. The dynamical diffraction program is the second most popular Server program, contributing 34% of total Server usage. It models dynamical X-ray diffraction from strained crystals and multilayers for any Bragg-case geometry including grazing incidence and exit. This paper reports on a revision of equations used by the program, which yields ten times faster calculations in most use cases, on implementing calculations of X-ray standing waves and on adding new options for modelling diffraction from monolayers.


1999 ◽  
Vol 286 (1-2) ◽  
pp. 313-321 ◽  
Author(s):  
Jerzy B. Pełka ◽  
Alessia Cedola ◽  
Stefano Lagomarsino ◽  
Silvia di Fonzo ◽  
Werner Jark ◽  
...  

2013 ◽  
Vol 28 (5) ◽  
pp. 689 ◽  
Author(s):  
Stanisław H. Nowak ◽  
Falk Reinhardt ◽  
Burkhard Beckhoff ◽  
Jean-Claude Dousse ◽  
Jakub Szlachetko

2011 ◽  
Vol 1349 ◽  
Author(s):  
Michael J. Bogan

ABSTRACTThe world’s first hard x-ray FEL (XFEL), the Linac Coherent Light Source (LCLS) is operational, steadily producing mJ energy, <75 fs pulses of 1.5 Å x-rays (1012 photons per pulse), a billion times more intensity than any other X-ray source. XFELs have stimulated the shift from the use of x-rays to probe periodic structures, such as crystals, to imaging non-periodic structures using ultrabright x-ray pulses shorter than the time for required for the onset of damage. The international community has embraced the potential as additional XFELs are currently being constructed in Japan, Italy and Germany with many more already planned or in construction elsewhere. Here the recent efforts to extend x-ray microscopy to the nanoscale for airborne particles using diffract-and-destroy methods are reviewed. Projecting current experimental results to future facilities suggests that gains of more than 104 in data acquisition rates are possible by 2020. This projection emphasizes the need for the development of fast x-ray detectors, infrastructure investments to handle the rapid data rate and storage requirements, as well as the appropriate training of scientists to handle data interpretation. Further improvements in particle delivery methods are also necessary, in particular to reduce sample consumption and to provide orthogonal data channels for each individual particle imaged. The projected growth of single particle CXDI data rates show great promise for the field. However, to achieve the resolution required to solve many scientific problems tractable with single-shot imaging, improvements in the absolute number of photons per pulse in a given area are still necessary.


2001 ◽  
Vol 696 ◽  
Author(s):  
Brad P. Tinkham ◽  
Duane M. Goodner ◽  
Donald A. Walko ◽  
Michael J. Bedzyk

AbstractX-ray diffraction and x-ray standing waves (XSW) have been used to investigate the quality of epitaxial ultra-thin Ge films grown on Si(001) with and without Te as a surfactant. The efficacy of Te as a surfactant in this application has been debated. We measured samples between 1 and 10 ML in thickness and our results clearly indicate that Ge films grown with Te are superior to those grown without Te. The coherent positions and coherent fract ons determined from XSW analysis agree well with those predicted by linear elasticity theory for Ge/Si(001). Furthermore, grazing incidence diffraction measurements (GIXD) suggests that 9 ML Ge grown on Si(001) with Te is strained in-plane while the same film grown without Te is relaxed.


2015 ◽  
Vol 22 (6) ◽  
pp. 1419-1425 ◽  
Author(s):  
Yuchun Tu ◽  
Yanyan Yuan ◽  
Karine Le Guen ◽  
Jean-Michel André ◽  
Jingtao Zhu ◽  
...  

The characterization of Mg–Co–Zr tri-layer stacks using X-ray fluorescence induced by X-ray standing waves, in both the grazing-incidence (GI) and the grazing-exit (GE) modes, is presented. The introduction of a slit in the direction of the detector improves the angular resolution by a factor of two and significantly improves the sensitivity of the technique for the chemical characterization of the buried interfaces. By observing the intensity variations of the MgKα and CoLα characteristic emissions as a function of the incident (GI mode) or detection (GE mode) angle, it is shown that the interfaces of the Si/[Mg/Co/Zr]×30multilayer are abrupt, whereas in the Si/[Mg/Zr/Co]×30multilayer a strong intermixing occurs at the Co-on-Zr interfaces. An explanation of this opposite behavior of the Co-on-Zr and Zr-on-Co interfaces is given by the calculation of the mixing enthalpies of the Co–Mg, Co–Zr and Mg–Zr systems, which shows that the Co–Zr system presents a negative value and the other two systems present positive values. Together with the difference of the surface free energies of Zr and Co, this leads to the Mg/Zr/Co system being considered as a Mg/CoxZrybi-layer stack, withx/yestimated around 3.5.


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