Determination of carbon in sediments by electron beam X-ray excitation

1973 ◽  
Vol 2 (4) ◽  
pp. 165-168 ◽  
Author(s):  
A. B. Poole
Keyword(s):  
2019 ◽  
Vol 34 (7) ◽  
pp. 1497-1502 ◽  
Author(s):  
Malte Wansleben ◽  
Claudia Zech ◽  
Cornelia Streeck ◽  
Jan Weser ◽  
Christoph Genzel ◽  
...  

Liquid-metal jet X-ray sources promise to deliver high photon fluxes, which are unprecedented for laboratory based X-ray sources, because the regenerating liquid-metal anode is less sensitive to damage caused by an increased electron beam power density.


Author(s):  
A. N. Artemiev ◽  
A. A. Snigirev ◽  
V. N. Korchuganov ◽  
A. G. Valentinov ◽  
V. V. Kvardakov ◽  
...  

2020 ◽  
Vol 77 (5) ◽  
pp. 443-446
Author(s):  
Kyoung Won Jang ◽  
Manwoo Lee ◽  
Heuijin Lim ◽  
Sang Koo Kang ◽  
Dong Hyeok Jeong
Keyword(s):  
X Ray ◽  

2018 ◽  
Vol 25 (2) ◽  
pp. 378-384
Author(s):  
Matthew Hand ◽  
Hongchang Wang ◽  
Francesco Maccherozzi ◽  
Marco Apollonio ◽  
Jingtao Zhu ◽  
...  

Insertion devices are utilized at synchrotron radiation facilities around the world for their capability to provide a high-brilliance X-ray beam. APPLE-II type undulators are especially important for their capacity to switch between a variety of photon beam polarization states. A high-precision soft X-ray polarimeter has been used to investigate the polarization calibration of an APPLE-II undulator (period length λu= 64 mm) installed on beamline I06 at Diamond Light Source. Systematic measurement of the beam polarization state at a range of linear arbitrary angles has been compared with the expected result for a given set of undulator gap and row phase parameters calculated from theory. Determination of the corresponding Stokes–Poincaré parameters from the measured data reveals a discrepancy between the two. The limited number of energy/polarization combinations included in the undulator calibration tables necessitates the use of interpolated values for the missing points which is expected to contribute to the discrepancy. However, by modifying the orbit of the electron beam through the undulator by at least 160 µm it has been found that for certain linear polarizations the discrepancies can be corrected. Overall, it is suggested that complete correction of the Stokes–Poincaré parameters for all linear angles would require alteration of both these aspects.


2015 ◽  
Vol 1084 ◽  
pp. 111-114
Author(s):  
Yury Cherepennikov ◽  
Alexey Gogolev ◽  
Alexander Wagner ◽  
Alexander Yuzhakov

The paper discusses the issue of creating a monochromatic X-ray source based on a small-size electron accelerator to be used for the purposes of medical diagnostics. We carried out the simulation of X-ray spectra generated by an electron beam with the energy of 4-10 MeV in the targets of different materials and thicknesses and determined the optimal parameters of the target. The radiation intensity was estimated and sources based on different accelerators were compared, with due consideration of the simulation results.


2014 ◽  
Vol 85 (7) ◽  
pp. 073302 ◽  
Author(s):  
Thomas M. Baumann ◽  
Alain Lapierre ◽  
Kritsada Kittimanapun ◽  
Stefan Schwarz ◽  
Daniela Leitner ◽  
...  

Author(s):  
H.J. Dudek

The chemical inhomogenities in modern materials such as fibers, phases and inclusions, often have diameters in the region of one micrometer. Using electron microbeam analysis for the determination of the element concentrations one has to know the smallest possible diameter of such regions for a given accuracy of the quantitative analysis.In th is paper the correction procedure for the quantitative electron microbeam analysis is extended to a spacial problem to determine the smallest possible measurements of a cylindrical particle P of high D (depth resolution) and diameter L (lateral resolution) embeded in a matrix M and which has to be analysed quantitative with the accuracy q. The mathematical accounts lead to the following form of the characteristic x-ray intens ity of the element i of a particle P embeded in the matrix M in relation to the intensity of a standard S


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