scholarly journals Synchrotron radiation vacuum chamber installation and beam size

1985 ◽  
Author(s):  
M. Shleifer ◽  
G. Williams
1987 ◽  
Vol 31 ◽  
pp. 495-502 ◽  
Author(s):  
Y. Gohshj ◽  
S. Aoki ◽  
A. Iida ◽  
S. Hayakawa ◽  
H. Yamaji ◽  
...  

SummaryA scantling X-ray fluorescence(XRF) microprobe using WoIter type 1 optics was developed, and micro and trace element analysis was carried out using synchrotron radiation up to 10 keV as an excitation source. The design parameters of the optical system and the performance of the system, such as the beam size and the intensity, are described. The MDL obtained for Mn was 6 ppm in relative concentration and about 0.1 pg in absolute amount. The estimated spatial resolution was better than 10 um.


Author(s):  
A. N. Artemiev ◽  
V. N. Korchuganov ◽  
A. G. Valentinov ◽  
V. V. Kvardakov ◽  
B. F. Kirillov ◽  
...  

2015 ◽  
Vol 22 (2) ◽  
pp. 288-316 ◽  
Author(s):  
Gianluca Geloni ◽  
Vitali Kocharyan ◽  
Evgeni Saldin

The maximum of the Wigner distribution (WD) of synchrotron radiation (SR) fields is considered as a possible definition of SR source brightness. Such a figure of merit was originally introduced in the SR community by Kim [(1986),Nucl. Instrum. Methods Phys. Res. A,246, 71–76]. The brightness defined in this way is always positive and, in the geometrical optics limit, can be interpreted as the maximum density of photon flux in phase space. For undulator and bending magnet radiation from a single electron, the WD function can be explicitly calculated. In the case of an electron beam with a finite emittance the brightness is given by the maximum of the convolution of a single electron WD function and the probability distribution of the electrons in phase space. In the particular case when both electron beam size and electron beam divergence dominate over the diffraction size and the diffraction angle, one can use a geometrical optics approach. However, there are intermediate regimes when only the electron beam size or the electron beam divergence dominate. In these asymptotic cases the geometrical optics approach is still applicable, and the brightness definition used here yields back once more to the maximum photon flux density in phase space. In these intermediate regimes a significant numerical disagreement is found between exact calculations and the approximation for undulator brightness currently used in the literature. The WD formalism is extended to a satisfactory theory for the brightness of a bending magnet. It is found that in the intermediate regimes the usually accepted approximation for bending magnet brightness turns out to be inconsistent even parametrically.


2011 ◽  
Vol 58 (1) ◽  
pp. 35-38 ◽  
Author(s):  
Jin-yeong Ryu ◽  
Eun-San Kim ◽  
Ji-Gwang Hwang ◽  
Hyang-Kyu Park ◽  
Hyun-Duk Kim ◽  
...  

Vacuum ◽  
1993 ◽  
Vol 44 (1) ◽  
pp. 7-10 ◽  
Author(s):  
K Kanazawa ◽  
M Yanokura ◽  
M Aratani ◽  
H Akiyama

2016 ◽  
Vol 40 (9) ◽  
pp. 097002 ◽  
Author(s):  
Kai Tang ◽  
Bao-Gen Sun ◽  
Yong-Liang Yang ◽  
Ping Lu ◽  
Lei-Lei Tang ◽  
...  

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