Design of a compact electron accelerator-driven pulsed neutron facility at AIST

Author(s):  
Koichi Kino ◽  
Takeshi Fujiwara ◽  
Michihiro Furusaka ◽  
Noriyosu Hayashizaki ◽  
Ryunosuke Kuroda ◽  
...  
Author(s):  
Brian E. O'Rourke ◽  
Takeshi Fujiwara ◽  
Kazuro Furukawa ◽  
Michihiro Furusaka ◽  
Noriyosu Hayashizaki ◽  
...  

2009 ◽  
Vol 56 (3) ◽  
pp. 1292-1296 ◽  
Author(s):  
Andrea Favalli ◽  
H.-C. Mehner ◽  
Jean-Michel Crochemore ◽  
Bent Pedersen

2017 ◽  
Vol 146 ◽  
pp. 03031 ◽  
Author(s):  
Tadafumi Sano ◽  
Jun-ichi Hori ◽  
Yoshiyuki Takahashi ◽  
Hiroshi Yashima ◽  
Jaehong Lee ◽  
...  

2011 ◽  
Author(s):  
Guinyun Kim ◽  
Manwoo Lee ◽  
Kyung Sook Kim ◽  
Sungchul Yang ◽  
Eunae Kim ◽  
...  

Neutron News ◽  
2013 ◽  
Vol 24 (4) ◽  
pp. 28-32 ◽  
Author(s):  
A.S. Tremsin ◽  
S.C. Vogel ◽  
M. Mocko ◽  
M.A.M. Bourke ◽  
V. Yuan ◽  
...  

Author(s):  
A. Strojnik ◽  
J.W. Scholl ◽  
V. Bevc

The electron accelerator, as inserted between the electron source (injector) and the imaging column of the HVEM, is usually a strong lens and should be optimized in order to ensure high brightness over a wide range of accelerating voltages and illuminating conditions. This is especially true in the case of the STEM where the brightness directly determines the highest resolution attainable. In the past, the optical behavior of accelerators was usually determined for a particular configuration. During the development of the accelerator for the Arizona 1 MEV STEM, systematic investigation was made of the major optical properties for a variety of electrode configurations, number of stages N, accelerating voltages, 1 and 10 MEV, and a range of injection voltages ϕ0 = 1, 3, 10, 30, 100, 300 kV).


Author(s):  
T. Egami ◽  
H. D. Rosenfeld ◽  
S. Teslic

Relaxor ferroelectrics, such as Pb(Mg1/3Nb2/3)O3 (PMN) or (Pb·88La ·12)(Zr·65Ti·35)O3 (PLZT), show diffuse ferroelectric transition which depends upon frequency of the a.c. field. In spite of their wide use in various applications details of their atomic structure and the mechanism of relaxor ferroelectric transition are not sufficiently understood. While their crystallographic structure is cubic perovskite, ABO3, their thermal factors (apparent amplitude of thermal vibration) is quite large, suggesting local displacive disorder due to heterovalent ion mixing. Electron microscopy suggests nano-scale structural as well as chemical inhomogeneity.We have studied the atomic structure of these solids by pulsed neutron scattering using the atomic pair-distribution analysis. The measurements were made at the Intense Pulsed Neutron Source (IPNS) of Argonne National Laboratory. Pulsed neutrons are produced by a pulsed proton beam accelerated to 750 MeV hitting a uranium target at a rate of 30 Hz. Even after moderation by a liquid methane moderator high flux of epithermal neutrons with energies ranging up to few eV’s remain.


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