488
Y. Yoshida
Fig. 9.40 Mapping technique consisting of linear actuator and multi-capillary X-ray lens, precision
XYZ-θ stage, and micro channel plate for electron detection, and Si-PIN detector for transmitted
γ-ray detection
Fig. 9.41 Doppler velocity of the programmable actuator (SMAC) as functions of time: (a) the
constant acceleration mode (acceleration = ± 10 mm/s 2 ) and (b) the constant velocity mode
(velocity = + 10 and -5.42 mm/s), respectively. (c) The Mössbauer spectra of α-Fe foil measured
either by a conventional Mössbauer driver (upper), or by the moving-coil actuator with the constant
acceleration mode (middle) and with the constant velocity mode (lower). Reprinted by permission
from Springer Nature: Springer, Hyperfine Interactions, 3D-Mössbauer spectroscopic microscope
for mc-Si solar cell evaluation, Ino, Y., Soejima, H., Hayakawa, K. Yukihira, et al., © Springer
International Publishing Switzerland 2016
Y. Yoshida
Fig. 9.40 Mapping technique consisting of linear actuator and multi-capillary X-ray lens, precision
XYZ-θ stage, and micro channel plate for electron detection, and Si-PIN detector for transmitted
γ-ray detection
Fig. 9.41 Doppler velocity of the programmable actuator (SMAC) as functions of time: (a) the
constant acceleration mode (acceleration = ± 10 mm/s 2 ) and (b) the constant velocity mode
(velocity = + 10 and -5.42 mm/s), respectively. (c) The Mössbauer spectra of α-Fe foil measured
either by a conventional Mössbauer driver (upper), or by the moving-coil actuator with the constant
acceleration mode (middle) and with the constant velocity mode (lower). Reprinted by permission
from Springer Nature: Springer, Hyperfine Interactions, 3D-Mössbauer spectroscopic microscope
for mc-Si solar cell evaluation, Ino, Y., Soejima, H., Hayakawa, K. Yukihira, et al., © Springer
International Publishing Switzerland 2016