Monte Carlo Simulation of Ion Implantation Profiles Calibrated for Various Ions over Wide Energy Range

2009 ◽  
Vol 9 (1) ◽  
pp. 67-74 ◽  
Author(s):  
Kunihiro Suzuki ◽  
Yoko Tada ◽  
Yuji Kataoka ◽  
Tsutomu Nagayama
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Ion Implantation ◽  
Energy Range ◽  
Wide Energy Range ◽  
Wide Energy

High-current microwave ion source for wide-energy-range O+ ion implantation

2000 ◽  
Vol 71 (2) ◽  
pp. 952-954 ◽  
Author(s):  
K. Tokiguchi ◽  
T. Seki ◽  
J. Ito ◽  
T. Sato ◽  
K. Mera
Keyword(s):  
Ion Implantation ◽  
Energy Range ◽  
Ion Source ◽  
Wide Energy Range ◽  
High Current ◽  
Microwave Ion Source ◽  
Wide Energy

scholarly journals NaI(Tl+Li) scintillator as multirange energies neutron detector

2021 ◽  
Vol 16 (12) ◽  
pp. P12011
Author(s):  
D. Ponomarev ◽  
D. Filosofov ◽  
J. Khushvaktov ◽  
A. Lubashevskiy ◽  
I. Rozova ◽  
...  
Keyword(s):  
Experimental Data ◽  
Monte Carlo ◽  
Energy Range ◽  
Neutron Detector ◽  
Neutron Detection ◽  
Detection Sensitivity ◽  
Wide Energy Range ◽  
Γ Radiation ◽  
Wide Energy

Abstract Novel NaIL detector (5 × 6 inch) was investigated for its neutron detection in wide energy range. It has been found that the detector together with its known ability to detect the γ-radiation it also allows to distinguish neutron signals in three quasi-independent ways. It is sensitive to neutron fluxes on a level down to 10-3 cm-2 s-1. In this work intrinsic α-background and neutron detection sensitivity for the NaIL detector were obtained. Experimental data was compared with results of Geant4 Monte Carlo (MC).

Particle-In-Cell/Monte-Carlo Simulation of Plasma and Neutral Gas Flow for the Inner Coating of PET Bottles by Plasma-Based Ion Implantation. N2 Gas Plasma

2005 ◽  
Vol 2 (6) ◽  
pp. 480-484 ◽  
Author(s):  
Yoshiko Miyagawa ◽  
Masaaki Tanaka ◽  
Hiroshi Nakadate ◽  
Masami Ikeyama ◽  
Soji Miyagawa
Keyword(s):  
Monte Carlo Simulation ◽  
Monte Carlo ◽  
Ion Implantation ◽  
Gas Flow ◽  
Particle In Cell ◽  
Pet Bottles ◽  
Neutral Gas ◽  
Gas Plasma

Molecular-Scale and Wide-Energy-Range Tunneling Spectroscopy on Self-Assembled Monolayers of Alkanethiol Molecules

ACS Nano ◽  
2012 ◽  
Vol 6 (10) ◽  
pp. 8728-8734 ◽  
Author(s):  
Masato Nakaya ◽  
Masaya Shikishima ◽  
Masahiro Shibuta ◽  
Naoyuki Hirata ◽  
Toyoaki Eguchi ◽  
...  
Keyword(s):  
Energy Range ◽  
Tunneling Spectroscopy ◽  
Self Assembled Monolayers ◽  
Wide Energy Range ◽  
Molecular Scale ◽  
Assembled Monolayers ◽  
Wide Energy ◽  
Self Assembled

New measurements and analysis of elastic scattering of $$^{13}$$C by $$^{9}$$Be nuclei in a wide energy range

2021 ◽  
Vol 57 (7) ◽  
Author(s):  
Marzhan Nassurlla ◽  
N. Burtebayev ◽  
B. K. Karakozov ◽  
S. B. Sakuta ◽  
I. Boztosun ◽  
...  
Keyword(s):  
Elastic Scattering ◽  
Energy Range ◽  
Wide Energy Range ◽  
Wide Energy

Design of an ultrahigh-energy-resolution and wide-energy-range soft X-ray beamline

2013 ◽  
Vol 21 (1) ◽  
pp. 273-279 ◽  
Author(s):  
L. Xue ◽  
R. Reininger ◽  
Y.-Q. Wu ◽  
Y. Zou ◽  
Z.-M. Xu ◽  
...  
Keyword(s):  
Energy Range ◽  
Energy Resolution ◽  
Wide Energy Range ◽  
Ultrahigh Energy ◽  
Exit Slit ◽  
Shanghai Synchrotron Radiation Facility ◽  
X Ray ◽  
Variable Line ◽  
Line Spacing ◽  
Wide Energy

A new ultrahigh-energy-resolution and wide-energy-range soft X-ray beamline has been designed and is under construction at the Shanghai Synchrotron Radiation Facility. The beamline has two branches: one dedicated to angle-resolved photoemission spectroscopy (ARPES) and the other to photoelectron emission microscopy (PEEM). The two branches share the same plane-grating monochromator, which is equipped with four variable-line-spacing gratings and covers the 20–2000 eV energy range. Two elliptically polarized undulators are employed to provide photons with variable polarization, linear in every inclination and circular. The expected energy resolution is approximately 10 meV at 1000 eV with a flux of more than 3 × 1010 photons s−1at the ARPES sample positions. The refocusing of both branches is based on Kirkpatrick–Baez pairs. The expected spot sizes when using a 10 µm exit slit are 15 µm × 5 µm (horizontal × vertical FWHM) at the ARPES station and 10 µm × 5 µm (horizontal × vertical FWHM) at the PEEM station. The use of plane optical elements upstream of the exit slit, a variable-line-spacing grating and a pre-mirror in the monochromator that allows the influence of the thermal deformation to be eliminated are essential for achieving the ultrahigh-energy resolution.

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