scholarly journals Dosimetry for Cell Irradiation using Orthovoltage (40-300 kV) X-Ray Facilities

10.3791/61645 ◽  
2021 ◽  
Author(s):  
Morgane Dos Santos ◽  
Vincent Paget ◽  
François Trompier ◽  
Gaëtan Gruel ◽  
Fabien Milliat
Keyword(s):  
X Ray ◽  
Cell Irradiation

X-ray microbeam measurement with radiophotoluminescent glass plate for single cell irradiation

2008 ◽  
Vol 43 (2-6) ◽  
pp. 912-916 ◽  
Author(s):  
Fuminobu Sato ◽  
T. Kuchimaru ◽  
T. Ikeda ◽  
K. Shimizu ◽  
Y. Kato ◽  
...  
Keyword(s):  
Single Cell ◽  
Glass Plate ◽  
X Ray ◽  
Cell Irradiation

scholarly journals Ion, X-Ray, UV And Neutron Microbeam Systems For Cell Irradiation

2011 ◽  
Author(s):  
A. W. Bigelow ◽  
G. Randers-Pehrson ◽  
G. Garty ◽  
C. R. Geard ◽  
Y. Xu ◽  
...  
Keyword(s):  
X Ray ◽  
Cell Irradiation

PARTIAL CELL IRRADIATION AND SOFT X-RAY MICRODIFFRACTION

1963 ◽  
Author(s):  
V. W. Burns ◽  
H. H. Pattee
Keyword(s):  
X Ray ◽  
Cell Irradiation

Microdosimetric characteristics of micro X-ray beam for single cell irradiation

2006 ◽  
Vol 53 (3) ◽  
pp. 1363-1366 ◽  
Author(s):  
T. Kuchimaru ◽  
F. Sato ◽  
Y. Higashino ◽  
K. Shimizu ◽  
Y. Kato ◽  
...  
Keyword(s):  
Single Cell ◽  
X Ray ◽  
Cell Irradiation

Carbon-nanotube field emission electron and X-ray technology for medical research and clinical applications

2017 ◽  
Author(s):  
Sigen Wang ◽  
Otto Zhou ◽  
Sha Chang
Keyword(s):  
Carbon Nanotube ◽  
Medical Research ◽  
Single Cell ◽  
Field Emission ◽  
Small Animal ◽  
Clinical Applications ◽  
X Ray ◽  
Clinical Cancer ◽  
Cell Irradiation ◽  
Cancer Studies

This article describes carbon-nanotube based X-ray technologies for medical research and clinical applications, including an X-ray source, microfocus X-ray tube, microcomputed tomography scanner, stationary digital breast tomosynthesis, microradiotherapy system, and single-cell irradiation system. It first examines electron field emission from carbon nanotubes before discussing carbon-nanotube field emission electron and X-ray technologies in greater detail. It highlights the enormous promise of these systems in commercial and research application for the future in diagnostic medical imaging; in-vivo imaging of small-animal modelsfor pre-clinical cancer studies; security screening; industrial inspection; cancer radiotherapy of small-animal models for pre-clinical cancer studies; and basic cancer research using single-cell irradiation.

Microdosimetric Characteristics of Micro X-Ray Beam for Single Cell Irradiation

2006 ◽  
Author(s):  
T. Kuchimaru ◽  
F. Sato ◽  
Y. Higashino ◽  
K. Shimizu ◽  
Y. Kato ◽  
...  
Keyword(s):  
Single Cell ◽  
X Ray ◽  
Cell Irradiation

scholarly journals Single floating cell irradiation technique with an X-ray microbeam

2018 ◽  
Vol 11 (1) ◽  
pp. 83-88
Author(s):  
Fuminobu Sato ◽  
Kikuo Shimizu ◽  
Isao Murata
Keyword(s):  
X Ray ◽  
Floating Cell ◽  
Cell Irradiation

Space and Time Distribution of Hard X-Ray Emission in a Loop at the Beginning of a Flare

1994 ◽  
Vol 144 ◽  
pp. 275-277
Author(s):  
M. Karlický ◽  
J. C. Hénoux
Keyword(s):  
Time Distribution ◽  
Electron Bombardment ◽  
Spatial Evolution ◽  
Superthermal Electrons ◽  
Flare Loop ◽  
X Ray ◽  
Superthermal Electron ◽  
Flare Loops ◽  
Chromospheric Evaporation ◽  
Temporal And Spatial

AbstractUsing a new ID hybrid model of the electron bombardment in flare loops, we study not only the evolution of densities, plasma velocities and temperatures in the loop, but also the temporal and spatial evolution of hard X-ray emission. In the present paper a continuous bombardment by electrons isotropically accelerated at the top of flare loop with a power-law injection distribution function is considered. The computations include the effects of the return-current that reduces significantly the depth of the chromospheric layer which is evaporated. The present modelling is made with superthermal electron parameters corresponding to the classical resistivity regime for an input energy flux of superthermal electrons of 109erg cm−2s−1. It was found that due to the electron bombardment the two chromospheric evaporation waves are generated at both feet of the loop and they propagate up to the top, where they collide and cause temporary density and hard X-ray enhancements.

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