Effect of geometrical parameter’s uncertainty of BIXS experimental setup for tritium analysis

[1]  Jingjun Zhu,et al.  Tritium analysis in titanium films by the BIXS method , 2012 .

[2]  S. Peng,et al.  Effects of internal bremsstrahlung of tritium β-decay and surface roughness in the BIXS method , 2011 .

[3]  Jingjun Zhu,et al.  Bremsstrahlung spectra produced by kilovolt electron impact on thick targets , 2009 .

[4]  F. Salvat,et al.  Cross sections for ionization of K, L and M shells of atoms by impact of electrons and positrons with energies up to 1 GeV: Analytical formulas , 2009 .

[5]  Jingjun Zhu,et al.  Measurements of the K-shell ionization cross sections of Si by 3-25-keV electron impact using the thick-target method , 2009 .

[6]  Z. An,et al.  Comparison of reconstruction methods of depth distribution of tritium in materials based on BIXS , 2009 .

[7]  M. Matsuyama.  Development of a new detection system for monitoring high-level tritiated water , 2008 .

[8]  Q. Hou,et al.  Reconstruction of depth distribution of tritium in materials by β-ray induced X-ray spectrometry , 2008 .

[9]  M. Mesradi,et al.  Experimental characterization and Monte Carlo simulation of Si(Li) detector efficiency by radioactive sources and PIXE. , 2008, Applied radiation and isotopes : including data, instrumentation and methods for use in agriculture, industry and medicine.

[10]  Francesc Salvat,et al.  Monte Carlo simulation of characteristic x-ray emission from thick samples bombarded by kiloelectronvolt electrons , 2008 .

[11]  Francesc Salvat,et al.  Calculations of inner-shell ionization by electron impact with the distorted-wave and plane-wave Born approximations , 2008 .

[12]  I. M. Kravchenko,et al.  Comparative study of the tritium distribution in metals , 2008 .

[13]  M. Matsuyama,et al.  New technique for non-destructive measurements of tritium in future fusion reactors , 2007 .

[14]  V. Philipps,et al.  Applicability of β-ray-induced X-ray spectrometry to in situ measurements of tritium retention in plasma-facing materials in ITER , 2006 .

[15]  F. Salvat,et al.  Distorted-wave calculation of cross sections for inner-shell ionization by electron and positron impact , 2003 .

[16]  V. Philipps,et al.  Non-destructive tritium measurements of Mk IIA divertor tile by BIXS , 2003 .

[17]  J. Sempau,et al.  Monte Carlo simulation of bremsstrahlung emission by electrons , 2002 .

[18]  V. Philipps,et al.  Nondestructive measurement of surface tritium by β-ray induced X-ray spectrometry (BIXS) , 2001 .

[19]  Kiyoshi Hasegawa,et al.  Tritium assay in materials by the bremsstrahlung counting method , 1998 .

[20]  J. Weese.  A regularization method for nonlinear ill-posed problems , 1993 .

[21]  Martin J. Berger,et al.  Bremsstrahlung energy spectra from electrons with kinetic energy 1 keV–10 GeV incident on screened nuclei and orbital electrons of neutral atoms with Z = 1–100 , 1986 .

[22]  Martin J. Berger,et al.  Bremsstrahlung spectra from electron interactions with screened atomic nuclei and orbital electrons , 1985 .

[23]  R. H. Pratt,et al.  Shape functions for atomic-field bremsstrahlung from electrons of kinetic energy 1–500 keV on selected neutral atoms 1 ≤ Z ≤ 92 , 1983 .

[24]  R. H. Pratt,et al.  Bremsstrahlung energy spectra from electrons of kinetic energy 1 keV ≤ T1 ≤ 2000 keV incident on neutral atoms 2 ≤ Z ≤ 92 , 1977 .

[25]  F. Bloch.  On the Continuous ?-Radiation Accompanying the -Decay , 1936 .

[26]  G. Uhlenbeck,et al.  Emission of gamma radiation during the beta decay of nuclei , 1936 .