2009
DOI: 10.1016/j.nimb.2009.08.012
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A microfocus X-ray tube based on a microstructured X-ray target

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Cited by 20 publications
(10 citation statements)
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“…For example, if the electron source energy was considered 50 kev, then the highest-energy in the electron-photon physics card was selected as 51kev to avoid confusion in the calculations. In calculating the spectra and range of dosage, considerations were as follows: output window material (substrates) of beryllium with a thickness of 0.5 mm, due to advantages such as transparency to shorter X-ray wavelengths, availability, high thermal capacity and high strength to weight ratio [ 38 ], low atomic number and X-ray transport without absorption even at low energies [ 39 ]. At all stages of simulation, the sources were placed in spherical phantom, and the density of water or air can be selected depending on the type of output.…”
Section: Methodsmentioning
confidence: 99%
“…For example, if the electron source energy was considered 50 kev, then the highest-energy in the electron-photon physics card was selected as 51kev to avoid confusion in the calculations. In calculating the spectra and range of dosage, considerations were as follows: output window material (substrates) of beryllium with a thickness of 0.5 mm, due to advantages such as transparency to shorter X-ray wavelengths, availability, high thermal capacity and high strength to weight ratio [ 38 ], low atomic number and X-ray transport without absorption even at low energies [ 39 ]. At all stages of simulation, the sources were placed in spherical phantom, and the density of water or air can be selected depending on the type of output.…”
Section: Methodsmentioning
confidence: 99%
“…[ 15 17 ], is employed. This method is used to express the intensity of X-ray photons Φ c ( x , hv ) emitted from the position x of target within the energy interval from hv to hv + d ( hv ) as: where Z is the atomic number of the target material; K is the constant K = 1.35 × 10 9 photons sr −1 mA −1 keV −1 s −1 ; hv 0 the maximum photon energy equal to the operation voltage; i e the tube current; Ω the solid angle in which the X-ray photons are emitted; n = 1, x = 1.109 − 0.00435 Z + 0.00175 hv 0 , and f the absorption term which describes the attenuation of emitted X-rays into the anode by Love and Scott’s distribution [ 11 , 18 ].…”
Section: Theories and Methodsmentioning
confidence: 99%
“…Ihsan et al . [ 11 ] proposed a micro-structured X-ray target for the purpose of achieving a small active X-ray focal spot size with an unfocused electron beam. They assumed that X-rays are produced only at the micro-structured target when irradiated with a larger scale electron beam, so the focal spot size of the generated X-ray is determined only by the lateral size of the microstructures.…”
Section: Introductionmentioning
confidence: 99%
“…A beryllium (Be) window with a thickness of 0.5 mm was used. The target parameters have been studied and optimized by our group, and the details can be found elsewhere (Ihsan et al, 2007(Ihsan et al, , 2009(Ihsan et al, , 2011. The photon flux averaged over the tally surface was obtained using 1 Â 10 9 particle histories with an interval of 100 eV.…”
Section: Angular Distribution Of Characteristic X-raysmentioning
confidence: 99%