Analytical dependence of effective atomic number on the elemental composition of matter and radiation energy in the range 10–1000 keV

Author:

Eritenko A.N.,Tsvetiansky A.L.,Polev A.A.

Publisher

Elsevier BV

Subject

Instrumentation,Nuclear and High Energy Physics

Reference24 articles.

1. The effective atomic numbers of materials for various gamma ray processes;Hine;Rhys. Rev.,1952

2. Effective atomic number of heterogeneous materials;Murty;Nature,1965

3. A.P. Ochkur, I.V. Tomsky, Yu.P. Yanshevsky, et al., Gamma methods in ore geology. Ed. A.P. Ochkur. Leningrad, Nauka, 1976, 407 p. (in Russian).

4. M.J. Berger, J.H. Hubbell, 1987/99. XCOM: Photon cross sections database, Web Version 1.2, available at http://physics nist.gov/xcom. National Institute of Standards and Technology, Gaithersburg, MD 20899, USA. Originally published as NBSIR 87-3597 “XCOM. Photon Cross Sections on Personal Computer”.

5. J.H. Hubbell, S.M. Zeltzer, Tables of X-ray mass attenuation coefficients from 1 keV to 20 MeV for elements Z=1 to Z=92.National Institute of Standarts and Tecnology (IR) Report No.5632 1995.

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1. Comparative study on results of calculating the effective atomic number by means of various methods in the photon energy region of 250–700 keV;Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms;2021-12

2. Estimation of the effective mass thickness and effective atomic number of the test object material by the dual energy method;Radiation Physics and Chemistry;2020-03

3. Separation of materials according to the effective atomic number using photons of two energies in the range of 60–700 keV;Nuclear Instruments and Methods in Physics Research Section B: Beam Interactions with Materials and Atoms;2020-01

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