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Odd-even effects for number of atoms in antiferromagnetic atomic chains on ferromagnetic substrate
Physics of the Solid State, 2010The ground state of an antiferromagnetic atomic chain on a ferromagnetic substrate has been studied taking into account the single-ion anisotropy energy. Qualitatively different behavior of even and odd atomic chains has been demonstrated. A phase diagram in terms of chain length-ferromagnet exchange field has been constructed.
A. A. Berzin, A. I. Morosov, A. S. Sigov
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Radiation Physics and Chemistry, 2017
Abstract The photon interaction parameters such as mass attenuation coefficient, effective atomic number, effective electron density, buildup factor have been measured for Fe(NO3)3, V4O2, NaCO3·H2O, C6H5FeO7·H2O and CuCI compounds using 137Ba, 157Gd and 241Am γ-rays sources in stable geometry.
Levet, Aytaç, Özdemir, Yüksel
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Abstract The photon interaction parameters such as mass attenuation coefficient, effective atomic number, effective electron density, buildup factor have been measured for Fe(NO3)3, V4O2, NaCO3·H2O, C6H5FeO7·H2O and CuCI compounds using 137Ba, 157Gd and 241Am γ-rays sources in stable geometry.
Levet, Aytaç, Özdemir, Yüksel
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Effective atomic number rule to exchange energy
1995This chapter assesses the effective atomic number rule. The effective atomic number rule applies to molecules where covalent bonding is strong and all the valence orbitals are being used in either homo- and hetero-polar covalent bonds or are occupied by non-binding electron-pairs.
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Effective Atomic Numbers of Low-Z Compounds for Photon Interaction
Nuclear Science and Engineering, 1997Effective atomic numbers are derived for the low-Z compounds polyethylene, polycarbonate, Teflon, Mylar, polystyrene, and polyvinyl chloride for total photon interaction in the 10- to 20000-keV energy region. The number generally decreases and then increases with increasing energy.
S. Guru Prasad +2 more
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Photon attenuation coefficient and effective atomic number study of cements
Applied Radiation and Isotopes, 1993Abstract The mass attenuation coefficients μ c ρ and the effective atomic numbers of four different cements have been calculated for total and partial photon interaction processes in the energy range 0.001–100,000 MeV. Small variations were noted in the mass attenuation coefficients due to chemical composition of cements for total and ...
G.S. Bhandal, K. Singh
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Effective density and atomic number determined from diffraction profiles
SPIE Proceedings, 2006X-ray diffraction (XRD) profiles are conventionally used to determine lattice spacings via Bragg's law in order to characterize crystalline materials. It does not appear to be widely known that they also permit compositional information, such as effective atomic number and a density descriptor, to be determined from materials having little or no ...
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Atomic-number dependence of relativistic effects on chemical bonding
2000Abstract The Atomic-number dependence of the relativistic effects on chemical bonding has been studied using the difference (ΔAPB) in the bond overlap populations between the relativistic and nonrelativistic DV-Xα calculations for various XH diatomic hydrides (XCu, Ag, and Au) and XF 6 hexafluorides (XS, Se, Mo, Ru, Rh, Te, W, Re, Os, Ir, Pt, U ...
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Effective Atomic Numbers for Fe–Mn Alloy Using Transmission Experiment
Chinese Physics Letters, 2007The effective atomic numbers (Zeff) and effective electron density (Ne) for Fe–Mn alloy with different Mn contents are calculated using the mass attenuation coefficients μ/ρ obtained via XCOM in the photon energy range of 1 keV–1 GeV. The results are compared with the values measured at the photon energy of 662, 1170 and 1332 keV.
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Determination of the effective atomic numbers of light composite materials
2009 IEEE Intrumentation and Measurement Technology Conference, 2009The analysis of physical and chemical characteristics of materials (composite or not) via the determination of change in the effective atomic number (Zeff) can be performed by measuring the relation between the intensities of γ-rays under coherent (Rayleigh) and inelastic (Compton) scattering.
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