Energy calculation of K1L1 multiply ionized Kβ satellite spectra emitted from Al, Al2O3, Si and SiO2

T. Yamamoto; M. Mochizuki; T. Suzuki; M. Uda

doi:10.1016/0168-583X(95)00881-0

Energy calculation of K¹L¹ multiply ionized Kβ satellite spectra emitted from Al, Al₂O₃, Si and SiO₂

T. Yamamoto, M. Mochizuki, T. Suzuki, M. Uda

School of Fundamental Science and Engineering

Research output: Contribution to journal › Article › peer-review

1 Citation (Scopus)

Abstract

Final states of a Kβ X-ray transition from a K¹L¹ multiply ionized state and a KLVAuger transition from a K¹L⁰ state are common in electronic configurations. Considering the above situation we developed a new method to calculate energies of the Kβ satellites emitted from the third-row elements in which informations on chemical bondings are reflected. For this purpose observed energies of the KLV Auger and calculated results for isolated atoms using the nonrelativistic Hartree-Fock-Slater orbital calculation were employed. The energies of the K¹L¹ Kβ satellites which were emitted from Al, Al₂O₃, Si and SiO₂ were calculated here for the first time.

Original language	English
Pages (from-to)	23-27
Number of pages	5
Journal	Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms
Volume	109-110
DOIs	https://doi.org/10.1016/0168-583X(95)00881-0
Publication status	Published - 1996 Apr

ASJC Scopus subject areas

Nuclear and High Energy Physics
Instrumentation

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title = "Energy calculation of K1L1 multiply ionized Kβ satellite spectra emitted from Al, Al2O3, Si and SiO2",

abstract = "Final states of a Kβ X-ray transition from a K1L1 multiply ionized state and a KLVAuger transition from a K1L0 state are common in electronic configurations. Considering the above situation we developed a new method to calculate energies of the Kβ satellites emitted from the third-row elements in which informations on chemical bondings are reflected. For this purpose observed energies of the KLV Auger and calculated results for isolated atoms using the nonrelativistic Hartree-Fock-Slater orbital calculation were employed. The energies of the K1L1 Kβ satellites which were emitted from Al, Al2O3, Si and SiO2 were calculated here for the first time.",

author = "T. Yamamoto and M. Mochizuki and T. Suzuki and M. Uda",

year = "1996",

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doi = "10.1016/0168-583X(95)00881-0",

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T1 - Energy calculation of K1L1 multiply ionized Kβ satellite spectra emitted from Al, Al2O3, Si and SiO2

AU - Yamamoto, T.

AU - Mochizuki, M.

AU - Suzuki, T.

AU - Uda, M.

PY - 1996/4

Y1 - 1996/4

N2 - Final states of a Kβ X-ray transition from a K1L1 multiply ionized state and a KLVAuger transition from a K1L0 state are common in electronic configurations. Considering the above situation we developed a new method to calculate energies of the Kβ satellites emitted from the third-row elements in which informations on chemical bondings are reflected. For this purpose observed energies of the KLV Auger and calculated results for isolated atoms using the nonrelativistic Hartree-Fock-Slater orbital calculation were employed. The energies of the K1L1 Kβ satellites which were emitted from Al, Al2O3, Si and SiO2 were calculated here for the first time.

AB - Final states of a Kβ X-ray transition from a K1L1 multiply ionized state and a KLVAuger transition from a K1L0 state are common in electronic configurations. Considering the above situation we developed a new method to calculate energies of the Kβ satellites emitted from the third-row elements in which informations on chemical bondings are reflected. For this purpose observed energies of the KLV Auger and calculated results for isolated atoms using the nonrelativistic Hartree-Fock-Slater orbital calculation were employed. The energies of the K1L1 Kβ satellites which were emitted from Al, Al2O3, Si and SiO2 were calculated here for the first time.

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JO - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms

JF - Nuclear Instruments and Methods in Physics Research, Section B: Beam Interactions with Materials and Atoms

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