Research Article
Year 2022,
Volume: 26 Issue: 1, 149 - 155, 28.02.2022
Abstract
References
- [1] K. Ikeda, “ITER on the road to fusion energy,” Nucl. Fusion, vol. 50, pp. 014002-10, 2010.
- [2] E. Hinnov, “Highly ionized atoms in tokamak discharges,” Phys. Rev. A, vol. 14, pp. 1533-1541, 1976.
- [3] I. Martinson and A. Gaupp, “Atomic physics with ion accelerators - beam-foil spectroscopy,” Phys. Rep., vol.15, pp. 113-180, 1974.
- [4] F. Hu, M. Mei, C. Han, B. Han, G. Jiang, and J. Yang, “Accurate multiconfiguration Dirac–Hartree–Fock calculations of transition probabilities for magnesium-like ions” J. Quant. Spectrosc. Radiat.Transfer, vol.149, pp.158-167, 2014.
- [5] J.A. Santana and E. Trabert. “Resonance and intercombination lines in Mg-like ions of atomic numbers Z = 13–92,” Phys. Rev. A, vol. 91, pp. 022503-7, 2015.
- [6] J.A. Santana, “Relativistic MR-MP energy levels: Low-lying states in the Mg isoelectronic sequence,” At. Data Nucl. Data Tables, vol. 111-112, pp. 87-186, 2016.
- [7] C. Iorga and V. Stancalie, “The study of the core–valence and core–core correlation effects on the radiative properties along the magnesium isoelectronic sequence,”Atomic Data and Nuclear Data Tables, vol. 123–124, pp.313-328, 2018.
- [8] L. Özdemir, G. Günday Konan and S. Kabakçı, “Energies and Radiative Transition Parameters for Mg-Like Tungsten,” Acta Phys. Pol. A, vol.124, no.4, pp. 649-657, 2013.
- [9] G. G. Konan, S. Kabakçı and L. Özdemir, “E1, E2 and M1 transitions between n=3 levels in magnesium-like tungsten,”Iran. J. Sci. Technol., vol. 38A4, pp. 415-421, 2014.
- [10] G. G. Konan, L. Özdemir and G. Ürer, “Energy levels and strong electric dipole transitions in magnesium-like gold,” J. Quant. Spectrosc. Radiat. Transfer, vol. 145, pp. 110-120, 2014.
- [11] G. G.Konan and L. Ozdemir, “Energies, wavelengths, transition probabilities, and oscillator strengths for electric dipole transitions of Na-like and Mg-like mercury,” Can. J. Phys., vol. 96, pp. 1098–1103, 2018.
- [12] G. G. Konan, “Calculation of energy levels and electric dipole (E1) transition parameters for magnesium-like bismuth, ”Can. J. Phys., vol. 97, pp. 959–965, 2019.
- [13] N. R. Badnell, “A Breit–Pauli distorted wave implementation for AUTOSTRUCTURE,” Comput. Phys. Commun., vol. 182, pp.1528-1535, 2011.
- [14] N. R. Badnell, “Dielectronic recombination of Fe 22+ and Fe21+,” J. Phys. B, vol. 19, pp. 3827-3835, 1986.
- [15] https://www.adas.ac.uk/man/chap7-01.pdf
- [16] N. R. Badnell, “On the effects of the two-body non-fine-structure operators of the Breit - Pauli Hamiltonian,” J. Phys. B, vol. 30, pp. 1-11, 1997.
- [17] L.W.Acton, M.E. Bruner and W.A. Brown, “Rocket spectrogram of a solar- flareinthe 10–100 Å region,”Astrophys. Journal, vol.291, pp. 865-78, 1985.
- [18] F.P. Keenan, J.J.Drake, S.Chung, N.S.Brickhouse, K.M.Aggarwal ans A.Z. Msezane, et al. , “Soft x-ray emission lines of Fe XV in solar flare observations and the chandra spectrum of capella, ”Astrophys. Journal, vol. 645, pp. 597–604, 2006.
- [19] S.O. Kastner, M.Swartz, A.K.Bhatia and J.Lapides, “Observations of n=3, n=4 transitions in the Mg I and Si I sequences for elements chromium through zinc,” J Opt. Soc. Am., vol.68, pp. 1558–64, 1978.
Year 2022,
Volume: 26 Issue: 1, 149 - 155, 28.02.2022
Abstract
In the present work, we have reported the energy levels, wavelengths, weighted oscillator strengths, and transition probabilities for electric dipole (E1) transitions of magnesium like platinum (Pt LXVII, Z=78). Accurate knowledge of Mg-like ions are of great importance for astrophysics, plasma, and thermonuclear fusion research. The atomic data are calculated with the AUTOSTRUCTURE code, where relativistic corrections are introduced according to the Breit–Pauli distorted wave approach. In the calculations, quantum electrodynamics effects and correlation contributions have been considered. The present results are in good agreement with other available values. There are no experimental works for Pt LXVII in the literature. We predict new theoretical data for several levels will be helpful for future experimental works.
References
- [1] K. Ikeda, “ITER on the road to fusion energy,” Nucl. Fusion, vol. 50, pp. 014002-10, 2010.
- [2] E. Hinnov, “Highly ionized atoms in tokamak discharges,” Phys. Rev. A, vol. 14, pp. 1533-1541, 1976.
- [3] I. Martinson and A. Gaupp, “Atomic physics with ion accelerators - beam-foil spectroscopy,” Phys. Rep., vol.15, pp. 113-180, 1974.
- [4] F. Hu, M. Mei, C. Han, B. Han, G. Jiang, and J. Yang, “Accurate multiconfiguration Dirac–Hartree–Fock calculations of transition probabilities for magnesium-like ions” J. Quant. Spectrosc. Radiat.Transfer, vol.149, pp.158-167, 2014.
- [5] J.A. Santana and E. Trabert. “Resonance and intercombination lines in Mg-like ions of atomic numbers Z = 13–92,” Phys. Rev. A, vol. 91, pp. 022503-7, 2015.
- [6] J.A. Santana, “Relativistic MR-MP energy levels: Low-lying states in the Mg isoelectronic sequence,” At. Data Nucl. Data Tables, vol. 111-112, pp. 87-186, 2016.
- [7] C. Iorga and V. Stancalie, “The study of the core–valence and core–core correlation effects on the radiative properties along the magnesium isoelectronic sequence,”Atomic Data and Nuclear Data Tables, vol. 123–124, pp.313-328, 2018.
- [8] L. Özdemir, G. Günday Konan and S. Kabakçı, “Energies and Radiative Transition Parameters for Mg-Like Tungsten,” Acta Phys. Pol. A, vol.124, no.4, pp. 649-657, 2013.
- [9] G. G. Konan, S. Kabakçı and L. Özdemir, “E1, E2 and M1 transitions between n=3 levels in magnesium-like tungsten,”Iran. J. Sci. Technol., vol. 38A4, pp. 415-421, 2014.
- [10] G. G. Konan, L. Özdemir and G. Ürer, “Energy levels and strong electric dipole transitions in magnesium-like gold,” J. Quant. Spectrosc. Radiat. Transfer, vol. 145, pp. 110-120, 2014.
- [11] G. G.Konan and L. Ozdemir, “Energies, wavelengths, transition probabilities, and oscillator strengths for electric dipole transitions of Na-like and Mg-like mercury,” Can. J. Phys., vol. 96, pp. 1098–1103, 2018.
- [12] G. G. Konan, “Calculation of energy levels and electric dipole (E1) transition parameters for magnesium-like bismuth, ”Can. J. Phys., vol. 97, pp. 959–965, 2019.
- [13] N. R. Badnell, “A Breit–Pauli distorted wave implementation for AUTOSTRUCTURE,” Comput. Phys. Commun., vol. 182, pp.1528-1535, 2011.
- [14] N. R. Badnell, “Dielectronic recombination of Fe 22+ and Fe21+,” J. Phys. B, vol. 19, pp. 3827-3835, 1986.
- [15] https://www.adas.ac.uk/man/chap7-01.pdf
- [16] N. R. Badnell, “On the effects of the two-body non-fine-structure operators of the Breit - Pauli Hamiltonian,” J. Phys. B, vol. 30, pp. 1-11, 1997.
- [17] L.W.Acton, M.E. Bruner and W.A. Brown, “Rocket spectrogram of a solar- flareinthe 10–100 Å region,”Astrophys. Journal, vol.291, pp. 865-78, 1985.
- [18] F.P. Keenan, J.J.Drake, S.Chung, N.S.Brickhouse, K.M.Aggarwal ans A.Z. Msezane, et al. , “Soft x-ray emission lines of Fe XV in solar flare observations and the chandra spectrum of capella, ”Astrophys. Journal, vol. 645, pp. 597–604, 2006.
- [19] S.O. Kastner, M.Swartz, A.K.Bhatia and J.Lapides, “Observations of n=3, n=4 transitions in the Mg I and Si I sequences for elements chromium through zinc,” J Opt. Soc. Am., vol.68, pp. 1558–64, 1978.
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Details
| Primary Language | English |
|---|---|
| Subjects | Metrology, Applied and Industrial Physics |
| Journal Section | Research Articles |
| Authors | |
| Early Pub Date | February 23, 2022 |
| Publication Date | February 28, 2022 |
| Submission Date | November 8, 2021 |
| Acceptance Date | December 29, 2021 |
| Published in Issue | Year 2022 Volume: 26 Issue: 1 |
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