Optical absorption spectrum of hydrogenic atoms in a strong magnetic field☆
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Cited by (202)
On the chemical bond complexity of the H<inf>2</inf><sup>+</sup> in 1-D: The ground-state avoided crossing
2021, Computational and Theoretical ChemistryMagnetoexcitons in monolayer transition-metal dichalcogenides
2020, Physics Letters, Section A: General, Atomic and Solid State PhysicsExciton absorption in narrow armchair graphene nanoribbons
2016, Physica B: Condensed MatterCitation Excerpt :Our mathematical approach is based on matching the Coulomb wave functions with the functions obtained upon solution of the Dirac equation in the intermediate region by the iteration method. This procedure has been originally developed by Hasegawa and Howard [4] for 3D excitons subject to a strong magnetic field and then successfully extended to problems related to semiconductor (see [5] and references therein) and graphene [7,18] nanostructures. The dependence of the exciton absorption coefficient on the ribbon width is studied analytically.
Energy levels of light atoms in strong magnetic fields
2014, Advances in Atomic, Molecular and Optical PhysicsCitation Excerpt :Advances in atomic structure theory were therefore leaning toward solid-state applications. It was only in 1961 that Hasegawa and Howard (1961) calculated the spectrum and oscillatoi strengths of the hydrogen atom in a uniform strong magnetic field and showed that in the limit of infinite field strengths, a simplified picture is obtained wherein the nucleus becomes the perturbation to the interaction of the electron with the field. This was the very first study to obtain the spectrum of hydrogen in strong magnetic fields.
Anisotropic magnetoexcitons in two-dimensional transition metal trichalcogenide semiconductors
2022, Physical Review ResearchAnalytic approximations to photoabsorption cross sections of once-ionized helium in magnetar atmospheres
2021, Journal of Physics: Conference Series
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A preliminary report on this work is presented in the Bull. Amer. Phys. Soc. (ser. 2) 5, 178 (1960).