2014
DOI: 10.1088/0253-6102/62/6/17
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Polarizabilities and Hyperpolarizabilities for Lithium Atoms in Debye Plasmas

Abstract: The effects of plasma environments on energies, oscillator strengths, polarizabilities and hyperpolarizabilities for lithium atom have been calculated by combining the l-dependent model potential of free lithium atom and linear variation method based on B-spline basis functions. The influence of plasma on lithium atom is represented by the Debye screened potential, which describes effectively the averaged effect of the plasma environment on atomic spectra. The results are in agreement with other reported ones.

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Cited by 11 publications
(4 citation statements)
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“…For example, it is related to another experimentally significant macroscopic property called refractive index [60]. The static 2 l -pole polarizability in terms of oscillator strengths for different energy state combinations is given by the relation [55][56][57]61]…”
Section: Theorymentioning
confidence: 99%
“…For example, it is related to another experimentally significant macroscopic property called refractive index [60]. The static 2 l -pole polarizability in terms of oscillator strengths for different energy state combinations is given by the relation [55][56][57]61]…”
Section: Theorymentioning
confidence: 99%
“…The effects of plasma environments on the transition energies, oscillator strengths, polarizabilities and hyperpolarizabilities of different atoms such as helium, lithium and sodium have been reported recently [38][39][40]. In the present work, a spherically confined hydrogen atom embedded in dense quantum plasma characterized by ECSCP is considered and the energy spectra, dipole matrix elements, and oscillator strengths for the system have been determined.…”
Section: Introductionmentioning
confidence: 96%
“…Dipole polarizability gives the lowest order response of system to applied fields while quadrupole and octupole polarizabilities refer to higher order interactions. The static 2l‐pole polarizability, where l = 1, 2, and 3 for dipole, quadrupole, and octupole cases, respectively, is given by the relation αl=nn2|ψn(r)|rl|ψn(r)|2(EnEn)false(EnEnfalse)2, where the initial state is n and the summation is over all intermediate vibrational states including the continuum.…”
Section: Theory and Computational Detailsmentioning
confidence: 99%