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Stark broadening of hydrogenic spectral lines by two-dimensional multimode quasimonochromatic electric fields

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Abstract

We studied the profile of the hydrogenic Ly-alpha line under the two-dimensional multimode quasimonochromatic electric field. We obtained the Stark profile of the main line and of the satellites in the form of the onefold integral. We demonstrated analytically and by numerical calculations that the Stark profile of the main line and of its satellites has a cusp in its center. This unusual shape of the Stark profile is a counterintuitive result.

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Data Availability Statement

This manuscript has no associated data or the data will not be deposited. [Authors’ comment: All data is included in the paper.]

Notes

  1. First, as noted in Sect. 4.1.5 of book [1], the problem involving a three-dimensional multimode QEF can be always reduced to the corresponding two-dimensional problem—see the transition from Eq. (4.1.34) to Eq. (4.1.35) in book [1]. Therefore, the three-dimensional setup in paper [8] is equivalent to the corresponding two-dimensional setup. Second, Kim and Wilhelm [8] obtained zero quasienergies for any ratio of the components of the multimode QEF, including the case where one of the QEF components is much smaller than the other one. Therefore, for proving that the result from paper [8] is erroneous, it was sufficient to show that the quasienergies are nonzeros for the case where one of the QEF components is much smaller than the other one.

  2. Here are some details. The argument f(w) of the exponential in Eq. (9) is: f(w) \(=\) - w\(^{\mathrm {2}}\) - [2D/(abw)]\(^{\mathrm {2}} \quad =\) - w\(^{\mathrm {2}}\) - w\(_{\mathrm {0}}^{\mathrm {4}}\)/w\(^{\mathrm {2}}\). We seek w \(=\) w\(_{\mathrm {0}}\)(1 \(+\) c), where \(| \mathrm{c} |< < 1\). This substitution, upon expanding up to the terms \(\sim \mathrm{c}^{\mathrm {2}}\), yields: f = - w\(_{\mathrm {0}}^{\mathrm {2}}\) - 4c\(^{\mathrm {2}}\)w\(_{\mathrm {0}}^{\mathrm {2}}\). Since c \(=\) (w - w\(_{\mathrm {0}})\)/w\(_{\mathrm {0}}\) and \(\mathrm{w}_{\mathrm {0}} \quad = [2 | D | /\mathrm{(ab)}]^{\mathrm {1/2}}\), we obtain f for expression (13).

References

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Oks, E. Stark broadening of hydrogenic spectral lines by two-dimensional multimode quasimonochromatic electric fields. Eur. Phys. J. D 75, 185 (2021). https://doi.org/10.1140/epjd/s10053-021-00194-5

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  • DOI: https://doi.org/10.1140/epjd/s10053-021-00194-5

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