Titlebook: Beam-Foil Spectroscopy; Volume 1 Atomic Stru Ivan A. Sellin,David J. Pegg Book 1976 Plenum Press, New York 1976 UV.atomic collision.collisi

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https://doi.org/10.1007/978-3-540-70974-9correlation (the RHF result for . is 2.97 MHz and the experimental result. −1.42 MHz) and because Li is a few-electron system and thus computationally tractable. The situation differs from other well-investigated anomalies. (e.g. contact terms in B I .P. and N I .S.) due to the large cancellation am

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https://doi.org/10.1007/978-3-540-70974-9Only electric dipole decays were observed. Measurement of transition energies for 3d.4f → 3d. and 3d.4p → 3d. lines as high as Z=66 allows one to construct formulae for interpolating with rather good confidence to energies in the NiI sequence for intermediate Z. No detailed equivalent information ap

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Human Papillomavirus and CO2 Laser Treatments involving new elements, higher energies, a broader wavelength range, shorter time intervals, pulsed beams, different targets, and new configurations in geometry or external fields. However, what is perhaps not so trivial is to propose experiments for which there is a specific purpose, experiments

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Mutational Profile of HPV-Positive HNSCC,ium, calcium, iron, nickel, zinc, and krypton. There are no measurements to date known to us for any of the spectra of bromine, and there are very few measurements on scandium, titanium, vanadium, germanium, arsenic, and selenium.

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Teresa A. Anderson,Aaron C. Ermelh has been discussed for some years. The scope of the present contribution is to review the various approaches to a solution of the problems which have appeared in the literature. Also other aspects of beam-foil spectroscopy with slow, heavy ions will be discussed. Thus, when intense heavy ion beams

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