Nature

Zeeman Effect of the Hyperfine Structure Components of the Mercury Resonance Line 2537 A

A. VIRONAS

Published Mar 28, 1936• 0 citations

Publisher

DOI: 10.1038/137531a0

Related papers

Zeeman- and Paschen-Back-effect of the hyperfine structure of the sodiumD 1-line

Laurentius Windholz

The European Physical Journal AJun 1, 198519 citations

Longitudinal and Transversal Zeeman Effects in D-Lines of Sodium and Green Line of Mercury

Hantaro Nagaoka

Proceedings of the Tokyo Mathematico-Physical Society. 2nd SeriesJun 27, 19100 citations

Zeeman- and Paschen-Back-effect of the hyperfine structure of the sodiumD 2-line

Laurentius Windholz, Maurizio E. Musso

Zeitschrift für Physik D Atoms Molecules and ClustersSep 1, 198821 citations

Hyperfine Structure of the Resonance Lines of Rubidium

A. V. Hollenberg

Physical ReviewJul 15, 19376 citations

Scattering in the wings of resonance lines and excitation of hyperfine structure levels.

Ia. B. Zeldovich, Igor I Sobel'man

Astronomy LettersMar 1, 19770 citations

Hyperfine Structure and Polarization of 1S01−2P13 of Mercury in Resonance Radiation

A. Ellett, Walter A. MacNair

Physical ReviewFeb 1, 192815 citations

Nature

Zeeman Effect of the Hyperfine Structure Components of the Mercury Resonance Line 2537 A

A. VIRONAS

Published Mar 28, 1936• 0 citations

Publisher

DOI: 10.1038/137531a0

Related papers

Zeeman- and Paschen-Back-effect of the hyperfine structure of the sodiumD 1-line

Laurentius Windholz

The European Physical Journal AJun 1, 198519 citations

Longitudinal and Transversal Zeeman Effects in D-Lines of Sodium and Green Line of Mercury

Hantaro Nagaoka

Proceedings of the Tokyo Mathematico-Physical Society. 2nd SeriesJun 27, 19100 citations

Zeeman- and Paschen-Back-effect of the hyperfine structure of the sodiumD 2-line

Laurentius Windholz, Maurizio E. Musso

Zeitschrift für Physik D Atoms Molecules and ClustersSep 1, 198821 citations

Hyperfine Structure of the Resonance Lines of Rubidium

A. V. Hollenberg

Physical ReviewJul 15, 19376 citations

Scattering in the wings of resonance lines and excitation of hyperfine structure levels.

Ia. B. Zeldovich, Igor I Sobel'man

Astronomy LettersMar 1, 19770 citations

Hyperfine Structure and Polarization of 1S01−2P13 of Mercury in Resonance Radiation

A. Ellett, Walter A. MacNair

The incomplete polarization of $\ensuremath{\lambda}2537\mathrm{A}$ of mercury in resonance radiation is due to the peculiar behavior of the outer two hyperfine structure lines. The three remaining hyperfine structure lines behave in accordance with the predictions of the theory of the anomalous Zeeman effect for a ${1}^{1}$ ${\mathrm{S}}_{0}$ - ${2}^{3}$ ${\mathrm{P}}_{1}$ line. Von Keussler's observation of complete polarization in 7900 gausses is explained, in part at least, by the observed shift of the -25.6 hyperfine structure line, and complete polarization is obtained with a field only 2000 gausses using a resonance radiation source.The incomplete polarization of $\ensuremath{\lambda}2537\mathrm{A}$ of mercury in resonance radiation is due to the peculiar behavior of the outer two hyperfine structure lines. The three remaining hyperfine structure lines behave in accordance with the predictions of the theory of the anomalous Zeeman effect for a ${1}^{1}$${\mathrm{S}}_{0}$-${2}^{3}$${\mathrm{P}}_{1}$ line. Von Keussler's observation of complete polarization in 7900 gausses is explained, in part at least, by the observed shift of the -25.6 hyperfine structure line, and complete polarization is obtained with a field only 2000 gausses using a resonance radiation source.

Physical ReviewFeb 1, 192815 citations

{1}^{1}

{\mathrm{S}}_{0}

{2}^{3}

{\mathrm{P}}_{1}

line. Von Keussler's observation of complete polarization in 7900 gausses is explained, in part at least, by the observed shift of the -25.6 hyperfine structure line, and complete polarization is obtained with a field only 2000 gausses using a resonance radiation source.