Abstract

We have measured the differential Stark shift in the 6s6p³P₁ state of mercury. The technique we used was to measure the shift in the magnetic-field level crossing in ¹⁹⁹Hg when an additional electric field was applied. We obtained the value E(m_J = ±1) − E(m_J = 0) = −2.367 ± 0.024 kHz/(kV/cm)² · ∊², where ∊ is the electric field.

© 1972 Optical Society of America

Absolute frequency and isotope shift measurements of mercury ¹S₀–³P₁ transition

Marcin Witkowski, Grzegorz Kowzan, Rodolfo Munoz-Rodriguez, Roman Ciuryło, Piotr Szymon Żuchowski, Piotr Masłowski, and Michał Zawada
Opt. Express 27(8) 11069-11083 (2019)

Hyperfine Structure in the ³P₁ Level of the Twenty-Four-Hour Isomer of Mercury 197†

Henry R. Hirsch
J. Opt. Soc. Am. 51(11) 1192-1202 (1961)

Isotope shift of 3 × 10⁵-yr ²⁰²Pb in the 6p² ³P₀−6p7s ³P1° 283.3-nm resonance line

F. A. Moscatelli, O. Redi, H. H. Stroke, R. L. Wiggins, and R. A. Naumann
J. Opt. Soc. Am. 73(2) 156-159 (1983)

Configurations 4f¹⁰6s6p and 4f⁹5d6s² in Neutral Dysprosium†

Donald C. Griffin, John S. Ross, and Robert D. Cowan
J. Opt. Soc. Am. 62(4) 571-579 (1972)

Isotope shifts in the 6p² P3₀-6p7s P31∘ 283.3-nm line of natural lead

F. A. Moscatelli, O. Redi, P. Schönberger, H. H. Stroke, and R. L. Wiggins
J. Opt. Soc. Am. 72(7) 918-922 (1982)