none4noA heterodyne spectroscopic scheme, using only one laser tuned to the atomic wavelength, is applied to the measurement of the He-3(F = 1/2-1/2 component)He-4 separation for the 2 S-3(1) - P-3(0) transition at 389 nm. The experimental result is 45 394 425(137) kHz and the isotope shift deduced in the absence of hyperfine structure is 42 184 180(139) kHz. A new value of the He-3 nuclear charge radius is obtained, [r2]1/2 = 1.923(36) fm, in a regime of low energy and momentum transfer.openMarin F.; Minardi F.; Pavone F.S.; Inguscio M.Marin F.; Minardi F.; Pavone F.S.; Inguscio M
We have calculated ac polarizabilities of the 2 3 S and 2 1 S states of both He 4 and He 3 in the ra...
An experiment is proposed to excite the “forbidden” $1s2s\,^3S_1$ - $1s2s\,^1S_0$ magnetic dipole ($...
An experiment is proposed to excite the "forbidden" 1s2s(3) S-1 - 1s2s(1) S-0 magnetic dipole (M1) t...
A heterodyne spectroscopic scheme, using only one laser tuned to the atomic wavelength, is applied t...
We perform high precision measurements of an isotope shift between the two stable isotopes of helium...
A source of narrow bandwidth (<800 MHz) tunable laser radiation at 58.4 nm has been developed and is...
Abstract. Accurate Quantum-Electrodynamics (QED) tests of the simplest bound three body atomic syste...
The He4 fine structure and He3 hyperfine structure as well as the isotope shift between He4 and He3 ...
With a phase-modulated extreme ultraviolet pulsed laser sourer the frequency of the I S-1-2 P-1 tran...
An rms nuclear charge radius rc =1.9642 (11) fm for He3 is derived from measurements of the 2 S13 -2...
The goal of this project was to measure the hyperfine structure of $\overline{\text{p}}^3$He$^+$ usi...
The unusually large hyperfine structure splittings in the 23P state of the 3He isotope is measured...
Abstract. We have measured the absolute frequency of the 1557-nm doubly forbidden transition between...
The hyperfine structure of 3He and the isotope shift Δ T(4He — 3He) in lines : λλ = 7 065 Å ; 4 713 ...
We have been developing a new nuclear laser spectroscopy method named "OROCHI" (Optical RI...
We have calculated ac polarizabilities of the 2 3 S and 2 1 S states of both He 4 and He 3 in the ra...
An experiment is proposed to excite the “forbidden” $1s2s\,^3S_1$ - $1s2s\,^1S_0$ magnetic dipole ($...
An experiment is proposed to excite the "forbidden" 1s2s(3) S-1 - 1s2s(1) S-0 magnetic dipole (M1) t...
A heterodyne spectroscopic scheme, using only one laser tuned to the atomic wavelength, is applied t...
We perform high precision measurements of an isotope shift between the two stable isotopes of helium...
A source of narrow bandwidth (<800 MHz) tunable laser radiation at 58.4 nm has been developed and is...
Abstract. Accurate Quantum-Electrodynamics (QED) tests of the simplest bound three body atomic syste...
The He4 fine structure and He3 hyperfine structure as well as the isotope shift between He4 and He3 ...
With a phase-modulated extreme ultraviolet pulsed laser sourer the frequency of the I S-1-2 P-1 tran...
An rms nuclear charge radius rc =1.9642 (11) fm for He3 is derived from measurements of the 2 S13 -2...
The goal of this project was to measure the hyperfine structure of $\overline{\text{p}}^3$He$^+$ usi...
The unusually large hyperfine structure splittings in the 23P state of the 3He isotope is measured...
Abstract. We have measured the absolute frequency of the 1557-nm doubly forbidden transition between...
The hyperfine structure of 3He and the isotope shift Δ T(4He — 3He) in lines : λλ = 7 065 Å ; 4 713 ...
We have been developing a new nuclear laser spectroscopy method named "OROCHI" (Optical RI...
We have calculated ac polarizabilities of the 2 3 S and 2 1 S states of both He 4 and He 3 in the ra...
An experiment is proposed to excite the “forbidden” $1s2s\,^3S_1$ - $1s2s\,^1S_0$ magnetic dipole ($...
An experiment is proposed to excite the "forbidden" 1s2s(3) S-1 - 1s2s(1) S-0 magnetic dipole (M1) t...