The hyperfine spectrum of the iodine R(115)20-1 line, at 570 nm, was obtained by conventional saturated absorption spectroscopy. The differences of nuclear electric-quadrupole (DELTAe Qq) and spin-rotation (DELTAC) constants between the B and X states were determined by a least-square fit to the experimental data. This line may provide a good frequency reference in coincidence with the S-1(0)-P-1(1) resonant transition of magnesium, at 285 nm, when this one is investigated with frequency doubled lasers.16215516
Absolute wave numbers with a typical uncertainty of 1 MHz (95% confidence) were measured for 102 hyp...
Abstract—With the aid of two iodine spectrometers, we report for the first time the measurement of t...
The hyperfine structures of six metastable levels arising from the 3d24s and 3d3 configurations in i...
The hyperfine structure splittings of the P(10)14-1, R(15)14-1, and R(99)15-1 transitions at 585 nm,...
Frequency-stabilized lasers are of considerable interest not only for the implementation of time and...
In a double saturation spectroscopy experiment, using the radiation from one single frequency cw las...
Several groups of stronger transition hyperfine spectra with third derivative technique based on sat...
[[abstract]]Internal-mirror 543 nm HeNe lasers are frequency-stabilized on the iodine hyperfine tran...
[[abstract]]We determine the linewidth of the hyperfine structure a(10) component of R(56) 32-0 tran...
International audienceThe hyperfine structure of higher rovibrational levels in the iodine B state h...
We report on the hyperfine-structure splitting of the 716 nm R 90 3–10 molecular iodine transition. ...
We report on the hyperfine-structure splitting of the 716 nm R(90)3-10 molecular iodine transition.W...
Doppler-free high-resolution spectroscopy is applied to molecular iodine at 532 nm by Nd:YAG lasers....
We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) ...
A high precision dense grid of reference lines in the hyperfine structure of the B–X system of molec...
Absolute wave numbers with a typical uncertainty of 1 MHz (95% confidence) were measured for 102 hyp...
Abstract—With the aid of two iodine spectrometers, we report for the first time the measurement of t...
The hyperfine structures of six metastable levels arising from the 3d24s and 3d3 configurations in i...
The hyperfine structure splittings of the P(10)14-1, R(15)14-1, and R(99)15-1 transitions at 585 nm,...
Frequency-stabilized lasers are of considerable interest not only for the implementation of time and...
In a double saturation spectroscopy experiment, using the radiation from one single frequency cw las...
Several groups of stronger transition hyperfine spectra with third derivative technique based on sat...
[[abstract]]Internal-mirror 543 nm HeNe lasers are frequency-stabilized on the iodine hyperfine tran...
[[abstract]]We determine the linewidth of the hyperfine structure a(10) component of R(56) 32-0 tran...
International audienceThe hyperfine structure of higher rovibrational levels in the iodine B state h...
We report on the hyperfine-structure splitting of the 716 nm R 90 3–10 molecular iodine transition. ...
We report on the hyperfine-structure splitting of the 716 nm R(90)3-10 molecular iodine transition.W...
Doppler-free high-resolution spectroscopy is applied to molecular iodine at 532 nm by Nd:YAG lasers....
We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) ...
A high precision dense grid of reference lines in the hyperfine structure of the B–X system of molec...
Absolute wave numbers with a typical uncertainty of 1 MHz (95% confidence) were measured for 102 hyp...
Abstract—With the aid of two iodine spectrometers, we report for the first time the measurement of t...
The hyperfine structures of six metastable levels arising from the 3d24s and 3d3 configurations in i...