We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) hyperfine transitions, and the P(144) 23-0 a(1) hyperfine transition at 560 nm with a frequency comb. The light source is based on an all-solid-state frequency quadrupled laser system. A frequency stability of 4 x 10(-12) is achieved over a 100 s integration time when the light source is frequency stabilized to the R(34) 20-0 a(1) line. The pressure and power broadening dependences of the R(34) 20-0 a(10) line are also investigated. (C) 2009 Optical Society of Americ
I demonstrate a technique for frequency stabilization and modulation transfer spectroscopy using a l...
We report on the hyperfine-structure splitting of the 716 nm R 90 3–10 molecular iodine transition. ...
The hyperfine structure splittings of the P(10)14-1, R(15)14-1, and R(99)15-1 transitions at 585 nm,...
We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) ...
We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) ...
We report absolute frequencymeasurements of the a1, a10, and a15 hyperfine components of molecular i...
International audienceThe absolute frequencies of the hyperfine components of the R(26) 62-0 transit...
The frequency of several hyperfine components of 127I2 has been measured at 514.67 nm using an optic...
Frequency-stabilized lasers are of considerable interest not only for the implementation of time and...
Frequency-stabilized lasers are of considerable interest not only for the implementation of time and...
[[abstract]]We report, for the first time, the observation of the iodine hyperfine transitions at 53...
We report on the hyperfine-structure splitting of the 716 nm R(90)3-10 molecular iodine transition.W...
In this paper, a preliminary result for an iodine frequency stabilized tunable diode laser at 633 nm...
Several groups of stronger transition hyperfine spectra with third derivative technique based on sat...
I demonstrate a technique for frequency stabilization and modulation transfer spectroscopy using a l...
I demonstrate a technique for frequency stabilization and modulation transfer spectroscopy using a l...
We report on the hyperfine-structure splitting of the 716 nm R 90 3–10 molecular iodine transition. ...
The hyperfine structure splittings of the P(10)14-1, R(15)14-1, and R(99)15-1 transitions at 585 nm,...
We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) ...
We report absolute frequency measurements of the molecular iodine R(34) 20-0 a(1), a(10), and a(15) ...
We report absolute frequencymeasurements of the a1, a10, and a15 hyperfine components of molecular i...
International audienceThe absolute frequencies of the hyperfine components of the R(26) 62-0 transit...
The frequency of several hyperfine components of 127I2 has been measured at 514.67 nm using an optic...
Frequency-stabilized lasers are of considerable interest not only for the implementation of time and...
Frequency-stabilized lasers are of considerable interest not only for the implementation of time and...
[[abstract]]We report, for the first time, the observation of the iodine hyperfine transitions at 53...
We report on the hyperfine-structure splitting of the 716 nm R(90)3-10 molecular iodine transition.W...
In this paper, a preliminary result for an iodine frequency stabilized tunable diode laser at 633 nm...
Several groups of stronger transition hyperfine spectra with third derivative technique based on sat...
I demonstrate a technique for frequency stabilization and modulation transfer spectroscopy using a l...
I demonstrate a technique for frequency stabilization and modulation transfer spectroscopy using a l...
We report on the hyperfine-structure splitting of the 716 nm R 90 3–10 molecular iodine transition. ...
The hyperfine structure splittings of the P(10)14-1, R(15)14-1, and R(99)15-1 transitions at 585 nm,...