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Optical frequency standards for time and length applications
FL Hong - Measurement Science and Technology, 2016 - iopscience.iop.org
The last decade has witnessed tremendous progress in research on optical frequency
metrology. Optical frequency standards using optical lattice and single-ion trap technologies …
metrology. Optical frequency standards using optical lattice and single-ion trap technologies …
Photonic chip for laser stabilization to an atomic vapor with 10−11 instability
Devices based on spectroscopy of atomic vapors can measure physical quantities such as
magnetic fields, RF electric fields, time and length, and rotation and have applications in a …
magnetic fields, RF electric fields, time and length, and rotation and have applications in a …
An ultra-stable laser based on molecular iodine with a short-term instability of 3.3× 10− 15 for space based gravity missions
Z Zhang, Z Wang, H Liu, W Yuan, W You… - … and Quantum Gravity, 2023 - iopscience.iop.org
Many space based gravity missions require frequency stabilized lasers with stringent
requirements. Toward those requirements, we develop a compact frequency-stabilized laser …
requirements. Toward those requirements, we develop a compact frequency-stabilized laser …
Frequency references based on molecular iodine for the study of Yb atoms using the 1S0 – 3P1 intercombination transition at 556 nm
Y Tanabe, Y Sakamoto, T Kohno, D Akamatsu… - Optics …, 2022 - opg.optica.org
We used precision spectroscopy to analyze the R (53) 24-1, P (49) 24-1, and R (95) 25-1
lines of molecular iodine (^ 127I_2) to establish optical frequency references for the laser …
lines of molecular iodine (^ 127I_2) to establish optical frequency references for the laser …
Iodine-frequency-stabilized laser diode and displacement-measuring interferometer based on sinusoidal phase modulation
We propose a sinusoidal phase modulation method to achieve both the frequency
stabilization of an external-cavity laser diode (ECLD) to an 127 I 2 saturated absorption …
stabilization of an external-cavity laser diode (ECLD) to an 127 I 2 saturated absorption …
Iodine-stabilized laser at telecom wavelength using dual-pitch periodically poled lithium niobate waveguide
K Ikeda, S Okubo, M Wada, K Kashiwagi, K Yoshii… - Optics …, 2020 - opg.optica.org
We demonstrate the third harmonic generation of a 1542-nm laser using a dual-pitch
periodically poled lithium niobate waveguide with a conversion efficiency of 66%/W^ 2. The …
periodically poled lithium niobate waveguide with a conversion efficiency of 66%/W^ 2. The …
Absolute frequency measurements and hyperfine structures of the molecular iodine transitions at 578 nm
We report absolute frequency measurements of 81 hyperfine components of the
rovibrational transitions of molecular iodine at 578 nm using the second harmonic …
rovibrational transitions of molecular iodine at 578 nm using the second harmonic …
Suppression of residual amplitude modulation appeared in commercial electro-optic modulator to improve iodine-frequency-stabilized laser diode using frequency …
Background: This paper shows how to suppress residual amplitude modulation (RAM)
appeared in a commercial electro-optic modulator (EOM) to improve an iodine-frequency …
appeared in a commercial electro-optic modulator (EOM) to improve an iodine-frequency …
Evaluation of laser frequency offset locking using an electrical delay line
Y Hisai, K Ikeda, H Sakagami, T Horikiri… - Applied Optics, 2018 - opg.optica.org
Frequency offset locking between two Nd: YAG lasers is performed using frequency locking
with an electrical delay line. The relative frequency instability of the offset locking is …
with an electrical delay line. The relative frequency instability of the offset locking is …
Absolute frequency measurement of molecular iodine hyperfine transitions at 554 nm and its application to stabilize a 369 nm laser for Y b+ ions cooling
We investigate 13 hyperfine structures of transition lines of 127 I 2 near 554 nm, namely, the
R (50) 22-0, P (46) 22-0, P (121) 24-0, P (69) 25-1, R (146) 25-0, R (147) 28-1, P (160) 26-0 …
R (50) 22-0, P (46) 22-0, P (121) 24-0, P (69) 25-1, R (146) 25-0, R (147) 28-1, P (160) 26-0 …