Phase-shifting interferometry with equal phase steps by use of a frequency-tunable diode laser and a Fabry–Perot cavity

2005 ◽  
Vol 44 (26) ◽  
pp. 5403 ◽  
Author(s):  
Youichi Bitou ◽  
Hajime Inaba ◽  
Feng-Lei Hong ◽  
Toshiyuki Takatsuji ◽  
Atsushi Onae
Keyword(s):  
Diode Laser ◽  
Phase Shifting ◽  
Tunable Diode Laser ◽  
Phase Shifting Interferometry ◽  
Fabry Perot ◽  
Frequency Tunable

scholarly journals High speed phase shifting interferometry using injection locking of the laser frequency to the resonant modes of a confocal Fabry-Perot cavity

2009 ◽  
Vol 17 (3) ◽  
pp. 1442 ◽  
Author(s):  
Chu-Shik Kang ◽  
Jong-Ahn Kim ◽  
Tae Bong Eom ◽  
Roma Jang ◽  
Hae Yong Park ◽  
...  
Keyword(s):  
High Speed ◽  
Laser Frequency ◽  
Injection Locking ◽  
Phase Shifting ◽  
Phase Shifting Interferometry ◽  
Resonant Modes ◽  
Fabry Perot

Narrow-Line and Frequency Tunable Diode Laser System for S–D Transition of Ca+Ions

2008 ◽  
Vol 47 (8) ◽  
pp. 6327-6332 ◽  
Author(s):  
Ying Li ◽  
Shigeo Nagano ◽  
Kensuke Matsubara ◽  
Hiroyuki Ito ◽  
Masatoshi Kajita ◽  
...  
Keyword(s):  
Diode Laser ◽  
Laser System ◽  
Tunable Diode Laser ◽  
Narrow Line ◽  
Ca Ions ◽  
Frequency Tunable

Fabry-Pérot Interferometer Using Tunable Diode Laser

2008 ◽  
Vol 28 (7) ◽  
pp. 1296-1300
Author(s):  
马骥驰 Ma Jichi ◽  
李岩 Li Yan ◽  
孙文科 Sun Wenke ◽  
许婕 Xu Jie
Keyword(s):  
Diode Laser ◽  
Tunable Diode Laser ◽  
Fabry Perot

scholarly journals Performance of a stabilized Fabry-Perot solar analyzer

1988 ◽  
Vol 123 ◽  
pp. 475-479
Author(s):  
D. M. Rust ◽  
T. Appourchaux ◽  
F. Hill
Keyword(s):  
Lithium Niobate ◽  
Diode Laser ◽  
Tunable Diode Laser ◽  
Stabilization System ◽  
Sacramento Peak ◽  
Instrumental Noise ◽  
Peak Observatory ◽  
Electro Optic ◽  
Fabry Perot ◽  
Sacramento Peak Observatory

A unique solar lineshift analyzer described by Rust, Burton and Leistner (1986) has been used at the Sacramento Peak Observatory to study solar oscillations. Operation of this “Stablized Solar Analyzer” (SSA) depends on the electro-optic effect in crystalline lithium niobate, the substrate of the solid Fabry-Perot etalon. Voltage on the etalon shifts the passband by ∼ 4.5 × 10−4 Å/V. The etalon has a passband of 0.175 Å at 6102.7 Å. The stabilization system uses a tunable diode laser to relate the Fabry-Perot passband to the D2 line of atomic Cs 133, at 8521.46 Å. This system reduced instrumental noise to less than Δλ/λ = 10−9 over a six-hour interval.

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