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A laser-lock concept to reach cm-1s-precision in Doppler experiments with Fabry-Perot wavelength calibrators

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dc.contributor.author Reiners, A
dc.contributor.author Banyal, R. K
dc.contributor.author Ulbrich, R. G
dc.date.accessioned 2020-11-17T14:09:11Z
dc.date.available 2020-11-17T14:09:11Z
dc.date.issued 2014-09
dc.identifier.citation Astronomy & Astrophysics, Vol. 569, A77 en_US
dc.identifier.issn 0004-6361
dc.identifier.uri http://prints.iiap.res.in/handle/2248/7119
dc.description Open Access © ESO http://dx.doi.org/10.1051/0004-6361/201424099 en_US
dc.description.abstract State-of-the-art Doppler experiments require wavelength calibration with precision at the cm s − 1 level. A low-finesse Fabry-Pérot interferometer (FPI) can provide a wavelength comb with a very large bandwidth as required for astronomical experiments, but unavoidable spectral drifts are di ffi cult to control. Instead of activ ely controlling the FPI cavity, we propose to passively stabilize the interferometer and track the time-dependent cavity length drift externally using the 87 Rb D 2 atomic line. A dual-finesse cavity allows drift tracking during observation. In the low-finesse spectral range, the cavity provides a comb transmission spectrum tailored to the astronomical spectrograph. The drift of the cavity length is monitored in the high-finesse range relative to an external standard: a single narrow transmission peak is locked to an external cavity diode laser and compar ed to an atomic frequency from a Doppler-free transition. Following standard locking schemes, tracking at sub-mm s − 1 precision can be achieved. This is several orders of magnitude better than currently planned high-precision Doppler experiments, and it allows freedom for relaxed designs including the use of a single-finesse interferometer under certain conditions. All components for the proposed se tup are readily availa ble, rendering this approach particularly interesting for upcoming Doppler experiments. We also show that the large number of interference modes used in an astronomical FPI allows us to unambiguously identify the interference mode of each FPI transmission peak defining its absolute wavelength solution. The accuracy reached in each resonance with the laser concept is then defined by the cavity length that is determined from the one locked peak and by the group velocity dispersion. The latter can vary by several 100 m s − 1 over the relevant frequency range and severely limits the accuracy of individual peak locations, although their interference modes are known. A potential way to determine the absolute peak positions is to externally measure the frequency of each individual peak with a laser frequency comb (LFC). Thus, the concept of laser-locked FPIs may be useful for applying the absolute accuracy of an LFC to astronomical spectrographs without the need for an LFC at the observatory. en_US
dc.language.iso en en_US
dc.publisher EDP Sciences en_US
dc.subject Techniques: radial velocities en_US
dc.subject Instrumentation: spectrographs en_US
dc.subject Planets and satellites: detection en_US
dc.subject Techniques: spectroscopic en_US
dc.title A laser-lock concept to reach cm-1s-precision in Doppler experiments with Fabry-Perot wavelength calibrators en_US
dc.type Article en_US


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