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 |