Ondřejov Echelle Spectrograph (OES) is a fibre-fed high-resolution spectrograph. The spectrograph is installed in a temperature-stabilised room. The light is directed via optical fiber
(core diameter 0.1 mm) from the primary focus to the coudé room where it is reflected to an echelle grating (made by Richardson Grating Laboratories) with the size of 408×165×74 mm
with 55 gr/mm and a blaze angle θ=69°. The optical mirror reflects the light further to a equilateral prism (made by TOPTEC Turnov, CZ, glass Schott LF5) with apical angle of 55°,
which separates the orders that are then brought to a focus on the detector. The detector is a nitrogen-cooled EEV 2048×2048 pixel CCD (Versarray 2048B, EEV 42-10-1-36B)
with a pixel size of 13.5 μm and a dynamical range of 65535 ADUs. The read-out noise is of about 3.5 e− rms, and a dark current of 1 e−/p/hr. In addition, the spectrograph is fed by
a calibration lamp. Also, the iodine cell is mounted on the telescope-spectrograph interface, providing a secondary spectral calibration source.
Dimensions of the base: 144x118 mm (118 mm is the length of the diffraction edge).
Height of the prism from the base: 140 mm.
Diffraction angle: 54.5°.
Density: 3.25 g/mm3.
Made by Walter, Faculty of Mathematics and Physics, Charles Univ., Prague, CZ.
Canon EF lens 200, F1.8L Ultrasonic.
Focal ratio: f/1.8.
Diameter of input beam: 111.1 mm.
field of view: 12°.
Dewar and CCD chip
Detector: Versarray 2048B.
Chip: EEV 42-40-1-368.
Dimensions: 2048x2048 pixels.
Size of pixel: 13.5 x 13.5 μm.
Reading noise: 10.
Cooling: liquid nitrogen.
Operational temperature: −110°C.
Made by Roper Scientific.
Wavelength coverage and performance
The details about the OES performance can be found in Kabáth et al., 2020, PASP, 132, 1009. The wavelength coverage of OES is from near UV (3753 Å) up to near IR (9195 Å). The resolving power is R=51600
at 5000 Å (R∼40000 in Hα) and spectral sampling is 2.4 Å/mm. The spectral range is covered by 56 usable orders. The number of spectral orders range from 92 to 36. The individual spectral order covers ∼70 Å
in the near UV region and ∼145 Å in near IR regions. In blue, spectral orders overlap, thus, it is possible to merge them. The overlapping interval is ∼20 Å in near UV. However, the overlapping intervals
gets shorter towards red and the last (short) overlapping intervals are between spectral orders covering 5782-5879 and 5879-5977 (the overlap is less than 1 Å). Between the orders covering 5879-5977
and 5978-6079, there is already a gap (∼1 Å). The gap is gradually increasing and around H the gap between consecutive orders is ∼13 Å and even ∼63 Å around 8800 Å.
The appropriate exposure time can be roughly estimated using Fig. XX. It is seen that for the signal-to-noise ratio (SNR) of 20, an 1-hour exposure time is needed for a 10-mag star.
This figure shows the situation before the upgrade with the optical fiber. Currently, the performance is of about factor 3-5 better. We can get SNR~40 in the Hα region with 3600-s exposure
for 12.5-mag star that is close to zenith. However, the particular SNR depends not only on the zenith distance but mainly on the observing conditions. The limiting precision regarding the
radial velocities is in the order of hundreds m/s for faint stars. By using the iodine cell, we can get precision of about a few tens of m/s. For more details see
Kabáth et al., 2020, PASP, 132, 1009
Single Order Spectrograph
Single order coudé spectrograph works in the first and second spectral orders. Wavelength coverage of the second order is 4000-5100 Å (near UV and blue) with order length of 233 Å.
Wavelength coverage of the first order is 5100-8900 Å (red and near IR) with order length of 470 Å. Resolving power is 12000 in Hα spectral region. The detector is an PyLoN 2048x512BX
pixel with nitrogen-cooled CCD (E2V 42-10 BX) with a pixel size of 13.5 μm, cooled by liquid nitrogen to −115°C and a dynamical range of 600.2 ADUs.
The main advantage is that it depicts wide interval of wavelengths (475 Å in the Hα spectral region) with uniform S/N.
Separating glass plate - the glass plate is installed in the tube connecting the coude room to the telescope. This tube is corresponding to the hour axis of the telescope. The light beam is going through
this tube to the slit head. The glass plate divides space in coudé room and the dome and thus it prevent from the draught.
Turning prism + eyepiece - the astronomer should be able to look to the field of view of the telescope (although it is not used very often). Then one can put a prism to the optical path and redirect
the light beam to the ocular with thread cross.
Dichroic mirrors - there are 4 dichroic mirror for the optimal separation of spectral orders: red, infrared, blue, and aluminium. However, the profit is not very important and thus,
mainly due to auto-guiding (see individual chapter in link below) we use aluminium mirror.
Slit width: 0.2 mm (0.6 arcsec).
Exposuremeter: just behind the slit, semitranslucent mirror, about 5% of the light to the exposuremeter.
Spectral filters - for the separation of spectral orders.
Collimator: focal ratio f/32, out of axis.
Grating - works in the first and second spectral orders.
Schmidt camera (correction plate + spherical mirror)
Camera: Schmidt camera, focal length 700mm.
Flat field lamp: Hollow cathode
Comparison light: ThAr lamp, 15 mA
Slitwidth: 0.2 mm (0.6 arcsec)
Spectral filters: to separate spectral orders
The photometric camera is installed in the primary focus. The focal length in primary focus is 9 m (focal ratio f/4.5) but the photometric camera changes the effective focal length in primary focus
to 7 m and focal ratio to f/3.5. The change between fibers (i.e. spectrographs) and photometric camera can be done within 1 minute.