Introduction

The Sardinia Radio Telescope is a 64-meter single-dish radio telescope. It is located in the Pranu Sanguni area of San Basilio, Sardinia, Italy, about 40 km north of Cagliari.

Its state-of-the-art technology includes an active surface with 1008 panels, which allows observations at high frequencies (from 0.3 up to 115 GHz). There are three main focal points where reveivers can be placed: primary focus (currently hosting the L-P dual band receiver); Gregorian focus (K-band receiver), and Beam Wave Guide focus (C-band receiver). In total, the telescope can accomodate up to 20 receivers. A number of additional receivers are currently being planned and built.

The telescope can be operated in single-dish or VLBI mode for radio astronomy, geodynamical studies or space science. Its geographical location allows it to observe at declinations above -33 degrees.

A general description of the SRT, including technical commissioning information and first light results, can be found in the technical commissioning paper: Bolli et. al, Journal of Astronomical Instrumentation, Vol. 4, Nos. 3 & 4 (2015) 1550008.

Scientific tests and applications for the SRT are described in the following scientific validation paper: Prandoni et. al, A&A 608, A40 (2017).

Science done with SRT during its early-science run (2016) with the various hardware and software described below can be found here: Science with SRT.

In the following sections, we outline information that is useful for observing with the SRT in the current call for proposals (published September 14, 2018 with a deadline of October 9, 2018). We note that remote observing is not currently available for the Sardinia Radio Telescope; each proposing team will need to send at least one observer to the SRT to prepare the observing schedules and perform the observations on site.

Antenna

The Sardinia Radio Telescope (SRT) is a 64-meter Gregorian radio telescope with shaped optics, a quasi-parabolic main mirror and a quasi-elliptical subreflector.

The antenna’s main characheristics are:

Position

Pranu Sanguni, San Basilio, Sardinia

Geodetic Coordinates

Lat 39° 29’ 34.93742” N; Long 9° 14’ 42.5764” E (WGS84)

Optical configuration

Primary, Gregorian & Beam Waveguide (BWG)

Primary mirror diameter

64 m

Subreflector diameter

8 m

Focal positions

primary f/D = 0.33; Gregorian f/D = 2.34; Beam waveguide (BWG) f/D = 1.8

Azimuth range

–90 to 450 degrees

Elevation range

5 – 90 degrees

Slew rate

0.85 degrees/s in azimuth; 0.5 degrees/s in elevation

Frequency coverage

0.3 – 115 GHz

Primary surface accuracy

300 μm rms

Pointing accuracy (rms)

2 – 5”

We note that while the elevation limits range from 5 to 90 degrees, observations should be planned for an elevation between 6 and 82 degrees. Only in exceptional cases should the observations go below 6 degrees or above 82 degrees.

Active surface

The primary reflector, which is 64 m across, is made of 1008 aluminium panels (with an RMS ≤ 65 μm each) driven by 1116 electromechanical actuators. This active surface is designed to compensate for the gravitational deformations of the whole surface at different elevations.

The observer can choose among three configurations:

  • shaped in tracking (it adjusts according to the observed elevation position)

  • parabolic in fixed position (optimized for El=45°)

  • parabolic in tracking (it adjusts according to the observed elevation position)

The shaped configuration is used for receivers in the Gregorian and BWG foci, while the parabolic configurations are used for the primary focus systems.

Receivers

In the current call for proposals, the following (cryogenically-cooled) receivers are available in both single-dish and VLBI modes:

RF band (GHz)

Type

Tsys@90degEL(K)

Beamsize (arcmin)

Max gain (K/Jy)

connected backends

C-Low

single-feed

25

4.2

0.75

TP, DFB,DBBC,SARDARA,SKARAB

C-high 5.7-7.7

single-feed

32-37

2.7

0.66

TP,DFB,DBBC,ROACH1,SARDARA

K 18-26.5

7-feed

70

0.8

0.66

TP (MB),DFB,DBBC,SARDARA (MB),SKARAB(MB)

(MB) means that the Multi-Beam option is available for observations in K-band with the TP, XARCOS and SARDARA backends.

  • The single-feed, L-P band dual-frequency receiver was installed at the primary focus of the telescope, and therefore requires the parabolic configuration. It allows for simultaneous observations at L and P bands. The polarization type is linear but is also transformed to circular thanks to a hybrid converter.

  • A single-feed C-high band receiver is installed at the Beam Wave Guide (BWG) focus of the telescope. The polarization type is circular.

  • A multi-feed K-band receiver is installed at the (secondary) Gregorian focus. Both C and K band receivers require the shaped configuration. The polarization type is circular.

[ ] is an estimate (*) at the band’s central frequency (for C-band: 45 degrees EL @ 7.3 GHz) (**) at 22.3 GHz with opacity 0.1 and ground air temperature of 293K.

The FWHM beam size, as a function of the frequency f, can be approximated by the following rule: FWHM(arcmin)=19.7/ f(GHz)

SRT receiver changes are quick, allowing for an efficient frequency agility. The selected receiver is set in its focal position within at most a few minutes. However, the use of a Gregorian cover to limit RFI in L/P band observations does not currently allow a quick receiver change between L/P bands and other bands (C or K). Receiver changes between C and K-bands are not affected. An automatic system for the installation and removal of the Gregorian cover is currently under development and will permit smooth and efficient frequency changes.

Special considerations about the L/P dual-band receiver: the RFI levels need to be minimized. A Gregorian cover limits RFI at L and P bands; if desired, it needs to be requested in the observation proposal. However the availability of the Gregorian cover is not a priori guaranteed.

Special considerations about the multi-beam K-band receiver: we have measured the sensibility of each channel. Here are the details below:

Feed,Pol

RMS(mJy)

Ratio w/feed2,pol1

Feed0,Pol0

19

1.00

Feed0,Pol1

27

1.42

Feed1,Pol0

18

0.95

Feed1,Pol1

23

1.21

Feed2,Pol0

21

1.11

Feed2,Pol1

19

1.00

Feed3,Pol0

15

0.79

Feed3,Pol1

50

2.63

Feed4,Pol0

303

15.95

Feed4,Pol1

17

0.89

Feed5,Pol0

-9999

-526.26

Feed5,Pol1

39

2.05

Feed6,Pol0

17

0.89

Feed6,Pol1

138

7.26

The second column indicates the RMS of the calibrator map (using 3c147). The third column indicates the sensibility ratio of each channel with respect to the Right channel of the second feed (which is stable). Channel 5,Pol0 (Left) is not usable.

Future receivers: the SRT was designed to accomodate up to 20 receivers. A 7-feed S-band receiver (3 – 4.5 GHz) is undergoing testing and designed to be placed at the primary focus of the telescope (requiring the parabolic configuration). The receiver had its first light in November 2016 (for its central feed). The full commissioning of this receiver is expected to end in 2021. Additionally, a number of high-energy receivers are being planned for the SRT. This includes a multi-feed W receiver and a cryocooled, 19-pixel dual-polarized Q-band system at the secondary/Gregorian focus.

More details about current and future receivers at Italian radio telescopes (SRT, Medicina and Noto) are included in this review document: receivers

Backends

The frontend (receiver) outputs are connected to the backend instruments either by coaxial cables or optical fibers, depending on whether the backend is located in the main building or below the dish. The following backends, designed for specific scientific activities, are available at the site:

These backends are available for the current call for proposals:

(+) C-low and C-high receivers (*) For the 1500 MHz SARDARA configuration, the actual available RF bandwidth is 1200 MHz with the C-band and K-band receivers. Similarly, for the 420 MHz SARDARA configuration, the effective RF bandwidth is 300 MHz with the K-band and C-band receivers. Instead, the L-band receiver only has 500 MHz of RF bandwidth; when the SARDARA 420 MHz configuration is needed, the actual available RF bandwidth for SARDARA is 100 MHz (when selecting the XXL3 or XXC3 filters) or 90 MHz (when selecting the XXL5 or XXC5 filters).

Total Power

The Total Power backend is a single-band, seven-beam backend for continuum observations. Located just below the dish, this backend is formed by 14 voltage-to-frequency converters that digitize the incoming RF signals. Different IF inputs can be selected from three focal points. Different bandwidths (maximum bandwidth: 0.1 - 2.1 GHz) and attenuation levels can be selected.

This backend consists of 14 sections. Each section processes a single IF channel with a single polarization, as input. The signal is detected by a broadband square-law detector and then digitized by an A/D converter. The nominal IF band is 2 GHz (0.1-2.1 GHz). On-board filters can restrict the band to 250, 680, or 1200 MHz. The same boards also perform the focus selection for the SARDARA backend. Here are the possible configurations of the Total Power backend for different receivers:

Receiver

Sections

Filters (MHz)

Sampling time (ms)

K-band

14

250,680,1200,2000

1 – 1000

C-band

2

250,680,1200,2000

1 – 1000

More information about XARCOS configurations can be found here: Melis et al., OAC Internal report N. 52.

It is worth noting that, given a particular configuration (e.g. XK00), the sections are obtained simultaneously. For each section, the bandwidth and starting frequency can then be set. For more information about this procedure, see XARCOS.

Notes:

  • XARCOS has been tested in circular polarization. Linear polarization observations are also admitted but in shared-risk mode. The full-Stokes configuration is therefore in shared-risk mode. Please contact the antenna staff.

  • At C-band, standing waves have been identified that affect observations for Tcontinuum/Tsys > 0.05 (value to be confirmed).

Digital Base Band Converter (DBBC)

This digital platform is based on a flexible architecture composed of four ADC boards, with 1 GHz of bandwidth each and four Xilinx FPGA boards for data processing. The platform is designed mainly for VLBI experiments; however, a wideband spectrometer has been developed for other purposes.

Digital Filter Bank mark 3 (DFB3)

This is an FX correlator developed by the Australia Telescope National Facility (ATNF) that performs full-Stokes observations. It allows for four inputs, each with a 1024 MHz maximum bandwidth and 8-bit sampling for a high dynamic range. The DFB3 is suitable for precise pulsar timing and searching. It allows for up to 8192 spectral channels in order to counter the effects of interstellar dispersion.

The available configurations for pulsar observations are the following:

Obs type

Nbins

BW(MHz)

Nfreq

folding

1024

1024

2048

folding

1024

1024

1024

folding

1024

1024

512

folding

1024

512

2048

folding

1024

512

1024

folding

1024

512

512

folding

512

1024

1024

folding

512

512

2048

folding

512

512

1024

folding

512

512

512

folding

512

256

512

folding

512

128

2048

folding

256

256

2048

folding

256

64

2048

folding

256

64

1024(*)

search

1024

1024

search

1024

512

search

512

1024

search

512

512

search

512

128

(*) This configuration does not work for pulsars with periods < 1.6 ms.

  • Choosing the best folding configuration depends in part on the period of the pulsar. One can find the best folding configuration for a range of folding periods here.

  • These search mode configurations have been succesfully tested for the acquisition of total intensity data (npol=1) for sampling times down to 100 microseconds. Full stokes data can be obtained only with slow sampling times (>= 512 microsec for 1024 channels over 512 MHz of bandwidth and >=256 microsec for 512 channels).

Further details about the DFB can be found in the ATNF DFB manual.

At the SRT, DFB observations are piloted using the SEADAS software.

SARDARA

The use of this backend is admitted in shared-risk mode. Users are required to contact the antenna staff prior to submission, in order to assess the availability of software/hardware services for their specific needs.

The SARDARA backend is composed of seven fully-reconfigurable ROACH-2 boards that allow it to perform wide-band spectro-polarimetric observations. The many observing modes covered by SARDARA include: continuum, spectroscopy and spectro-polarimetry. In the future, it will also be able to perform high-time resolution for pulsars and fast transients (not currently available). Its sampling time can be set from 5ms to 1 s. It is the backend of choice for On-The-Fly (OTF) spectro-polarimetric observations. Available configurations consist of:

in C-low, C-high and K bands:

  • 420 MHz bandwith with 1024 or 16384 channels

  • 1500 MHz bandwidth with 1024 or 16384 channels

SARDARA’s spectral resolution and sensitivity are defined by its full 1500 MHz bandwidth. However only 1200 MHz of the full 1500 MHz bandwidth is usable, since the 1200 MHz filter of the Total Power backend’s Focus Selector is being used as input to SARDARA.

More detailed information on the SARDARA backend can be found here: SARDARA.

SKARAB

The SKARAB backend is composed of seven fully-reconfigurable SKARAB boards that allow it to perform wide-band spectro-polarimetric observations. The many observing modes covered by SKARAB include: continuum, spectroscopy and spectro-polarimetry. In the future, it will also be able to perform high-time resolution for pulsars and fast transients (not currently available). Its sampling time can be set from 5ms to 1 s. It is the backend of choice for On-The-Fly (OTF) spectro-polarimetric observations.

The available bandwidhths are:

  • 16, 20, 23, 32, 40, 46.875, 64, 80, 93.75, 128, 160, 187.5, 1400 MHz

Each band can be divided in 65536 frequency bins or 32768 for full Stokes configurations. The 1400 MHz bandwidth can have also 2048 frequency bins in full Stokes mode

Calibration

Pointing model

This calibration procedure was used to calculate the pointing errors in ideal conditions, i.e. at night without sunlight. Actual conditions will most likely require new pointing measurements in order to take into account possible errors due to environmental factors. Pointing measurements before starting an observing session are highly recommended and can be included in the observation schedule.

In the table below, we report the calculated rms values in ideal conditions:

Parameter

Value (deg) for L-band

Value (deg) for C-band

Value (deg) for K-band

Az-mean

+0.000440

+0.000850

Az-rms

+0.001944(*)

+0.000790

+0.000870

El-mean

-0.001660

-0.001280

El-rms

+0.001944(*)

+0.000910

+0.001200

(*) values for L-band from Bolli et al (2015)

Focus curve calibration

The focus curve is applied in real time. However, it is highly recommended that for C and K-band observations, the observer perform a focus calibration before starting an observing session.

Gain curve calibration

From the measured gain curves (Gain vs. Elevation), one fits a 2-degree polynomial with the parameters C0, C1 and C2:

gain (K/Jy) = C2 El^2 + C1 El + C0

Parameter

Value (L-band)

Value (C-band)

Value (K-band)

C0

0.5061

0.545439

0.364897

C1

0.002390

0.00525597

0.00624137

C2

-0.000021

-4.55697e-5

-4.60020e-5

L-band: from Orlati et al.

C-band: valid from 2018.

K-band: from Prandoni et al. (2017). The DPFU is 0.60 K/Jy.

Beam shape

In the following tables, the second lobe and third lobe percentages correspond to the contribution of the counts in that lobe as compared to the central beam.

  • C-band

Elevation range (deg)

Second lobe (%)

Third lobe (%)

15-25

1.7

0.65

25-35

1.7

0.42

35-50

1.4

0.41

50-65

1.0

0.41

65-75

1.5

0.43

75-85

2.0

0.40

  • K-band

Elevation range (deg)

Second lobe (%)

Third lobe (%)

20-40

11

0.6

40-60

4.9

0.5

60-80

3.4

0.5

List of calibrators

Here is a list of useful calibrators for various types of calibration:

Flux

Polarization angle

Instrumental polarization

3C286

3C286

3C84

3C147

3C138

NGC7027

3C48

3C295

For pointing calibration, see below in “Useful links”.

Derotator alignment

The derotator has been aligned within 1-2 arcseconds.

Data quicklook

Information about a data quicklook will be inserted here very soon.

Data conversion

Conversion of data acquired in spectroscopic mode

Conversion to the GILDAS data format is provided for data acquired in Nodding and Position Switching modes with the SARDARA and XARCOS backends, including spectra containing the signal from the noise diode (when used).

User guide and observing modes

Instructions for observing at the SRT with different modalities (receivers, backends, modes) are provided here: instructions

A complete manual about the Italian radio antennas is found here: DISCOS.

Observing tools

Source visibilites can be determined using the CASTIA online tool.

The online Exposure Time Calculator (ETC) can be found here: ETC tool.