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Advances in Astronomy
Volume 2010 (2010), Article ID 701534, 8 pages
http://dx.doi.org/10.1155/2010/701534
Research Article

Recent GRBs Observed with the 1.23 m CAHA Telescope and the Status of Its Upgrade

1Instituto de Astrofísica de Andalucía (IAA-CSIC), 18008 Granada, Spain
2Imaging Processing Laboratory (IPL), University of Valencia, 46010 Valencia, Spain
3INAF/Brera Astronomical Observatory, Via Bianchi 46, Lecco, 23807 Merate, Italy
4Universidad de Málaga, 29071 Málaga, Spain
5LAEX-CAB (INTA-CSIC), LAEFF, P.O. Box 78, Villanueva de la Cañada, 28691 Madrid, Spain
6Institute of Planetary Research, DLR, 12489 Berlin, Germany

Received 2 July 2009; Revised 22 October 2009; Accepted 4 January 2010

Academic Editor: Taro Kotani

Copyright © 2010 Javier Gorosabel et al. This is an open access article distributed under the Creative Commons Attribution License, which permits unrestricted use, distribution, and reproduction in any medium, provided the original work is properly cited.

Abstract

We report on optical observations of Gamma-Ray Bursts (GRBs) followed up by our collaboration with the 1.23 m telescope located at the Calar Alto observatory. The 1.23 m telescope is an old facility, currently undergoing upgrades to enable fully autonomous response to GRB alerts. We discuss the current status of the control system upgrade of the 1.23 m telescope. The upgrade is being done by our group based on the Remote Telescope System, 2nd Version (RTS2), which controls the available instruments and interacts with the EPICS database of Calar Alto. (Our group is called ARAE (Robotic Astronomy & High-Energy Astrophysics) and is based on members of IAA (Instituto de Astrofísica de Andalucía). Currently the ARAE group is responsible to develop the BOOTES network of robotic telescopes (Jelínek et al. 2009).) Currently the telescope can run fully autonomously or under observer supervision using RTS2. The fast reaction response mode for GRB reaction (typically with response times below 3 minutes from the GRB onset) still needs some development and testing. The telescope is usually operated in legacy interactive mode, with periods of supervised autonomous runs under RTS2. We show the preliminary results of several GRBs followed up with observer intervention during the testing phase of the 1.23 m control software upgrade.

1. Introduction

The 1.23 m telescope is at the German-Spanish observatory of Calar Alto (CAHA) in the province of Almeria, Southeast of Spain. The observatory’s altitude (2168 m), mean seeing (0.; see [1]), and a large fraction (65%) of clear nights make Calar Alto one of the most competitive observatories in Europe in the optical and near-infrared bands. The observatory harbours five telescopes, but only three are currently operative: the 1.23 m, 2.2 m, and 3.5 m telescopes. Figure 1 shows a view of the Calar Alto observatory. The arrow indicates the position of the 1.23 m telescope.

701534.fig.001
Figure 1: View of the Calar Alto observatory. The picture shows the five telescopes of Calar Alto and the staff building (lower-right corner). The arrow shows the localization of the 1.23 m telescope.

The 1.23 m telescope is a Ritchey-Crétien telescope built in 1975 by Carl Zeiss. The focal ratio of the telescope is f/8 with a total field of view of and a focal plane scale of ~/mm. The aberrationfree field of view is limited to ~. The German mount of the telescope is driven by a mechanical and hydraulic system renovated in 2008 by the observatory staff. Figure 2 shows a drawing and a picture of the of 1.23 m CAHA telescope.

fig2
Figure 2: The 1.23 m telescope of Calar Alto. (a) The drawing shows the mechanics and the hydraulic system of the 1.23 m telescope of Calar Alto. One of the mechanical peculiarities of the telescope is the presence of a steel sphere (indicated by a red arrow) which, by means of a high-pressure hydraulic system, supports all the weight of the telescope. (b) Picture of the 1.23 m inside the dome. As seen, the instrumentation is always located in the Cassegrain focus. Note the German mount of the telescope.

Two instruments are available for the 1.23 m, the MAGIC near-infrared camera and the 2 k2 k SITE#2b optical CCD. Currently, most of the time () only the optical CCD is used, as the MAGIC camera, one of the first near-infrared cameras ever built, was superseded by modern instruments on larger telescopes. In addition to the offering of the MAGIC near-infrared camera, CAHA is considering the possibility of installing visitor instruments on the 1.23 m telescope.

The field of view of the optical CCD camera is with a pixel size of 24 m. That translates to a pixel scale of 0. per pixel. The readout time of the whole chip in 11 binning mode is very long, close to 4 minutes. For this reason rapid followup observations of transients like Gamma-Ray Bursts (GRBs) are usually carried out trimming the window and/or binning the CCD by 22 pixels. Using this technique, the readout time is usually kept below one minute.

The CCD chip is refrigerated using liquid nitrogen, which makes dark current negligible, fewer than 2 electrons per hour. The readout noise is also low, about 7 electrons. However, the chip has several bad columns which RTS2 (see next section and [2]) must avoid at the time of a GRB alert (see the vertical lines on the image of GRB 090628, Figure 6). The optical camera is equipped with a filter wheel. A Wollaston prism can be also mounted in the filter wheel, which makes the 1.23 m telescope suitable also for polarimetric studies.

2. Upgrading the 1.23 m Control Software with RTS2

A call for proposals was issued by CAHA in 2008 for the use of the 1.23 m telescope over 4 years. Six teams obtained observing time, having the following scientific drivers: Solar System bodies, Binary stars, Transits of exoplanets, T Tauri stars, and GRBs. The 1.23 m is also scheduled for public outreach purposes, usually associated to high schools.

The ARAE (Robotic Astronomy & High-Energy Astrophysics) group of IAA (Instituto de Astrofísica de Andalucía, partner in the CAHA operations) agreed to contribute to CAHA by providing the control system of the 1.23 m telescope. (See http://www.iaa.es/arae/ and http://www.iaa.es/bootes/index.php for more details.) The ARAE group was granted 26 GRB triggers per year with an average duration of 0.5 nights per trigger. The upgrade of the telescope and its instrument control system is currently being carried out based on RTS2 (see [2] and references therein). One of the key requirements of the upgrade is to keep the existing telescope software and hardware untouched. The system must remain operational every night throughout the upgrade.

As none of the telescope instruments, nor their control electronics and software was developed by our group, we are kept away from the complex details of their construction and internal operation. As described later, we exclusively communicate with the control interfaces of the existing software.

The existing control system is an adapted version of that currently used by the 3.5 m Calar Alto telescope. It allows the observer to control the instruments through graphical user interface (GUI) programs running on two main observatory computers—one for the telescope control and the other for the camera. The observer is responsible for preparing the observing plan, opening and closing of the dome, taking care of executing exposures, inspecting images for good pointing and their quality, and synchronizing the telescope and the filter wheel movements with the CCD exposures. The major drawbacks of this approach are obvious: the observer spends most of the night working hard to get the data and keep the system running, and the system is prone to human errors when the observer is tired. Moreover, the observing logs are either hard to extract from the technical log or are not created by the system at all, and the interruption of the observation to react on a quickly evolving target of opportunity requires observer presence and attention.

In contrast, RTS2 was designed to create an autonomous observatory environment. The observer is allowed to interact with the system, and at worst case to take full manual control. The system is able to guide the observatory through the night, taking care of closing and opening the dome, acquiring sky flats, darks, and last, but not least, keeping detailed logs of the images acquired, judging pointing accuracy and producing preliminary results.

RTS2 device drivers are responsible for handling any errors that occur during their operation. If possible, the device is reset, and another attempt to get it operating is made. The RTS2 rts2-xmlrpcd component is responsible for communicating the errors to the users and custom scripts, which allows for the execution of more complicated scenarios. One of the core principles is to avoid restarting drivers that have failed. If the driver produces a core dump, it is safely removed from the system and it is up to the observer to restart it. This feature also allows RTS2 to be quite flexible—for example, a configuration without any telescope, just with a camera and other instrumentation, can be made without changing a single line of code. More information on handling the errors and other related issues is provided in [3].

The autonomous capabilities of the RTS2 system reside in a generic layer, with underlying hardware-specific drivers and communication via the TCP/IP network stack. So in an ideal world, once the provided skeleton drivers are used to write low-level RTS2 drivers for the hardware, every telescope can be made fully autonomous. To our knowledge, this is a big step forward from the traditional, incremental way of how observatory control software has been developed. Instead of being written primarily as a set of controls for the hardware, with some subsequent autopilot features, RTS2 was designed from the start to provide autonomous capabilities. Secondarily RTS2 also provides a way for the observer to interact directly with the hardware.

2.1. Current State of the Upgrade

Development of the first version of the RTS2 drivers was a question of a few days (and nights), since the RTS2 drivers were being written by the main author of RTS2 (with the assistance of the CAHA staff). The major obstacle which we had to face was running RTS2 on an old Solaris operating system, which is used to run the 1.23 m control computers. As RTS2 was written in quite portable C++ on Linux, and using GNU Autotools (GNU Autotools website: http://www.gnu.org/software/autoconf) for build control, the porting process involved changing a few unavailable functions (and renaming the variables called “sun”; “sun” is a defined symbol on Solaris systems). The system is now able to operate the same as any other observatory using RTS2.

The remaining obstacle is the lack of a natural incorporation of the autoguider in the RTS2 environment. This fact prevents us from taking images with long exposure times. Tests performed with the 1.23 m showed that exposures longer than 300 s produce elongated Point-Spread-Functions (PSFs), especially under sub-arc-second seeing conditions. The guider is an old instrument, with a quite complicated interface, without any autonomous capabilities. Thus, some time will be needed before we will be able to perform observations with the guider smoothly integrated in RTS2.

Currently the 1.23 m is able to respond to GRB alerts generated by the GRB Coordinates Network (GCN). The maximum slew time of the 1.23 m telescope is 4 minutes for the most unfavourable move. Usually the response time is below 3 minutes. The response time is limited by the speed of the current engines/mechanics moving the dome and the telescope. Given that the existing telescope/dome mechanical parts are strong and reliable, CAHA does not plan to renew them, so we do expect to overcome the slew-time limitation in the near future. The RTS2 Gamma-Ray Burst Daemon (rts2-grbd) of the 1.23 m is continuously linked via TCP/IP network socket to the GCN server at Goddard Space Flight Center (GSFC). In order to react to GCN alerts, it was necessary to accommodate the GCN connection in the CAHA firewall. Figure 3 shows a working scheme of the 1.23 m response mode to GCN alerts under RTS2.

fig3
Figure 3: The MAGIC near-infrared and optical CCD cameras of the 1.23 m telescope, both in the Cassegrain focus of the telescope. (a) shows MAGIC near-infrared camera. The MAGIC detector is a 256256 pixel HgCdTe array, providing a field of view of . The filter wheel of MAGIC allows broad-band imaging. The instrument is only mounted by special request, so it is not usually available. (b) shows optical CCD camera running on the 1.23 m telescope of Calar Alto. The optical CCD camera is based on a 2 k2 k SITE#2b chip. The green tube is the dewar and the white box is the electronic system associated to the camera. The filter wheel is located in the black flange just on the detector dewar.
701534.fig.004
Figure 4: Flow diagram of the GCN network and the response mode of the 1.23 m telescope. The whole process can take up to 4 minutes, depending on the position of the GRB on sky. The time needed to receive the coordinates from the high-energy satellite in the RTS2 server takes just a few seconds (usually less than 15 seconds). Currently most of the delay is due to the slow pointing of the 1.23 m, which could take up to 4 minutes in the worst case.

When a high-energy satellite (usually the Swift mission with its BAT [4] detector) localizes a GRB, the position is dumped in a few seconds from the GRB occurrence to ground-tracking stations and distributed by the GCN to its subscribers. In our case the GCN packet reaches the CAHA rts2-grbd server. Then the ongoing observations are interrupted and the 1.23 m is pointed towards the GRB position in order to start a series of short exposures (usually with the CCD windowed and binned in order to save readout time). Interrupting an observing run is a standard mechanism in RTS2 (see details in [3]). The interruption can be either hard, which interrupts the current exposure, or soft, which waits for the current exposure to finish. The rules governing this choice will be decided by the observers once the system is fully operational.

The RTS2 control system stores most of the data in a database (Postgresql website: http://www.postgresql.org). It includes tools for retrieving and manipulating information from the database. New targets can be entered through command line tools, autonomously from various triggering systems, or from the RTS2 Web interface.

The system has a powerful internal scripting engine, which enables users to define the observing strategy. By tracking devices states, the system handles synchronization among instruments, so the user does not have to know the details of the execution of the underlying observation. Scripting enables the user to specify all image parameters, dithering strategy, selected filters, and much more. For example, the following script runs observations in band, based on a series of 9 dithered images with an exposure time (per frame) of 240 seconds, with a 1  1 CCD binning and trimming the CCD to a subwindow of 500400 pixels [ = 600, = 1100, = 300, and = 700]:

Note that the syntax for the subwindow in the above example is (, -, , -). We have incorporated in RTS2 a call to the automatic astrometric calibration package described in [5]. This “on-the-fly” astrometric calibration corrects the telescope pointing, so the object can be placed on the desired () coordinates of the detector. The optical distortion on the CCD is negligible (less than one tenth of a pixel), so we decided to make a simple (and hence fast) fit considering a rotation term and a center field shift. The astrometric calibration is done on every frame. Polynomial fit is not used. The typical astrometric error (using 20 stars) is below , good enough to correct the 1.23 m pointing. The typical standard deviation in the inferred rotation angle is 0.1 degrees when 20 field stars are used in the fit. The success rate of the “on-the-fly” calibration is above 95%. The astrometric calibration of the remaining images is done manually afterwards.

In the near future we plan to provide also a rough photometric calibration based on the USNO-B catalogue [6]. Simultaneously to the telescope triggering an e-mail is sent to the 1.23 m users to warn them on the occurrence of the GRB. Additionally the GCN alert triggers the creation of an e-mail and an SMS for the ARAE group with relevant information of the GRB (coordinates, Galactic reddening, finding chart, elevation curves, and other information). Please see [7] for more details about this system.

Further improvements on this status are likely doable, so we feel confident that, under the current limitations (for instance, the telescope slew speed), we could reduce the GRB response times. This might allow us to detect the prompt optical emission associated to the gamma-ray event.

Another potential upgrade of the 1.23 m telescope could be the incorporation of MAGIC in RTS2. Rapid response observations with MAGIC would make the 1.23 m telescope very competitive in the GRB field. Currently this is beyond our scopes (and also beyond the CAHA man-power maintenance capabilities), but we do not discard it since the flexibility of RTS2 to accommodate new devices would allow us to integrate MAGIC (and new possible visitor instruments) quickly.

2.2. Integration of the Legacy Interfaces to RTS2

The following subsections provide descriptions of the legacy interfaces and their interaction with RTS2.

2.2.1. Interaction of RTS2 with the Calar Alto EPICS

The individual operations of the CAHA telescopes are coordinated, and controlled, by the Experimental Physics and Industrial Control System (EPICS website: http://www.aps.anl.gov/epics/index.php). The task of EPICS is to provide access and control of all the CAHA telescopes, as well as data from the central weather station and from the seeing and extinction monitors. The seeing and extinction monitors are based on small aperture telescopes located in CAHA whose values are available through EPICS.

The 1.23 m telescope mount, its focuser, and the camera filter wheel are all fully controllable through EPICS. The legacy telescope interface accepts objects coordinates in the J2000 coordinate system, and handles all the required calculations internally, including precession, aberration, reflection, and telescope pointing model offsets. Both the filter wheel and the focuser can be controlled through their own EPICS channels. Other devices in the 1.23 m telescope system do not exist in the EPICS universe: the CCD detector, the auto-guider camera, the dome itself, and various auxiliary switches (e.g., the dome lights).

We use the information provided through EPICS to automate several tasks of the 1.23 m. For instance, the meteorological information available from the EPICS is used to trigger the bad weather state, and hence to close the dome (Based on calculated Sun position through libnova, see http://libnova.sf.net) and stop observations. Bad weather is also triggered when both other telescopes are closed—this is the rule imposed on the 1.23 m operations by CAHA. For discussion on how the weather state voting is integrated into RTS2, including its fail-safe capabilities, (Network crashes and other failures (including the EPICS ones) are properly handled inside RTS2. A detailed description on how the weather voting system works is beyond the scope of this paper. We refer the reader to the extended discussion given in [3].) please see [3].

Yet another possible application lies in coordinating observations with the other Calar Alto telescopes. From the EPICS system, RTS2 can learn what the targets of the other telescopes are, whether they are in the RTS2 database, and depending on the target information can either start their monitoring or remove them from the list of targets which should be observed.

2.2.2. CCD Integration within RTS2

The optical CCD detector is connected to its own control computer. The control computer communicates with the control software, running on a master workstation, over the network. From the available C source code, we created an RTS2 device driver. All the major settings are supported, including binning and partial chip readout. The camera behaves as just another RTS2 supported CCD camera, visible in monitoring software and available for scripting.

2.2.3. Guider Camera and Its Integration in RTS2

The guider is built from a video camera with an image intensifier, fed from a pickoff mirror on a two-axis stage. This allows to place the guider image anywhere in the telescope field of view (FoV), thus eliminating the significant disadvantages of autoguiding-by-astrometry using the main camera: limited detector FoV, low gain, and a requirement for short exposure times. The guider camera has its own control computer, which assumes that the observer is sitting in front of it (e.g., the video output is sent directly to the screen). Partial remote control has since been provided, in part by placing a web camera in front of the guiding screen.

We would like to improve this setup with a fully integrated RTS2 device, which would transparently provide automatic search for bright stars in the FoV, and guiding capabilities. In principle, RTS2 is able to do this, and some promising tests were already carried out on the other RTS2 controlled telescopes. Currently the biggest problem is to figure out how to communicate with the guider, and to implement a full autoguiding loop.

2.2.4. Dome Control and Other Switches

As the dome is a critical component, its control is separate from the EPICS system (although dome status is reported to EPICS). In order to change the dome state, special commands must be run on the dome control computer. Similar commands are available to turn off and on dome lights and to control the telescope drives, the hydraulics, the tracking, and the mirror cover. Those commands are fully interfaced in RTS2, so RTS2 is able to control all those switches.

3. Preliminary Results

Although not fully autonomous, the 1.23 m has already performed followup optical observations of GRBs. None of the results below itemized was acquired by the automatic response mode of the RTS2 package, but some data were manually acquired by using RTS2 as the observing tool. Most of the data were taken by in situ observers, using the currently available GUI.

All the below listed GRBs showed X-ray afterglows which were localized by the XRT X-ray telescope on board Swift (see [8] for detailed information on the XRT instrument). So their X-ray afterglows were localized with uncertainties of only a few arc seconds, making the corresponding optical studies much more efficient.

GRB
The optical afterglow of this GRB [9] was observed with the 1.23 m in the band during two consecutive nights one week after the gamma-ray event. The observations were accompanied with -band observations carried out with the 3.5 m telescope of Calar Alto equipped with Omega. The data of the afterglow are currently being analyzed and are part of an international monitoring which will be published in [10].

GRB
We detected the afterglow of GRB 090424 [11] in on April 24.87 UT with a magnitude of . The preliminary results were reported in [12]. In the days following GRB 090424, a long-term monitoring was performed in and bands in order to search for the underlying supernova. Figure 5 shows a colored image constructed with the 1.23 m images taken in April 24.87 UT. The final results have been included in [13].

701534.fig.005
Figure 5: The figure shows the optical afterglow of GRB 090424 as detected with the 1.23 m CAHA telescope. The image has been created by combining -band images taken with the 2 k2 k CCD camera currently in use. The upper right box shows a magnified picture of the afterglow region. The magnitude of the afterglow was . The mean observing epoch of the image is April 24.87 UT. North is up and East is right. The field of view of the images is .
701534.fig.006
Figure 6: The picture shows the coadded -band image taken for GRB 090621B with the 1.23 m telescope of Calar Alto. The faintest of the two objects (the most upper one indicated with tick marks) represents the candidate reported in [14]. Approximately towards the Southwest, it is marked the candidate reported by [15], brighter than the one of [14]. The cyan circles show the USNO-A2 catalogue stars used for the astrometric and photometric calibrations. The field of view of the image is , with North up and East left.
701534.fig.007
Figure 7: Coadded -band image of GRB 090628 taken with the 1.23 m telescope. The large circle represents the preliminary XRT error circle [18], whereas the small one shows the refined one [20] reported for GRB 090628. The field of view of the image is . The total exposure time is 3120 s. The individual images were taken in June 28.9486–29.0225 UT (1.43–3.20 hours after the gamma-ray event). No objects were found in both error circles down to . More detailed information can be found in [21].

GRB
We detected the two afterglow candidates reported for this GRB [16] by Levan et al. and Galeev et al. [14, 15]. The observations were done in the band, 4.14–4.75 hours after the GRB. A deep second epoch observation is pending in order to search for photometric variability of the candidates. The preliminary results were reported in [17]. Figure 6 shows both candidates.

GRB
-band observations of the XRT position [18] were carried out 1.43–3.20 hours after the gamma-ray event. No counterpart was found down to in the XRT error box. Simultaneous near-infrared observations would have been very helpful in order to discriminate the possible high-redshift nature of this GRB but unfortunately they were not possible. The results of the observations were reported in [19].

GRB
This GRB was observed in July 27.9646-28.0063 UT in the band, 0.45–1.45 hours after the gamma-ray event. The afterglow reported by [23] was detected with a magnitude of , using as calibrator the USNO B1.0 star with and coordinates RA = 21 :  03 : 49.099, DEC = +64 : 55 : 58.23. The results can be found in [24].

The Discovery of the Optical Afterglow of GRB
GRB 090813 represents the first optical afterglow discovered with the 1.23 m CAHA telescope. -band observations of the XRT position were initiated 437 s after the GRB trigger, revealing an object with a rough magnitude of coincident with the XRT position. The lack of the object on the DSS strongly suggested its association with the optical afterglow of GRB 090813. The preliminary results were reported in [25].

GRB
This is the only GRB detected by the INTEGRAL satellite to date that we have followed up with the 1.23 m telescope. We carried out a series of -band observations with different exposure times ranging from 180 s to 700 s. The total exposure time invested for this GRB was 9520 s, with a mean observing epoch of Aug 14.1259 UT. No optical object was found within the refined X-ray error circle provided hours later by XRT. The 3 limiting magnitude of the coadded image is . A more extended description can be found in [21].

4. Conclusions

The 1.23 m is a wide-purpose telescope which is currently used by six international teams to perform long-term projects with a duration of four years. The ARAE group of IAA is responsible for automating the telescope operations so that such teams can perform their (usually long) observing campaigns without errors, yet enabling quick override observations of GRBs.

The GRB results obtained to date have been mostly taken by night observers. Use of the fully autonomous mode, provided by RTS2, is pending nontrivial integration of the guider. After this is done, we have reasonable hopes to believe that telescope will be able to react to GRB alerts in a few minutes. This could allow us to detect the optical emission at the first stages of the explosion, making the associated GRB science much more attractive for the GRB community.

We acquired images for seven GRBs, detecting the optical afterglows of four of them. The typical reaction time of these observations ranged from 8 minutes up to a few hours. When fully implemented, the autonomous system should be able to react to triggers within 4 minutes. We have reasonable hopes to obtain much more interesting and world-competitive results in the near future.

Acknowledgments

The research of J. Gorosabel, A.J. Castro-Tirado, R. Cunniffe and M. Jelínek is supported by the Spanish programmes AYA2008-03467/ESP, AYA2009-14000-C03-01, and AYA2007-63677. We are very grateful to all of the CAHA staff and in particular to Ulli Thiele for his excellent support with the 1.23 m telescope. P. Kubánek would like to acknowledge generous financial support provided by Spanish Programa de Ayudas FPI del Ministerio de Ciencia e Innovación (Subprograma FPI-MICINN) and European Fondo Social Europeo. We also would like to thank the two anonymous referees for their helpful comments.

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