This poster briefly outlines the research being undertaken at The Open University in the search for electromagnetic (EM) counterparts to gravitational wave candidates detected by the LIGO/Virgo Collaboration (LVC). This includes the setup of the PIRATE facility, which is a robotic telescope located in Tenerife, Spain, and is used as both a research and teaching telescope. Additionally the poster describes the methods used to perform rapid follow-up to gravitational wave alerts from LIGO/Virgo, and how the images are processed to look for fading transients. Lastly there is a short summary of results from the last observing campaign, corresponding to the second LIGO observing run (O2)

Kolb, Ulrich

Roberts, Dean

English

Open Research Online (Open)

Open Research OnlineThe Open University’s repository of research publicationsand other research outputsRapid response gravitational wave follow-up with thePIRATE robotic telescopeConference or Workshop ItemHow to cite:Roberts, Dean and Kolb, Ulrich (2018). Rapid response gravitational wave follow-up with the PIRATE robotictelescope. In: European Week of Astronomy and Space Science: RAS National Astronomy Meeting, 3-6 Apr 2018,Liverpool, UK.For guidance on citations see FAQs.c© [not recorded]Version: PosterCopyright and Moral Rights for the articles on this site are retained by the individual authors and/or other copyrightowners. For more information on Open Research Online’s data policy on reuse of materials please consult the policiespage.oro.open.ac.ukDean Roberts & Ulrich KolbSchool of Physical Sciences,The Open University, UK Rapid response gravitational wave follow-up with the PIRATE robotic telescope2. PIRATE Facility3. Method1. IntroductionThe existence of gravitational waves (GW) has been theorised for over 100 years,but they were not detected conclusively until 2015 (Abbott et al., 2016), owing totheir incredibly weak signal. These signals were detected by the LIGO/VirgoCollaboration (LVC) using incredibly sensitive interferometers, that are up to 4km inlength. And since 2015 they have detected gravitational waves emanating from 6compact binary mergers, and all but one of these were binary black holes. Howeverlast August the LVC detected gravitational waves from a binary neutron star mergerfor the first time (Abbott et al., 2017).In addition to the GW signal, an electromagnetic counterpart (EM), known as akilonova (see Figure 1), was also discovered. After a brief gamma-ray flash, theoptical signature of this counterpart was dominated by the kilonova process, butthis signal rapidly faded by several orders of magnitude in just 10 day (Figure 2).That is why follow-up observations such as these require rapid response times tocatch them before they disappear. The observations taken by several observatoriesof AT 2017gfo showed that with an initial magnitude of ~17 (i-band) (Coulter et al.,Soares-Santos et al., 2017), were it visible to the northern hemisphere at this timethen it would have also been observable with PIRATE. Nevertheless, PIRATE tookpart in the EM follow-up campaign for O2 and the results of which are given later.Previously PIRATE was located at the Observatorio Astronómico de Mallorca where it madeimportant contributions to time-domain astrophysics research projects, such as monitoringexoplanet transits (Gómez Maqueo Chew, et al., 2013) and eclipsing binaries (Lohr, et al.,2015), but it also played a major role in the teaching of undergraduate astronomy coursesat The Open University where it was used to teach undergraduate students the basics oftelescope operation. However, during 2016 the telescope was relocated to a new site atthe Observatorio del Teide in Tenerife where it is now housed in a new 4.5m dome atop the2400m high mountain, alongside its twin facility COAST (Figure 3).PIRATE itself consists of a 17-inch (0.43m) optical tube assembly (OTA) mounted on top of a10Micron GM4000 HPS mount (Figure 4). Attached to the end of the OTA is a an FLI ProLinecamera which contains a CCD chip with 16 Mega Pixels, that provide a 43’ field of view witha pixel scale of 0.63”/pixel (Kolb, 2014). In addition to this it is equipped with a 7 positionfilter wheel containing 3 broadband filters (Baader R, G, B), 3 narrowband filters (Hα, OIII,SII) and a clear filter. The telescope is controlled by an automated observatory controlsoftware called ABOT that allows students and staff to control the telescope in real timeover the internet; as well as schedule observations to be taken during the night. ABOT isalso deployed for BlackGEM, Solaris and MeerLICHT (Sybilski, 2015).The second LIGO observing run (O2) ran from 30th November 2016 to 25th August2017 and during this period they released 10+ alerts to the observing community, ofthese PIRATE was able to follow up 70% to some degree. For 4 of these we have 7+days of observations, which cover around 35 fields of view, in total we obtained 70nights of observations comprising of over 2,000 images.Having processed all the data we concluded that no unexpected transients weredetected in our data, however all the alerts we followed up originated from binaryblack hole mergers which aren’t expected to produce an electromagneticcounterpart.The plot in Figure 7 shows the lightcurve of a previously known W Uma classvariable star, that was serendipitously detected while performing our follow-upobservations, and there are dozens more similar examples to this in our data set.Lastly, the plot in Figure 8 shows the lightcurve of the MASTER OTJ033744.97+723159.0, which was a Type IIb supernova discovered pre-maximum bythe MASTER group while performing follow-up observations of another LIGO alert.We were able to observe this target for over 60 days with PIRATE whichdemonstrates its capability as a transient follow-up telescope.ReferencesAbbott, B. P.; et al. (2016, February). Observation of Gravitational Waves from a Binary Black Hole Merger. Physical Review Letters, 116. Abbott, B. P.; et al.  (2017, October). Multi-messenger Observations of a Binary Neutron Star Merger. Astrophysical Journal Letters, 848, L12.Bertin, E. (2010, October) SExtractor: Source Extractor. Astrophysics Source Code Library, 1010.064.Coulter D. A. et al., (2017, October) Swope Supernova Survey 2017a (SSS17a) the Optical Counterpart to a Gravitational Wave Source, Science, eaap9811Gómez Maqueo Chew, Y., Faedi, F., Pollacco, D., Brown, D. J., Doyle, A. P., Collier Cameron, A., . . . Armstrong, D. J. (2013, November). Discovery of WASP-65b and WASP-75b: Two hot Jupiters without highly inflated radii. Astronomy & Astrophysics, 559.Kolb, U. (2014). The PIRATE Facility: At the crossroads of research and teaching. In J. Tello, A. Riva, D. Hiriart, & A. Castro-Tirado (Ed.), RevMexAA, 45, pp. 16-19.Lohr, M. E., Norton, A. J., Gillen, E., Busuttil, R., Kolb, U. C., Aigrain, S., . . . González, E. (2015, June). The doubly eclipsing quintuple low-mass star system 1SWASP J093010.78+533859.5. Astronomy & Astrophysics, 578.Metzger, B. D. and Berger, F. (2012, February).  What is the Most Promising Electromagnetic Counter-part of a Neutron Star Binary Merger?ApJ, 746:48.Pian E. et al., (2017, October) Spectroscopic identification of r-process nucleosynthesis in a double neutron-star merger, Nature, 551, 67Soares-Santos, M. et al., (2017, October) The Electromagnetic Counterpart of the Binary Neutron Star Merger LIGO/Virgo GW170817. I. Discovery of the Optical Counterpart Using the Dark Energy Camera, AstrophysicalJournal, 848, L16Singer, L. (2015). LIGO-Virgo EM Follow-Up Tutorial. LIGO Document Database (Website). Retrieved from https://dcc.ligo.org/LIGO-G1500442/public Singer, L., Chen, H.-Y., Holz, D. E., Farr, W. M., Price, L. R., Raymond, V., . . . Mandel, I. (2016, September). Going the Distance: Mapping Host Galaxies of LIGO and Virgo Sources in Three Dimensions Using Local Cosmography and Targeted follow-up. The Astrophysical Journal Letters, 829:L15.Sokolovsky, K. V.; Lebedev, A. A. (2017, April) VaST: Variability Search Toolkit. Astrophysics Source Code Library, 1704.005.Sybilski, P. (2015, April). ABOT: Software for global networks of robotic telescopes. Sybilla Technologies (Website). Retrieved from http://sybillatechnologies.com/downloads/PS%20ST%20ESA.pdfWhite, D. J., Daw, E. J., & Dhillon, V. S. (2011, April). A list of galaxies for gravitational wave searches. Classic and Quantum Gravity, 28(8). Background Image: Edward HandFigures 3 & 4. The PIRATE telescope by day in the shadow of Mt Teide and at night under the Milky Way . Image Credits: Johannes BaaderOne of the key advantages in using a robotic telescope is the rapid response times it canachieve for any astronomical alerts of interest, such as gamma-ray bursts andgravitational waves. However to utilize this it was necessary to create a bespoke pipelinethat would process the incoming alerts quickly, but more importantly, without anyhuman intervention. The result was a Python script built on one written by Leo Singer(Singer, 2015) to receive and process gravitational-wave candidate alerts from AdvancedLIGO and Virgo via GCN alerts (see Figures 5 & 6).The alerts contain a sky localization probability map (known as a skymap) and the keystep in this process is deciding which areas of the skymap to observe given theirrelatively large size. Currently this is done using a simple method of highest to lowestprobability and with a maximum number of observations cut-off. However an alternativeway would be to target individual galaxies within the search area, such as those in theGravitational Wave Galaxy Catalogue (White, Daw, & Dhillon, 2011), and even potentiallyin a 3D search volume using the new 3D skymaps (Singer, et al., 2016).Once the data is calibrated we use the source extraction software SExtractor (Bertin E.,2010) to perform photometry, which then gets passed on to a variable star detectionsoftware VaST (Sokolovsky & Lebedev, 2017). This generates lightcurves for all the starsin a reference image across the dataset; and it then uses multiple variability indices toshow which stars have high variability across the time series. The index we rely on is theratio of the variance over the mean square successive difference, which highlights starswith variability over longer time scales.4. ResultsFigure 5. A flowchart showing the different stages of LIGO GW trigger analysis. Image Credit: LIGO/Virgo CollaborationFigure 6. A flowchart highlighting the different stages of the PIRATE alert pipeline.Figure 1 (Left)  An illustration of electromagnetic counterparts from binary neutron star mergers. Metzger & Berger (2012). Figure 2 (Right) Multiband optical light curve of AT 2017gfo using the VLT Survey Telescope (VST) Pian et al. (2017).This poster briefly outlines the research being undertaken at The Open University in the search for electromagnetic (EM) counterparts to gravitational wave candidates detected by the LIGO/VirgoCollaboration (LVC). This includes the setup of the PIRATE facility, which is a robotic telescope located in Tenerife, Spain, and is used as both a research and teaching telescope. Additionally the posterdescribes the methods used to perform rapid follow-up to gravitational wave alerts from LIGO/Virgo, and how the images are processed to look for fading transients. Lastly there is a short summaryof results from the last observing campaign, corresponding to the second LIGO observing run (O2).AbstractFigure 7. The lightcurve of a W UMa type eclipsing binary, detected while searching for GW counterparts. Figure 8. Two lightcurves in Red & Blue filters of a Type IIbsupernova, first discovered by the MASTER network.

Rapid response gravitational wave follow-up with the PIRATE robotic telescope

This poster briefly outlines the research being undertaken at The Open University in the search for electromagnetic (EM) counterparts to gravitational wave candidates detected by the LIGO/Virgo Collaboration (LVC). This includes the setup of the PIRATE facility, which is a robotic telescope located in Tenerife, Spain, and is used as both a research and teaching telescope. Additionally the poster describes the methods used to perform rapid follow-up to gravitational wave alerts from LIGO/Virgo, including a description of the types of EM signals that could be discovered. Lastly there is a short summary of the current observing campaign, corresponding to the second LIGO observing run (O2)

Open Research OnlineThe Open University’s repository of research publicationsand other research outputsRapid response gravitational wave follow-up with thePIRATE robotic telescopeOtherHow to cite:Roberts, Dean and Kolb, Ulrich (2017). Rapid response gravitational wave follow-up with the PIRATE robotictelescope. The Open University.For guidance on citations see FAQs.c© 2017 The AuthorsVersion: PosterCopyright and Moral Rights for the articles on this site are retained by the individual authors and/or other copyrightowners. For more information on Open Research Online’s data policy on reuse of materials please consult the policiespage.oro.open.ac.ukDean Roberts & Ulrich KolbSchool of Physical Sciences,The Open University, UK Rapid response gravitational wave follow-up with the PIRATE robotic telescope2. PIRATE Facility3. Method1. IntroductionThe existence of gravitational waves has been theorised for over 100 years, but theywere not detected conclusively until 2015 (Abbott et al., 2016), owing to theirincredibly weak signal. Currently there are two main sources of gravitational wavesthat can be detected; compact binary mergers and burst events, the latter of whichhas not yet had a confirmed detection. However there have been 3 confirmeddetections of compact binary mergers which have all been between binary blackholes (GW150914, GW151226 & GW170104). Due to the radiationless nature ofblack holes and long coalescence timescales it is not expected that electromagnetic(EM) counterparts will be produced when two black holes merge. However thescenario is different when two neutron stars merge because they are expected toproduce observable EM counterparts as shown in Figure 1 - this can range all theway from gamma-rays down to radio (Chu, et al., 2016). There is also predicted to betwo types of EM emission, firstly a short gamma-ray burst is expected to be releasedat the time of merger, which would fade through the EM spectrum. And then in thesubsequent hours and days an event known as a kilonova might occur, that ispowered by the radioactive decay of the neutron rich material that surrounds thenewly merged compact object. It is expected that both these events will be visible inthe optical and if the event is close/bright enough then they should be observable toground based telescopes such as PIRATE.Previously PIRATE was located at the Observatorio Astronómico de Mallorca where it madeimportant contributions to time-domain astrophysics research projects, such as monitoringexoplanet transits (Gómez Maqueo Chew, et al., 2013) and eclipsing binaries (Lohr, et al.,2015), but it also played a major role in the teaching of undergraduate astronomy coursesat The Open University where it was used to teach undergraduate students the basics oftelescope operation. During 2016 the telescope was relocated to the Observatorio del Teidein Tenerife where it is now housed in a new dome atop the 2400m mountain (Figure 2).PIRATE itself consists of a 17-inch (0.43m) optical tube assembly (OTA) mounted on top of a10Micron GM4000 HPS mount (Figure 3). Attached to the end of the OTA is a KAF-16803CCD chip housed within a FLI ProLine PL16803 camera. This camera contains 4096 X 4086pixels that provide a 43’ field of view with a pixel scale of 0.63”/pixel (Kolb, 2014). Inaddition to this it is equipped with a 7 position filter wheel containing 3 broadband filters(Baader R, G, B), 3 narrowband filters (Hα, OIII, SII) and a clear filter. The telescope iscontrolled by an automated observatory control software called ABOT that allows studentsand staff to control the telescope in real time over the internet; as well as scheduleobservations to be taken during the night. ABOT is also deployed for BlackGEM, Solaris andMeerLICHT (Sybilski, 2015).We are currently in the process of analysing all data obtained during the secondLIGO observing run (O2) which ran from 30/11/16 to 25/08/17, however due to theembargo surrounding O2 data and results we cannot say any more other thanPIRATE performed follow-up observations on 6 of the 8 triggers announced in theJune update on the LIGO news website (http://www.ligo.org/news.php).Up until the 23rd June PIRATE had been observing for 58 nights in total, duringwhich it acquired 1,700 images in search of an EM counterpart corresponding tothese 6 gravitational wave candidate alerts, and analysis is ongoing with any resultsbeing published in co-operation with the LVC.The plots in Figures 6 & 7 are taken from a similar research project where PIRATEhas been monitoring the Kepler field that contains the variable star KIC8462852(otherwise known as Tabby’s Star) with a high cadence over several months. Bothstars shown below are red supergiants that show some irregular pulsatingbehaviour (Figure 6) over a period of a few days and what appears to be an eclipsingbinary (Figure7) with a ~100 day period.ReferencesAbbott, B. P.; et al (2016, February). Observation of Gravitational Waves from a Binary Black Hole Merger. Physical Review Letters, 116. Bertin, E. (2010, October) SExtractor: Source Extractor. Astrophysics Source Code Library, 1010.064.Chu, Q.; et al. (2016, March). Capturing the electromagnetic counterparts of binary neutron star mergers through low-latency gravitational wave triggers. MNRAS, 459.Collins, K. A.; Kielkopf, J. F.; Stassun, K. G.; Hessman, F. V. (2017, February). AstroImageJ: Image Processing and Photometric Extraction for Ultra-Precise Astronomical Light Curves. The Astronomical Journal, 153:77.Gómez Maqueo Chew, Y., Faedi, F., Pollacco, D., Brown, D. J., Doyle, A. P., Collier Cameron, A., . . . Armstrong, D. J. (2013, November). Discovery of WASP-65b and WASP-75b: Two hot Jupiters without highly inflated radii. Astronomy & Astrophysics, 559.Kolb, U. (2014). The PIRATE Facility: At the crossroads of research and teaching. In J. Tello, A. Riva, D. Hiriart, & A. Castro-Tirado (Ed.), RevMexAA, 45, pp. 16-19.Lohr, M. E., Norton, A. J., Gillen, E., Busuttil, R., Kolb, U. C., Aigrain, S., . . . González, E. (2015, June). The doubly eclipsing quintuple low-mass star system 1SWASP J093010.78+533859.5. Astronomy & Astrophysics, 578.Singer, L. (2015). LIGO-Virgo EM Follow-Up Tutorial. LIGO Document Database (Website). Retrieved from https://dcc.ligo.org/LIGO-G1500442/public Singer, L., Chen, H.-Y., Holz, D. E., Farr, W. M., Price, L. R., Raymond, V., . . . Mandel, I. (2016, September). Going the Distance: Mapping Host Galaxies of LIGO and Virgo Sources in Three Dimensions Using Local Cosmography and Targeted follow-up. The Astrophysical Journal Letters, 829:L15.Sokolovsky, K. V.; Lebedev, A. A. (2017, April) VaST: Variability Search Toolkit. Astrophysics Source Code Library, 1704.005.Sybilski, P. (2015, April). ABOT: Software for global networks of robotic telescopes. Sybilla Technologies (Website). Retrieved from http://sybillatechnologies.com/downloads/PS%20ST%20ESA.pdfWhite, D. J., Daw, E. J., & Dhillon, V. S. (2011, April). A list of galaxies for gravitational wave searches. Classic and Quantum Gravity, 28(8). Background Image: Edward HandFigures 2 & 3. The PIRATE telescope by day in the shadow of Mt Teide and at night under the Milky Way . Image Credits: Johannes BaaderOne of the key advantages in using a robotic telescope is the rapid response times it canachieve for any astronomical alerts of interest, such as gamma-ray bursts andgravitational waves. However to utilize this it was necessary to create a bespoke pipelinethat would process the incoming alerts quickly, but more importantly, without anyhuman intervention. The result was a Python script built on one written by Leo Singer(Singer, 2015) to receive and process gravitational-wave candidate alerts from AdvancedLIGO and Virgo via GCN alerts (see Figures 4 & 5).The alerts contain a sky localization probability map (known as a skymap) and the keystep in this process is deciding which areas of the skymap to observe given theirrelatively large size. Currently this is done using a simple method of highest to lowestprobability and with a maximum number of observations cut-off. However an alternativeway would be to target individual galaxies within the search area, such as those in theGravitational Wave Galaxy Catalogue (White, Daw, & Dhillon, 2011), and even potentiallyin a 3D search volume using the new 3D skymaps (Singer, et al., 2016).The data is calibrated and plate solved using the image processing software AstroImageJ(Collins K., et al., 2016). We use the source extraction software SExtractor (Bertin E.,2010) to perform photometry on our images, which then gets passed on to a variablestar detection software VaST (Sokolovsky & Lebedev, 2017). This generates lightcurvesfor all the stars in a reference image; from which it then produces a plot of magnitudesagainst a measure of variability for the lightcurves, typically standard deviation.4. ResultsFigure 4. A flowchart showing the different stages of LIGO GW trigger analysis. Image Credit: LIGO/Virgo CollaborationFigure 5. A flowchart showing the different stages of the PIRATE alert pipeline. Image Credit: Simulating Extreme SpacetimesFigures 6 & 7. Lightcurves of two variable stars within the Kepler field, KIC8396947 (left) and KIC8397019 (right), using data taken with the PIRATE telescope.Figure 1. Predicted counterpart time-scales for binary neutron star mergers. (Chu, et al., 2016)This poster briefly outlines the research being undertaken at The Open University in the search for electromagnetic (EM) counterparts to gravitational wave candidates detected by the LIGO/VirgoCollaboration (LVC). This includes the setup of the PIRATE facility, which is a robotic telescope located in Tenerife, Spain, and is used as both a research and teaching telescope. Additionally the posterdescribes the methods used to perform rapid follow-up to gravitational wave alerts from LIGO/Virgo, including a description of the types of EM signals that could be discovered. Lastly there is a shortsummary of the current observing campaign, corresponding to the second LIGO observing run (O2).Abstract

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Rapid response gravitational wave follow-up with the PIRATE robotic telescope

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