Kendall Ackley’s research while affiliated with University of Warwick and other places

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Publications (54)


Leveraging Movement Representation from Contrastive Learning for Asteroid Detection
  • Article

December 2024

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13 Reads

Publications of the Astronomical Society of the Pacific

Noppachanin Kongsathitporn

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Akara Supratak

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Kanthanakorn Noysena

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[...]

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Rene P. Breton

To support asteroid-related studies, current motion detectors are utilized to select moving object candidates based on their visualizations and movements in sequences of sky exposures. However, the existing detectors encounter the manual parameter settings which require experts to assign proper parameters. Moreover, although the deep learning approach could automate the detection process, these approaches still require synthetic images and hand-engineered features to improve their performance. In this work, we propose an end-to-end deep learning model consisting of two branches. The first branch is trained with contrastive learning to extract a contrastive feature from sequences of sky exposures. This learning method encourages the model to capture a lower-dimensional representation, ensuring that sequences with moving sources (i.e., potential asteroids) are distinct from those without moving sources. The second branch is designed to learn additional features from the sky exposure sequences, which are then concatenated into the movement features before being processed by subsequent layers for the detection of asteroid candidates. We evaluate our model on sufficiently long-duration sequences and perform a comparative study with detection software. Additionally, we demonstrate the use of our model to suggest potential asteroids using photometry filtering. The proposed model outperforms the baseline model for asteroid streak detection by +7.70% of f1-score. Moreover, our study shows promising performance for long-duration sequences and improvement after adding the contrastive feature. Additionally, we demonstrate the uses of our model with the filtering to detect potential asteroids in wide-field detection using the long-duration sequences. Our model could complement the software as it suggests additional asteroids to its detection result.


GERry: A Code to Optimise the Hunt for the Electromagnetic Counter-parts to Gravitational Wave Events

July 2024

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1 Read

The search for the electromagnetic counterparts to gravitational wave (GW) events has been rapidly gathering pace in recent years thanks to the increasing number and capabilities of both gravitational wave detectors and wide field survey telescopes. Difficulties remain, however, in detecting these counterparts due to their inherent scarcity, faintness and rapidly evolving nature. To find these counterparts, it is important that one optimises the observing strategy for their recovery. This can be difficult due to the large number of potential variables at play. Such follow-up campaigns are also capable of detecting hundreds or potentially thousands of unrelated transients, particularly for GW events with poor localisation. Even if the observations are capable of detecting a counterpart, finding it among the numerous contaminants can prove challenging. Here we present the Gravitational wave Electromagnetic RecovRY code (GERry) to perform detailed analysis and survey-agnostic quantification of observing campaigns attempting to recover electromagnetic counterparts. GERry considers the campaign's spatial, temporal and wavelength coverage, in addition to Galactic extinction and the expected counterpart light curve evolution from the GW 3D localisation volume. It returns quantified statistics that can be used to: determine the probability of having detected the counterpart, identify the most promising sources, and assess and refine strategy. Here we demonstrate the code to look at the performance and parameter space probed by current and upcoming wide-field surveys such as GOTO & VRO.



Figure 1. The complete GOTO network as of April 2023. Top: GOTO-North on La Palma, with GOTO-1 on the left and GOTO-2 on the right. Bottom: GOTO-South at Siding Spring, with GOTO-3 on the left and GOTO-4 on the right.
Figure 4. A screenshot of the GOTO Marshall web interface. The source shown is the type II supernova SN2024cld, which was discovered as part of the GOTO-FAST survey. 25, 26
The Gravitational-wave Optical Transient Observer (GOTO)
  • Preprint
  • File available

July 2024

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25 Reads

The Gravitational-wave Optical Transient Observer (GOTO) is a project dedicated to identifying optical counter-parts to gravitational-wave detections using a network of dedicated, wide-field telescopes. After almost a decade of design, construction, and commissioning work, the GOTO network is now fully operational with two antipodal sites: La Palma in the Canary Islands and Siding Spring in Australia. Both sites host two independent robotic mounts, each with a field-of-view of 44 square degrees formed by an array of eight 40 cm telescopes, resulting in an instantaneous 88 square degree field-of-view per site. All four telescopes operate as a single integrated network, with the ultimate aim of surveying the entire sky every 2-3 days and allowing near-24-hour response to transient events within a minute of their detection. In the modern era of transient astronomy, automated telescopes like GOTO form a vital link between multi-messenger discovery facilities and in-depth follow-up by larger telescopes. GOTO is already producing a wide range of scientific results, assisted by an efficient discovery pipeline and a successful citizen science project: Kilonova Seekers.

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Figure 1. The complete GOTO network as of April 2023. Top: GOTO-North on La Palma, with GOTO-1 on the left and GOTO-2 on the right. Bottom: GOTO-South at Siding Spring, with GOTO-3 on the left and GOTO-4 on the right.
Figure 4. A screenshot of the GOTO Marshall web interface. The source shown is the type II supernova SN2024cld, which was discovered as part of the GOTO-FAST survey. 25, 26
The Gravitational-wave Optical Transient Observer (GOTO)

July 2024

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21 Reads

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6 Citations

The Gravitational-wave Optical Transient Observer (GOTO) is a project dedicated to identifying optical counterparts to gravitational-wave detections using a network of dedicated, wide-field telescopes. After almost a decade of design, construction, and commissioning work, the GOTO network is now fully operational with two antipodal sites: La Palma in the Canary Islands and Siding Spring in Australia. Both sites host two independent robotic mounts, each with a field-of-view of 44 square degrees formed by an array of eight 40 cm telescopes, resulting in an instantaneous 88 square degree field-of-view per site. All four telescopes operate as a single integrated network, with the ultimate aim of surveying the entire sky every 2-3 days and allowing near-24-hour response to transient events within a minute of their detection. In the modern era of transient astronomy, automated telescopes like GOTO form a vital link between multi-messenger discovery facilities and in-depth follow-up by larger telescopes. GOTO is already producing a wide range of scientific results, assisted by an efficient discovery pipeline and a successful citizen science project: Kilonova Seekers.


Magnetars as powering sources of gamma-ray burst associated supernovae, and unsupervized clustering of cosmic explosions

June 2024

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25 Reads

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11 Citations

Monthly Notices of the Royal Astronomical Society

We present the semi-analytical light curve modelling of 13 supernovae associated with gamma-ray bursts (GRB-SNe) along with two relativistic broad-lined (Ic-BL) SNe without GRB association (SNe 2009bb and 2012ap), considering millisecond magnetars as central-engine-based power sources for these events. The bolometric light curves of all 15 SNe in our sample are well-regenerated utilizing a χ2-minimization code, MINIM, and numerous parameters are constrained. The median values of ejecta mass (Mej), magnetar’s initial spin period (Pi), and magnetic field (B) for GRB-SNe are determined to be ≈5.2 M⊙, 20.5 ms, and 20.1 × 1014 G, respectively. We leverage machine learning (ML) algorithms to comprehensively compare the three-dimensional parameter space encompassing Mej, Pi, and B for GRB-SNe determined herein to those of H-deficient superluminous SNe (SLSNe-I), fast blue optical transients (FBOTs), long GRBs (LGRBs), and short GRBs (SGRBs) obtained from the literature. The application of unsupervized ML clustering algorithms on the parameters Mej, Pi, and B for GRB-SNe, SLSNe-I, and FBOTs yields a classification accuracy of ∼95 per cent. Extending these methods to classify GRB-SNe, SLSNe-I, LGRBs, and SGRBs based on Pi and B values results in an accuracy of ∼84 per cent. Our investigations show that GRB-SNe and relativistic Ic-BL SNe presented in this study occupy different parameter spaces for Mej, Pi, and B than those of SLSNe-I, FBOTs, LGRBs, and SGRBs. This indicates that magnetars with different Pi and B can give birth to distinct types of transients.


Figure 1. The quasi-bolometric light curves of the 13 GRB-SNe and two relativistic Ic-BL SNe used in the present study, along with their low-order spline function fitting curves, are shown. Data courtesy: Cano et al. 2017b,a; Izzo et al. 2019; Melandri et al. 2019, 2022; Kumar et al. 2022, and references therein.
Magnetars as Powering Sources of Gamma-Ray Burst Associated Supernovae, and Unsupervised Clustering of Cosmic Explosions

March 2024

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47 Reads

We present the semi-analytical light curve modelling of 13 supernovae associated with gamma-ray bursts (GRB-SNe) along with two relativistic broad-lined (Ic-BL) SNe without GRBs association (SNe 2009bb and 2012ap), considering millisecond magnetars as central-engine-based power sources for these events. The bolometric light curves of all 15 SNe in our sample are well-regenerated utilising a χ2 −minimisation code, MINIM, and numerous parameters are constrained. The median values of ejecta mass (Mej), magnetar's initial spin period (Pi) and magnetic field (B) for GRB-SNe are determined to be ≈ 5.2 M⊙, 20.5 ms and 20.1 × 10^14 G, respectively. We leverage machine learning (ML) algorithms to comprehensively compare the 3-dimensional parameter space encompassing Mej, Pi, and B for GRB-SNe determined herein to those of H-deficient superluminous SNe (SLSNe-I), fast blue optical transients (FBOTs), long GRBs (LGRBs), and short GRBs (SGRBs) obtained from the literature. The application of unsupervised ML clustering algorithms on the parameters Mej, Pi, and B for GRB-SNe, SLSNe-I, and FBOTs yields a classification accuracy of ∼95%. Extending these methods to classify GRB-SNe, SLSNe-I, LGRBs, and SGRBs based on Pi and B values results in an accuracy of ∼84%. Our investigations show that GRB-SNe and relativistic Ic-BL SNe presented in this study occupy different parameter spaces for Mej, Pi, and B than those of SLSNe-I, FBOTs, LGRBs and SGRBs. This indicates that magnetars with different Pi and B can give birth to distinct types of transients.


The high-energy properties of GRB 230307A
a, The light curve of the GRB at 64-ms time resolution with the Fermi/GBM. The shaded region indicates the region in which saturation may be an issue. The burst begins very hard, with the count rate dominated by photons in the hardest (100–900-keV) band, but rapidly softens, with the count rate in the hard band being progressively overtaken by softer bands (such as 8–25 keV and 25–100 keV) beyond about 20 s. This strong hard-to-soft evolution is reminiscent of GRB 211211A (ref. ²⁰) and is caused by the motion of two spectral breaks through the gamma-ray regime (see Methods). b, The X-ray light curves of GRBs from the Swift X-ray telescope. These have been divided by the prompt fluence of the burst, which broadly scales with the X-ray light curve luminosity, resulting in a modest spread of afterglows. The greyscale background represents the ensemble of long GRBs. GRB 230307A is an extreme outlier of the >1,000 Swift GRBs, with an extremely faint afterglow for the brightness of its prompt emission. Other merger GRBs from long bursts, and those suggested to be short with extended emission (EE), occupy a similar region of the parameter space. This suggests that the prompt to afterglow fluence could be a valuable tool in distinguishing long GRBs from mergers and those from supernovae.
JWST images of GRB 230307A at 28.5 days post burst
a, The wide-field image combining the F115W, F150W and F444W images. The putative host is the bright face-on spiral galaxy, whereas the afterglow appears at a 30-arcsec offset, within the white box. The scale bar at the lower left represents 10″. b–g, Cut-outs of the NIRCam data around the GRB afterglow location. The source is faint and barely detected in the bluer bands but very bright and well detected in the red bands. In the red bands, a faint galaxy is present northeast of the transient position. This galaxy has a redshift of z = 3.87 but we consider it to be a background object unrelated to the GRB (see Supplementary Information).
JWST/NIRSpec spectroscopy of the counterpart of GRB 230307A
The top portion shows the 2D spectrum rectified to a common wavelength scale. The transient is well detected beyond 2 microns but not shortward, indicative of an extremely red source. Emission lines from the nearby galaxy at z = 3.87 can also be seen offset from the afterglow trace. The lower panel shows the 1D extraction of the spectrum in comparison with the latest (10-day) AT2017gfo epoch and a kilonova model. A clear emission feature can be seen at about 2.15 microns at both 29 and 61 days. This feature is consistent with the expected location of [Te III], whereas redder features are compatible with lines from [Se III] and [W III]. This line is also clearly visible in the scaled late-time spectrum of AT2017gfo (refs. 27,32), whereas the red colours are also comparable with those of AT2017gfo as measured with Spitzer (ref. ²⁴; shown scaled to the 29-day NIRSpec spectrum). Error bars on photometry refer to the 1σ error bar on the y axis and the filter width on the x axis.
A comparison of the counterpart of GRB 230307A with AT2017gfo associated with GW170817
AT2017gfo has been scaled to the same distance as GRB 230307A. Beyond about 2 days, the kilonova dominates the counterpart. The decay rates in both the optical and infrared are very similar to those in AT2017gfo. These are too rapid for any plausible afterglow model. There is also good agreement in the late-time slope between the measurements made at 4.4 microns with the JWST and at 4.5 microns for AT2017gfo with Spitzer²⁴. Error bars refer to the 1σ uncertainty.
Heavy element production in a compact object merger observed by JWST

October 2023

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165 Reads

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166 Citations

Nature

The mergers of binary compact objects such as neutron stars and black holes are of central interest to several areas of astrophysics, including as the progenitors of gamma-ray bursts (GRBs)1, sources of high-frequency gravitational waves (GW)2 and likely production sites for heavy element nucleosynthesis via rapid neutron capture (the r-process)3. Here we present observations of the exceptionally bright gamma-ray burst GRB 230307A. We show that GRB 230307A belongs to the class of long-duration gamma-ray bursts associated with compact object mergers4-6, and contains a kilonova similar to AT2017gfo, associated with the gravitational-wave merger GW1708177-12. We obtained James Webb Space Telescope mid-infrared (mid-IR) imaging and spectroscopy 29 and 61 days after the burst. The spectroscopy shows an emission line at 2.15 microns which we interpret as tellurium (atomic mass A=130), and a very red source, emitting most of its light in the mid-IR due to the production of lanthanides. These observations demonstrate that nucleosynthesis in GRBs can create r-process elements across a broad atomic mass range and play a central role in heavy element nucleosynthesis across the Universe.



Gamma-ray Transient Network Science Analysis Group Report

August 2023

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43 Reads

The Interplanetary Network (IPN) is a detection, localization and alert system that utilizes the arrival time of transient signals in gamma-ray detectors on spacecraft separated by planetary baselines to geometrically locate the origin of these transients. Due to the changing astrophysical landscape and the new emphasis on time domain and multi-messenger astrophysics (TDAMM) from the Pathways to Discovery in Astronomy and Astrophysics for the 2020s, this Gamma-ray Transient Network Science Analysis Group was tasked to understand the role of the IPN and high-energy monitors in this new era. The charge includes describing the science made possible with these facilities, tracing the corresponding requirements and capabilities, and highlighting where improved operations of existing instruments and the IPN would enhance TDAMM science. While this study considers the full multiwavelength and multimessenger context, the findings are specific to space-based high-energy monitors. These facilities are important both for full characterization of these transients as well as facilitating follow-up observations through discovery and localization. The full document reports a brief history of this field, followed by our detailed analyses and findings in some 68 pages, providing a holistic overview of the role of the IPN and high-energy monitors in the coming decades.


Citations (27)


... (hereafter GOTO 0650) obtained with OPTICAM (Castro et al. 2019(Castro et al. , 2024. GOTO 0650 was discovered by the Gravitational-wave Optical Transient Observer (GOTO; Steeghs et al. 2022;Dyer et al. 2024) on Oct. 4 202403:36:36 UT (Killestein et al. 2024a. The transient reached an L band (∼ g r) magnitude of 13.7 in the discovery images and was associated with a ∼ 22 nd mag quiescent counterpart implying an outburst amplitude of ∼ 8.5 mag, typical of WZ Sge stars. ...

Reference:

Bridging the Gap: OPTICAM Reveals the Hidden Spin of the WZ Sge Star GOTO 065054.49+593624.51
The Gravitational-wave Optical Transient Observer (GOTO)

... An alternative scenario involving rotational energy loss via magnetic dipole radiation was explored 108 , linking the magnetar's spindown rate to the radiative diffusion timescale. Fitting the light curve of SN 2025kg with a magnetar-powered model yields best-fitting parameters of M ej = 2.42 +0. ...

Magnetars as powering sources of gamma-ray burst associated supernovae, and unsupervized clustering of cosmic explosions
  • Citing Article
  • June 2024

Monthly Notices of the Royal Astronomical Society

... Moreover, it plays a significant role in the scientific argument of Disberg and Nelemans (2023), who aimed to explain the gap at m ≈ 17M ⊙ , and it is therefore designed to optimally display the mass distribution and its apparent gap. Examples of propositional images in astrophysics can include graphs inferred from simulations (e.g., Figure 4 of Disberg et al. 2025) or observations (e.g., Figure 1 of Arcavi et al. 2017), or sometimes even pictures of the observations themselves (e.g., Figure 2 of Levan et al. 2024). ...

Heavy element production in a compact object merger observed by JWST

Nature

... The focus of this paper is the Type Ibn supernova SN 2023tsz. It was discovered by the Gravitational-wave Optical Transient Observer (GOTO; Steeghs et al. 2022;Dyer et al. 2022Dyer et al. , 2024 on 2023 September 28 and reported to the Transient Name Server under the name GOTO23anx (Godson et al. 2023). There was a prior non-detection and two detections from All-sky Automated Survey for Supernovae (ASAS-SN; Shappee et al. 2014;Kochanek et al. 2017) on September 13, 19, and 25 respectively. ...

The Gravitational-wave Optical Transient Observer (GOTO)
  • Citing Conference Paper
  • August 2022

... This landmark discovery opened a new observational window for exploring strong-field spacetime geometry. With the enhanced sensitivity of detectors in the LIGO-Virgo-KAGRA collaboration [2,3] and the upcoming launch of the space-based interferometer LISA, which is designed to capture millihertz gravitational waves [4,5], developing accurate waveform models has become increasingly critical. These models are essential for extracting the mass, spin, and other dynamical parameters of the merging bodies, from the gravitational-wave signals. ...

Search for intermediate-mass black hole binaries in the third observing run of Advanced LIGO and Advanced Virgo

... A number of optical AGN flares measured by the Zwicky Transient Facility (ZTF) [43] have been investigated as possible EM counterparts to certain BBH GW events of the LVK experiment [11,14]. These MM associations are currently debated, mostly because the spatial correlation among the different messengers is challenging [15,17,18,44,45]. Given the current LVK localization volume in the sky, if AGNs indeed host the observed BBH mergers, the possible EM counterpart of a single GW event should be found among hundreds or thousands of known AGNs [29]. ...

Current observations are insufficient to confidently associate the binary black hole merger GW190521 with AGN J124942.3+344929

... (a) Posterior distribution on the ellipticity in the Bayesian search15 . Each method's 95% upper limit is drawn as a vertical line, and lies below the spin-down limit, indicating that the spin-down limit has been surpassed for this pulsar. ...

Gravitational-wave Constraints on the Equatorial Ellipticity of Millisecond Pulsars
  • Citing Article
  • October 2020

The Astrophysical Journal Letters

... It consists (in its final configuration) of a battery of four (now two) 1.8 m f/4.4 Wynne-Cassegrain telescopes combined to reach a FOV of 7 deg 2 . On a similar line, project GOTO (Dyer et al. 2020(Dyer et al. , 2024 aims at searching for GW-optical transients by using a set of eight 40 cm f/2.5 Wynne-Newtonian telescopes, flanked in a common mount to mosaic the sky up to a 44 deg 2 FOV. Celestial transients are also investigated by the LAST project (Ben-Ami et al. 2023 ), using a battery of 48 f/2.2 telescopes of 27.9 cm co v ering up to 355 deg 2 on sky. ...

The Gravitational-wave Optical Transient Observer (GOTO)
  • Citing Conference Paper
  • December 2020

... Each GOTO telescope operates autonomously, while target scheduling is coordinated by a central system located at Warwick University in the UK. 15 A visual representation of the network is shown in Figure 3. The individual telescopes are operated using the GOTO Telescope Control System (G-TeCS), 16,17 with each using a "pilot" control program to issue commands and monitor feedback from individual hardware daemons. The pilots each receive pointings from the central scheduler, which ranks and distributes targets to each telescope. ...

Developing the GOTO telescope control system