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Opening our ears to short gravitational-wave bursts in the third LIGO–Virgo observing run

Dated 09 July 2021. Read this summary in PDF format (in English) and in other languages: Italian .


The third observing run (O3) of the Advanced LIGO and Advanced Virgo detectors ended in March 2020. During O3 several tens of Gravitational Waves (GWs) have been confirmed, originating from the compact binary coalescence (CBC) of Black Holes and/or Neutron Stars. However, CBCs are only one type of GW sources among a wider range of possibilities. Here we focus on a type of GW transients that have particularly short time duration (less than 1 second): we also call these “short bursts”. Potential examples of short burst sources (besides binary black hole mergers) include core-collapse supernovae, cosmic string cusps, or pulsar glitches — as well as the exciting possibility of totally new unpredicted sources.

Unmodeled Searches

Given the lack of precise models for most of these potential sources, it is important to process the data with algorithms capable of detecting almost any type of signal, as long as it is short: this is a so-called “unmodeled” short-duration transient search. Compared to the dedicated CBC search approach, where we search in the data for features corresponding to known waveform ‘templates’, an unmodeled search extracts excesses in the data which could be compatible with GWs satisfying minimal assumptions. However, the downside to this unmodeled approach is that these search algorithms are limited by the presence of noise artifacts (detector glitches - not to be confused with pulsar glitches) in the data, which can resemble a genuine GW signal. Thanks to the information from auxiliary channels, which monitor the external and internal state of the interferometers, a large fraction of these detector glitches can be identified and vetoed. This helps to improve the statistical significance of possible candidates.

Two search algorithms have been considered for this work: coherent Waveburst (cWB) extracts a list of GW signal candidates from the data, and BayesWave (BW) performs a follow-up analysis of the cWB candidates. The two algorithms have been tested on a set of ad-hoc simulated waveforms where a few different generic signal ‘shapes’ have been added to the data to determine how energetic a GW must be to be observable by our detectors.

Results

Figure 1 shows the list of candidates from the search, compared with the expected distribution in the case where they come from noise excesses. The predicted distribution is obtained with the widely used procedure of time-shifting detector data. No new GW candidates have been found, apart from some of the already detected CBC sources (the ones that imprint a short-duration signal in the data, corresponding to massive compact objects). While in the previous runs we characterized the sensitivity of similar searches by considering ad-hoc generic waveforms, in this work we additionally investigate how well the search is able to detect two specific possible astrophysical sources: core-collapse supernovae (CCSN) and isolated neutron stars (NS).

Figure 2 shows the distance ranges from Earth within which our searches would detect a CCSN with an efficiency between 10 and 50%, depending on different GW emission models. We also want to know how large a pulsar glitch would need to be, in order to be detected in our data. Figure 3 shows the size of pulsar glitch that could be detected with an efficiency of 50%, assuming various emission models described by different equations of state and considering as a reference the distance and spin of the Vela pulsar.

Find Out More:

Glossary

  • Transient: Astronomical phenomenon with a short timescale, in contrast to other, typical astrophysical events which may last from thousands to billions of years. There is a wide range of GW transients. In this search, we are focusing on the shorter duration GW transients.
  • Auxiliary channels: Used to monitor the environmental behaviour around the detector, they register whatever can contribute to identify any disturbances. Some examples are magnetometer or seismometer readings, or monitors recording human activities or weather conditions.
  • Core-collapse Supernova: At the end of a star’s evolution, after the production of elements heavier than hydrogen through nuclear fusion, a star of mass larger than 8 times the Sun collapses under its own gravity. This process heats the surface and creates a shock propagating outward from the star. This shock may eventually break up the star’s envelope leading to an explosion.
  • Neutron star: A collapsed core of a dead star, typically around 1.4 times the mass of our Sun with a radius of about 10 km.
  • Equation of State: The internal structure of a NS can be described by the Equation of State, which tells us about the relationship between pressure and density inside the NS. Since we still do not know what is the precise internal structure of these objects, we use different models of the equation of state to cover several possibilities.
  • Pulsar glitch: A pulsar is a neutron star that has been observed through its pulses of electromagnetic radiation (usually in the radio band). Not all neutron stars can be observed as a pulsar, because they do not emit electromagnetic radiation in the direction of the Earth, or because they do not emit at all. A fraction of the neutron star population is known to show transient glitches, measured by electromagnetic observations of pulsars. The two most-explored mechanisms in the literature for these pulsar glitches are star quakes and superfluid-crust interactions.
  • Time-shift analysis: Standard method in gravitational-wave science to assess the confidence of a candidate. It is performed by applying different time-shifts between the data streams from two or more detectors. Eventual triggers coming from this time-shifts analysis are generated by accidental coincidences and they resemble the statistical distribution of the candidates in the original data (not shifted). Repeating these time-shifts a huge number of times allows us to increase the confidence on the significance assessment.
  • Cosmic String: Hypothetical one-dimensional objects that may have formed in the early Universe, while it was cooling down and expanding.
  • Cusp: A fixed point on a curve at which a point tracing the curve would exactly reverse its direction of motion.
  • Waveform: Representation of how a gravitational-wave signal varies with time.
  • Sensitivity: A way of describing a detector's ability to detect a signal. Detectors with lower noise are able to detect weaker signals and therefore are said to have higher (or greater) sensitivity.
  • Vela Pulsar: A pulsar located in the constellation of Vela, remnant from a Supernova explosion.
  • Parsec (pc): A unit of distance largely used in astronomy. It corresponds approximately to 31 trillion kilometres.

Figures from the publication

You can click on each figure for a larger version. For more information on how these figures were generated and their meaning, see the scientific article.

cumulative number of events at different inverse false alarm rates

Figure 1 (figure 2 in the paper): Cumulative number of events (vertical axis) shown against the probability of being generated randomly by noise excesses (expressed as inverse false alarm rate in years, horizontal axis). Two sets of symbols connected with lines show the total number found by the search (circular points) and after having discarded all known CBC sources from the data (triangular points). The solid line represents the expected noise-only background and shaded regions indicate its statistical uncertainty.

sensitive distances for detecting different CCSN waveforms

Figure 2 (figure 7 in the paper): Distances of a source from Earth at which our algorithms can detect different CCSN waveforms. The left edge of each box refers to the distance (in thousands of parsecs, denoted kpc) at which we detect 10% of the signals, while the right edge shows the distance corresponding to 50% efficiency. The vertical axis refers to different CCSN waveforms; see the paper for more details on the models considered. Different colors represent results from the two detection algorithms used.

sizes of pulsar glitches that we could detect

Figure 3 (figure 8 in the paper): This shows the size of a pulsar glitch that could be detected at 50% efficiency by our analysis. This is calculated with reference to a Vela-like pulsar — i.e. considering a fixed distance of 287 parsec and a spin (rotation around the neutron star’s own axis) frequency of around 11 Hz. The horizontal spread of the boxes represents the variation in the size of pulsar glitch when the different possible mass ranges for the neutron star, as shown on the corresponding vertical axis, is taken into account. Two extreme equations of state are considered: soft (APR4) and hard (H4). More details about these two different equations of state can be found in the scientific publication.

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