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Gravitational and multimessenger after the observation of a merger

Tito Dal Canton

XXXVIII International Symposium on Physics in Collision Bogotá, 2018 Contents

● Theory, instruments and methods

● Current results

● Near and long-term future

2 Multimessenger astronomy

Radio Infrared Optical Ultraviolet X-rays γ-rays

Matter, composition, chemistry, temperature

Supernova SN1987A Cosmic rays

Nuclear reactions, decays

Gravitational waves

Motion/geometry, regardless of composition 3 Gravitational waves

1 8 G π Radiation from Rμ ν− R gμ ν= 4 T μ ν 2 c accelerated motion: G Q¨ T μ ν=0 h ∼ ij c4 r gμ ν=ημ ν+hμ ν

|ημ ν|≪1

Black hole & neutron star binaries

Collapse of stellar cores

Rotating neutron stars

Decay of Hulse-Taylor binary

4 The instruments of GW astronomy

LIGO

Observable quantity: strain h = ΔL/L

Astrophysical signals h < 10-21

5 Virgo The instruments of GW astronomy

Amplitude spectral density of detector noise (Aug 2017)

Less sensitive

More sensitive

PRL 119, 141101 (2017)

6 Analysis of GW data

Transient signals (< ~1 min) Continuous signals (> ~1 day)

Robust analytic/numerical Deterministic waveform model (e.g. rotating neutron stars) (e.g. mergers)

Stochastic No waveform model - yet (e.g. superposition (e.g. stellar core collapse) of incoherent signals)

Time-frequency decompositions, excess power above noise Correlation (coincident or coherent)

Matched filtering Bayesian inference for parameter estimation (coincident or coherent) 7 Detecting compact binary mergers

Compact binary merger template waveform Template bank

Matched filtering

Instrumental transient

8 Organizing multimessenger observations

Fermi/GBM INTEGRAL Low-latency detection (e.g. GW) LIGO/Virgo Overlap in time / sky location Gamma-ray coordinates network / Low-latency detection (e.g. GRB) Transient astronomy network Low-latency detection (e.g. GRB) MASTER Swift-BAT IceCube Targeted followup (e.g. optical)

TITLE: GCN CIRCULAR NUMBER: 23153 SUBJECT: GRB 180818B: Fermi GBM observations DATE: 18/08/18 23:14:07 GMT FROM: Peter Veres at UAH Blind deep search (e.g. GW) P. Veres (UAH), C. Meegan (UAH) and A. von Kienlin (MPE) report on behalf of the Fermi GBM Team:

"At 12:28:57.24 UT on 18 August 2018, the Fermi Gamma-Ray Burst Monitor triggered and located GRB 180818B (trigger 556288142 / 180818520). Overlap in time / sky location which was also detected by the Swift/BAT (Marshall et al., GCN 23149). The GBM on-ground location is consistent with the Swift position. 9 […] Blind deep search (e.g. GRB) Contents

● Theory, instruments and methods

● Current results

● Short- and long-term future

10 Performance of advanced GW detectors

S/N ~ d-1 & S/N > ~8 to have a detection → Maximum d (range)

Virgo

Number of detected sources 3 ∼d T obs

losc.ligo.org 11 A zoo of mergers Actual data on losc.ligo.org GW151226 GW150914

GW170104 GW170608

SXS collaboration

GW170814

12 Are they really black holes?

● Perfectly match theoretical waveforms

● Waveform shape → Quasi-circular orbit

● df / dt → Limits on masses

● Maximum frequency → Min separation

● Black holes are the only known objects

that can weigh ~10 MSun and orbit at ~100 Hz

● ~1 MSun radiated in GWs and no clear evidence of multimessenger counterparts

13 How heavy are these black holes?

14 Do these black holes spin?

15 Do LIGO/Virgo black holes match x-ray candidates?

Nielsen 2016

Hynes 2010 ??? LIGO/Virgo black holes

16 What created these binary black holes?

Binary Dynamical BH capture with common envelope in dense clusters

?

Primordial BHs decoupling from the background (e.g. arXiv:1801.10327)

Need more events! 17 Testing general relativity with LIGO/Virgo’s black holes

Deviations in post-Newtonian coefficients - arXiv:1606.04856

GW150914, GW151226, GW170104:

−23 Mg ≤ 7.7 × 10 eV from limits on waveform phase deviations Phys. Rev. Lett. 118, 221101 (2017) Pre- and post-merger parameter consistency 18 GW170817: a neutron star merger

Most precisely localized

Loudest

Closest

PRL 119, 161101 (2017) 19 Longest GW170817’s components

Two objects with masses …and no sign of significant spins similar to neutron stars…

20 arXiv:1805.11579 GW170817’s components

Disfavored equations of state Tidal deformability parameter

Two black holes 21 arXiv:1805.11579 170817’s γ-ray burst arXiv:1710.05834

???

● “Ordinary” short GRB on its own

● But knowledge of distance implies it is incredibly dim 22 ● Hard spike + thermal tail 170817’s γ-ray burst

23 arXiv:1710.05834 Fundamental physics with GW170817 and its γ-rays

Two reference events spatially coincident and temporally closer than 10 s:

● End of GW waveform ● Start of γ-ray emission

Propagate over ~1024 m…

Speed of GWs vs Lorentz invariance Equivalence principle

GWs and photons “fall” in the same way

24 arXiv:1710.05834 170817: UV - optical - IR

NGC 4993

25 arXiv:1710.05833 170817: UV - optical - IR

26 arXiv:1710.05833 Kilonova and nucleosynthesis from GW170817

arXiv:1710.05841

a

r

X

i

v

:

1

1

0

8

.

6

0

5

6

Post-merger ejecta expanding at ~0.2 c

Blue → red evolution, rapid cooling

Late spectral features 27 of heavy elements GW170817 as a standard siren for cosmology

GW Luminosity distance

Sky location

H0

Host Redshift NGC 4993 arXiv:1710.05835

Need more events! 28 170817: radio and x-ray afterglow

arXiv:1805.04093 arXiv:1801.06164

● X-ray flux increases, starts fading at ~150 days ● Radio flux follows similar evolution

✗ Off-axis “top-hat” jet arXiv:1803.06853 ✓ Off-axis jet with angular structure 29 ✓ Isotropic outflow model 170817’s non-detections

Neutrinos Post-merger GWs

● IceCube

● ANTARES arXiv:1805.11579

● Pierre Auger Observatory Consistent with off-axis jet

Current sensitivity insufficient for setting constraints

30 A ~300 TeV ν from an active blazar?

● Atmospheric origin not fully excluded ● Chance association rejected at 3σ ● Consistent with long-expected blazar origin of neutrinos

31 arXiv:1807.08816 Theoretical & modeling efforts GW waveforms MM counterparts

Credit: S. Noble

arXiv:1701.08738

arXiv:1806.05697 32 Contents

● Theory, instruments and methods

● Current results

● Short- and long-term future

33 GW astronomy in the near future arXiv:1304.0670v6

34 GW astronomy in the near future

O2 O3 - Feb 2019, ~1 year ● Open public alerts ● End-of-run results papers ● Many more BH-BH mergers ● Binary merger population ● Few to O(10) NS-NS mergers ● Up to a few/year with sGRBs ● Improve tests of GR ● BH-NS mergers? ● Additional ● New sources? multimessenger followup studies ● Supernovæ ● Continuous waves

● Stochastic background

35 Multimessenger astronomy in the near future

Fermi Swift Chandra INTEGRAL XMM-Newton NuStar ZTF TAROT

IceCube CHIME LSST

SVOM ISS-TAO BurstCube arXiv:1708.09292 JWST

36 GW astronomy in the far future

3rd generation ground-based interferometers

Cosmic Explorer (US) Einstein Telescope (EU) ● L-shaped ● Underground ● 40 km arms ● 10 km arms ● Cryogenic? ● Cryogenic

arXiv:1607.08697

● Higher binary merger rates ● SNR > 20 at cosmological redshifts ● Early alert for binary mergers

37 GW astronomy in the far future

Space interferometers – LISA mission

arXiv:1702.00786

38 Phys. Rev. Lett. 120, 061101 Multimessenger astronomy in the far future

ATHENA

TAP

WFIRST

LUVOIR SKA 39 Gracias!

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