Massive stellar black holes: formation and dynamics

Similar documents
The impact of metallicity on the demographics of ULXs

The Maxwell's demon of star clusters

Unravelling the progenitors of merging black hole binaries

The dynamics of neutron star and black hole binaries in young star clusters

Dynamics of Stars and Black Holes in Dense Stellar Systems:

Stellar mass black holes in young massive and open clusters and their role in gravitational-wave generation

arxiv: v1 [astro-ph.ga] 18 Aug 2017

Jongsuk Hong (KIAA) MODEST /06/28. Collaborators: E. Vesperini, A. Askar, M. Giersz, M. Szkudlarek & T. Bulik

Massive star clusters

Massive Stellar Black Hole Binaries and Gravitational Waves

How do black hole binaries form? Studying stellar evolution with gravitational wave observations

Optical/IR Counterparts of GW Signals (NS-NS and BH-NS mergers)

Gravitational Waves from Compact Object Binaries

What have we learned from the detection of gravitational waves? Hyung Mok Lee Seoul National University

arxiv: v1 [astro-ph.he] 3 Jan 2019

A new route towards merging massive black holes

Coalescing Binary Black Holes Originating from Globular Clusters

Gruppo Virgo MiB+PR (PI Bernuzzi) Gruppo Virgo TO (PI Nagar)

arxiv: v1 [astro-ph.sr] 19 May 2015

Ultraluminous X-ray Sources forming in low metallicity natal environments

Investigating Ultraluminous X-ray Sources through multi-wavelength variability, broadband spectra, and theoretical modelling

Insights into binary evolution from gravitational waves

Chemical Evolution and the Mass Function of Stellar Mass Black Holes

Long Gamma Ray Bursts from metal poor/pop III stars. Sung-Chul Yoon (Amsterdam) Norbert Langer (Utrecht) Colin Norman (JHU/STScI)

Michela Mapelli. N-body techniques for astrophysics: Lecture 1 General Introduction

Stellar Black Hole Binary Mergers in Open ClusterS

The Evolution of Stellar Triples

A synthetic model of the gravitational wave background from evolving binary compact objects

Open problems in compact object dynamics

Formation Processes of IMBHs

Ultraluminous X-ray Sources: The most extreme X-ray binaries

Binary black holes: formation scenarios and merger rates

Supernova Explosions and Observable Consequences

Forming Intermediate-Mass Black Holes in Dense Clusters Through Collisional Run-away

Fundamental Physics, Astrophysics and Cosmology with ET

Binary sources of gravitational waves

Can black holes be formed in dynamic interactions in star clusters?

GW170817: Observation of Gravitational Waves from a Binary Neutron Star Inspiral

Pulsars as probes for the existence of IMBHs

Dancing in the dark: spotting BHS & IMBH in GC

arxiv: v1 [astro-ph.he] 7 Sep 2017

Dynamics of Stars and Black Holes in Dense Stellar Systems:

Distinguishing source populations. with LIGO/VIRGO

High-energy follow-up studies of gravitational wave transient events

Black Hole Subsystems in Galactic Globular Clusters: Unravelling BH Populations in GCs using MOCCA Star Cluster Simulations

Matt Brorby (U of Iowa) with Philip Kaaret (U of Iowa) Illustration: NASA/CXC/M.Weiss

Monte Carlo Models of Dense Star Clusters

Cosmology with Gravitational Wave Detectors. Maya Fishbach

Lecture 8: Stellar evolution II: Massive stars

Gravitational Waves. Masaru Shibata U. Tokyo

GRAVITATIONAL WAVE ASTRONOMY

INITIAL POPULATIONS OF BLACK HOLES IN STAR CLUSTERS

The origin of the coalescing compact object binaries

The Theory of Supernovae in Massive Binaries

Nuclear astrophysics with binary neutron stars

arxiv: v1 [astro-ph.he] 11 Jul 2016

FORMATION AND EVOLUTION OF COMPACT BINARY SYSTEMS

arxiv:astro-ph/ v1 17 Apr 1999

Probing the Creation of the Heavy Elements in Neutron Star Mergers

2 Ivanova, Fregeau, & Rasio

arxiv: v1 [astro-ph.he] 5 Dec 2016

Formation and cosmic evolution of supermassive black holes. Debora Sijacki

Ultra-stripped Type Ic supernovae generating double neutron stars

HSIN-YU CHEN. ERC 454, 5640 South Ellis Ave. Chicago, IL (515)

A Detailed Look at Cas A: Progenitor, Explosion & Nucleosynthesis

Theoretical Supernova Modeling: Exploring the Progenitor-Explosion-Remnant Connection by Neutrino-Driven Explosion Models

Dynamics of star clusters containing stellar mass black holes: 1. Introduction to Gravitational Waves

Modeling Chemically Homogeneous Evolution in COMPAS

Compact Binaries - 3 ASTR2110 Sarazin

LIGO Detection of Gravitational Waves. Dr. Stephen Ng

Black Hole Subsystems in Galactic Globular Clusters: Unravelling BH Populations in GCs using MOCCA Star Cluster Simulations

Double-core evolution and the formation of neutron star binaries with compact companions

Gamma-ray nucleosynthesis. Predictions - Gamma-ray nuclei - Production sites Observations - Point sources - Diffuse emission

Stars and their properties: (Chapters 11 and 12)

Blue Straggler Formation in Clusters

LISA: Probing the Universe with Gravitational Waves. Tom Prince Caltech/JPL. Laser Interferometer Space Antenna LISA

Lecture 13: Binary evolution

Nobuya Nishimura Keele University, UK

Compact Binaries as Gravitational-Wave Sources

Why is star formation correlated with molecular gas? Simon Glover

MODEST-8. Introduction to MUSE. Steve McMillan

Searching for gravitational waves. with LIGO detectors

A complete sample of bright Swift short GRBs

ON THE MAXIMUM MASS OF STELLAR BLACK HOLES

Gravity. Newtonian gravity: F = G M1 M2/r 2

White dwarf populations. Gijs Nelemans Radboud University Nijmegen

The Origin of Supermassive Black Holes. Daniel Whalen. McWilliams Fellow Carnegie Mellon

New Scenario for IMBH Formation in Globular Clusters - Recent Developm. Observational Imprints

Cooling, dynamics and fragmentation of massive gas clouds: clues to the masses and radii of galaxies and clusters

Science Olympiad Astronomy C Division Event MIT Invitational

LECTURES on COLLISIONAL DYNAMICS: 4. HOT TOPICS on COLLISIONAL DYNAMICS

Black holes in dormant X-ray transients

arxiv: v1 [astro-ph.he] 20 Jul 2015

Synergy with Gravitational Waves

Lobster X-ray Telescope Science. Julian Osborne

Stellar collisions and their products

Dr G. I. Ogilvie Lent Term 2005 INTRODUCTION

Gravitational Wave Detectors: Back to the Future

1 Searching for Optical counterparts of Gravitational

arxiv:astro-ph/ v1 18 Dec 2003

Transcription:

Michela Mapelli INAF-Osservatorio Astronomico di Padova FIRB 2012 fellow MERAC 2015 prize 8 Massive stellar black holes: formation and dynamics Collaborators: Mario Spera, Sandro Bressan, Brunetto Ziosi, Marica Branchesi, Alessandro Trani, Elisa Bortolas, Paolo Esposito, Luca Zampieri Roma, April 11th 2016

OUTLINE: 1. the masses of GW150914: why are they important? 2. the main ingredients: stellar winds and direct collapse 3. dynamics plays `gooseberry' 4. what has been done? 5. what has still to be done? 5. technical issues!

1. the masses of GW150914: why are they important? GW150914 shows that 1. BH-BH binaries exist 2. they can merge in a Hubble time BH BH 36 (+5,-4) Msun 29 (+4,-4) Msun Abbott+2016a,b,c.. 3. massive stellar BHs exist i.e. stellar BHs with mass >25 Msun (Mapelli+ 2009)

1. the masses of GW150914: why are they important? Massive stellar BHs exist i.e. stellar BHs with mass >25 Msun (Mapelli+ 2009) Dynamical mass measurements of ~10 BH masses in MW X-ray binaries compilation from Orosz+ 2003, Ozel+ 2010

1. the masses of GW150914: why are they important? Massive stellar BHs exist i.e. stellar BHs with mass >25 Msun (Mapelli+ 2009) Dynamical mass measurements of ~10 BH masses in MW X-ray binaries compilation from Orosz+ 2003, Ozel+ 2010

2. the main ingredients: stellar winds and direct collapse THEORETICAL MODELS of BH MASS DEPEND ON: 1. STELLAR WINDS: Massive stars (>30 Msun) might lose >50% mass by winds Stellar wind models underwent major upgrade in last ~10 yr (Vink+ 2001, 2005; Bressan+ 2012; Tang, Bressan+ 2014; Chen, Bressan+ 2015) Mass loss depends on metallicity 2. SUPERNOVA: Direct collapse: if final mass of star >30-40 Msun there is no supernova and most star mass becomes BH (Fryer+ 1999, 2001; Heger+ 2003; Mapelli+ 2009) 1. + 2. = METAL-POOR STARS PRODUCE MORE MASSIVE BH

2. the main ingredients: stellar winds and direct collapse Heger et al. (2003)

2. the main ingredients: stellar winds and direct collapse Z= 0 Z= Z 100 30 END ENDMASS MASS[M ] [M ] END MASS [M ] 30 10 3 30 10 10 3 30 100 ZAMS MASS [M ] NO mass losses FINAL MASS FAILED SN SN 30 30 100 100 ZAMS MASS [M ] My cartoon from Heger et al. (2003)

2. the main ingredients: stellar winds and direct collapse What about intermediate metallicity between zero and solar? Model Stellar Evolution Supernova Model Max. BH mass at Z~0.01 Zsun MM+ 2009 Maeder+ 1992 Fryer+ 1999 ~50 Msun MM+ 2010 Portinari+ 1998 Fryer+ 1999 ~80 Msun Belczynski+ 2010 Hurley+ 2000 and Vink+ 2001 Fryer+ 1999 ~80 Msun Fryer+ 2012 Hurley+ 2000 and Vink+ 2001 Fryer+ 2012 ~80 Msun MM+ 2013,2014 Spera, MM & Bressan 2015 SeBa (Portegies Zwart+ 2001) and Vink+ 2001 PARSEC (Bressan+ 2012; Tang, Bressan+ 2014; Chen, Bressan+ 2015) O'Connor+2011 Fryer+ 2012 Ertl+ 2015 (6 different SN models compared) ~85 Msun ~130 Msun

2. the main ingredients: stellar winds and direct collapse What about intermediate metallicity between zero and solar? PARSEC stellar evolution (Tang, Bressan+ 2014; Chen, Bressan+ 2015) + delayed SN model (Fryer+ 2012) Spera, MM & Bressan 2015 used as fig.1 by Abbott+ 2016 paper on Astrophysical implications of LIGO detection

3. dynamics plays `gooseberry' LIGO observed a BH-BH BINARY How do BH-BH (or BH-NS, NS-NS) binaries form? 1) PRIMORDIAL BINARY 2) DYNAMICALLY FORMED BINARY

3. dynamics plays `gooseberry' LIGO observed a BH-BH BINARY How do BH-BH (or BH-NS, NS-NS) binaries form? 1) PRIMORDIAL BINARY: 2 stars form from same gas cloud and evolve into 2 BHs NOT SO EASY: mass transfer, common envelope, SN kicks CE phase BH+MS IS THE ENVELOPE EJECTED? envelope YES BH-BH can form NO cores merge to single BH Studied via POPULATION SYNTHESIS CODES: integration of ISOLATED binaries (Starlab, Portegies Zwart+ 2001; MM+2013; BSE, Hurley+ 2002; StarTrack, Belczynski+ 2010; SEVN, Spera+ 2015)

3. dynamics plays `gooseberry' LIGO observed a BH-BH BINARY How do BH-BH (or BH-NS, NS-NS) binaries form? 2) DYNAMICALLY FORMED BINARY: 2 BHs enter a binary dynamically only in dense clusters, but stars form in dense clusters >90% BH-BH binaries form dynamically in star clusters Exchanges favour formation of massive BH-BH binaries (Ziosi, MM+ 2014)

3. dynamics plays `gooseberry' LIGO observed a BH-BH BINARY How do BH-BH (or BH-NS, NS-NS) binaries form? 2) DYNAMICALLY FORMED BINARY: Requires N-body simulations of star clusters coupled with stellar evolution GPU simulations MM+ 2013, 2014, Ziosi, MM+ 2014, MM 2016, Kimpson+ 2016

3. dynamics plays `gooseberry' LIGO observed a BH-BH BINARY How do BH-BH (or BH-NS, NS-NS) binaries form? 2) DYNAMICALLY FORMED BINARY: Chirp masses of BH-BH systems accounting for both primordial and dynamical binaries From Ziosi, MM+ 2014 GW150914 0.01 Zsun 0.1 Zsun 1 Zsun

4. what has been done? OUR TEAM @ INAF: http://web.pd.astro.it/mapelli/group.html funded ONLY by COMPETITIVE GRANTS (FIRB, PRIN, MERAC) 1. most up-to-date model for the mass of BHs, used by the LIGO collaboration to constrain Z: WE PREDICTED MASSIVE BHs before LIGO detection 2. we investigate the dynamical processes: We found that 90% BH-BHs form DYNAMICALLY MM+ 2009, 2010, 2013; MM & Zampieri 2014; Ziosi, MM, Branchesi, Tormen 2014; Spera, MM & Bressan 2015

4. what has still to be done (for discussion)? EVERYTHING SOLVED? NO: we can just reject models with BH mass < 20 Msun OPEN QUESTIONS for THEORISTS @ INAF: STELLAR EVOLUTION: uncertainties in supernova model binary evolution contains free parameters (COMMON ENVELOPE is the black beast) DYNAMICS: initial conditions might be wrong (NO GAS, few primordial binaries!!!) role of mergers between stars (runaway collision scenario) processes as Spitzer's instability and Kozai not investigated can change the merger rate by orders of magnitude ELECTROMAGNETIC COUNTERPARTS: our study focussed on BHs, still low statistics for NSs how many EM counterparts do we expect and what are they?

5. technical issues (for discussion) Dynamical simulations are computationally expensive: 1 BH-BH merger every ~ 100 simulated star clusters Each simulation requests ~ 100 GPU hours 10 000 GPU hours for a single MERGER!!! RESOURCES: We have a 64 core machine @ OAPD (FIRB2012 project) We obtain more time @ CINECA via competitive proposals, but CINECA decides what clusters to buy (these are often non-suitable x astro people) WE NEED MORE COMPUTATIONAL FACILITIES TO REMAIN COMPETITIVE!!!! Tier 1 machine @ INAF : a crazy thing? Can be used by theorists and observers x data- analysis

Our team: http://web.pd.astro.it/mapelli/group.html Mario Spera Brunetto Ziosi Elisa Bortolas Alessandro Trani MAN POWER: we are a small group @ INAF-Padova funded ONLY by COMPETITIVE GRANTS (FIRB, PRIN, MERAC) (1 staff member, 1 postdoc, 2 PhD students, 1 ex-phd student + several collaborators @ INAF and other institutes)

Conclusions After LIGO, we know that BH-BH exist, merge in a Hubble time, and that MASSIVE BHs (>25 Msun) exist Massive BHs have been successfully predicted by a INAF team: we have the expertise @ INAF We are not alone @ INAF: see next talk by Marco Limongi Understanding massive BHs requires models of stellar evolution, binary evolution and DYNAMICS of stellar objects: INTERDISCIPLINARY AND COMPLEX Future challenges include: full description of dynamics, understanding common envelope, formation of NS-NS For the discussion: models of double compact-object binaries require COMPUTING TIME with GPUs THANK YOU!!!

From Spera et al. 2015 based on SN model by Ertl et al. 2015 M4 is the mass enclosed within radius where dimensionless entropy per baryon is 4 2 parameters: M4 and the compactness of Fe core

From Fig. 10 Spera et al. 2015 Comparison of 5 SN models at Z=0.002=0.1 Zsun (consistent with GW150914)

From Fig. 13 Spera et al. 2015 Comparison of 3 stellar evolution models at Z=0.002=0.1 Zsun (consistent with GW150914)

5. technical issues! Dynamical simulations are computationally expensive 1 BH-BH merger every ~ 100 simulated star clusters parameter space investigation is missing Each simulation requests > 2 weeks on CPUs ~ 1 100 hr on GPUs We have a 64 core machine @ OAPD (18k euro from FIRB2012 project) CINECA: high success rate of proposals but CINECA decides what clusters to buy (not suitable to astro people) WE NEED MORE COMPUTATIONAL FACILITIES TO BE COMPETITIVE!!!! Tier 1 machine @ INAF : a crazy thing? ~1-2 M EUR first investment (obsolescence ~ 5 yr) ~100k EUR maintenance /yr Can be used by theorists and observers x data- analysis