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Title: Gravitational Wave Astrophysics, Compact Binaries, and Numerical Relativity


1
Gravitational Wave Astrophysics, Compact
Binaries, and Numerical
Relativity
  • Joan Centrella
  • Gravitational Astrophysics Laboratory
  • NASA/GSFC

Numerical Relativity 2005 Compact Binaries
November 2 4 , 2005
2
Most of the information we have about the
Universe so far has come to us in the form of . .
.
  • Electromagnetic radiation
  • Visible light naked eye observations,optical
    telescopes
  • Full electromagnetic spectrum radio, IR, UV,
    visible, X-rays, Gamma-rays
  • Particle nuclear astrophysics, neutrinos,
    cosmic rays

These cosmic messengers provide a wealth of
information, making astronomy one of the crowning
glories of 20th century science.
3
A Different Type of Astronomical
MessengerGravitational Waves . . .
  • Hulse-Taylor binary pulsar PSR 191316
  • Orbital period decay agrees with GR to within the
    obs errors of lt 1
  • Nobel Prize 1993
  • ripples in spacetime curvature
  • travel at velocity v c
  • generated by matter distributions w/
    time-changing quadrupole moments
  • ? carry info about bulk motion





    of sources
  • transverse ? act normal to propagation direction
  • 2 polarization states, h and hx
  • interact weakly with matter
  • ? carry info about deep, hidden regions in the
    universe

4
Amplitudes of Gravitational Wave Sources . . .
  • Characteristic amplitude
  • r distance to source
  • RSch 2GM/c2
  • Q (trace-free) quadrupole moment of source
  • v characteristic nonspherical velocity
    in source
  • Estimate upper limits
  • 1.4 MSun NS at
  • r 15 kpc, h 10-17
  • r 15 Mpc, h 10-20
  • r 200 Mpc, h 10-21
  • r 3000 Mpc, h 10-22
  • 4 x 106 Msun MBH at
  • r 3000 Mpc, h 10-16
  • Strongest sources have
  • large masses moving
  • with velocities v c

5
Detecting gravitational waves. . .
  • Resonant mass detectors, laser interferometers
  • Detector of length scale L
  • A passing gravitational wave causes distortion of
    detector that produces a strain amplitude h(t)
    ?L/L
  • Source waveforms scale as h(t) 1/r

(graphic courtesy of B. Barish, LIGO-Caltech)
6
Estimating Gravitational Wave frequencies . . .
  • Binary orbital frequency
  • M M1 M2, M1 M2
  • a separation
  • NS/NS, a 10 R
  • fGW 200 Hz
  • BH/BH, a 10 M
  • fGW 100 Hz
  • MBH/MBH, a 10 M
  • fGW 3 x 10-4 Hz
  • Natural frequency
  • 1.4 MSun NS, R 10 km
  • fo 2 kHz
  • 10 MSun BH
  • fo 1 kHz
  • 4 x 106 MSun MBH
  • fo 3 mHz

7
Ground-based interferometers . . .
  • detect high frequency GW
  • broad band
  • kilometer-scale arms
  • Current projects
  • LIGO Hanford, WA, and Livingston, LA L 4
    km
  • VIRGO France/Italy, near
    Pisa L 3 km
  • GEO600 Germany/Britain, Hanover L 600 m
  • Typical sources NS/NS, NS/BH, BH/BH, stellar
    collapse, LMXBs...

8
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9

10
  • Significant progress in ground-based GW
    detectors....
  • LIGO
  • has a set of running detectors
  • data analysis process has matured
  • the main initial LIGO science run S5
  • to take 1 full year of integrated data
  • set to begin later this year
  • reorganization of LIGO lab and LSC into a single
    LIGO
  • Advanced LIGO upgrade
  • showing good technical progress
  • optimistic about starting funding from NSF in
    2008
  • VIRGO, GEO600
  • also progressing
  • ? the age of GW observations is beginning in
    earnest!

11
LISA Laser Interferometric Space Antenna
  • NASA/ESA collaboration
  • detect low frequency GW
  • 3 spacecraft
  • equilateral triangle
  • orbits Sun at 1 AU
  • 20o behind Earth in its orbit
  • arm length L 5 x 106 km
  • optical transponders receive and re-transmit
    phase locked light
  • launch 2015
  • Typical sources MBH/MBH, Galactic compact
    binaries, NS/MBH, BH/MBH

12
Recent LISA Accomplishments
  • The LISA Project has been in the Formulation
    Phase one year.
  • ESA has engaged a contractor for formulation
    studies. The Architecture Definition Phase of
    that contract is complete.
  • The LISA Project team has mapped out 35 design
    studies, 13 are done, 5 are ongoing, and the rest
    to be finished by Apr. 06.
  • LISA Pathfinders major milestone, the
    Preliminary Design Review, is nearly complete.
    ESAs LISA Test Package has built and tested
    engineering models. NASAs ST-7 has built and
    tested engineering models.
  • Ground-based technology development is
    progressing on microthrusters, phasemeter,
    lasers, etc.
  • LISA data analysis planning has started both in
    the U.S. and Europe.

13
Gravitational Reference Sensor
Engineering model of the gravitational reference
sensor for LISA Pathfinder
14
Interferometry
Engineering model of the interferometer for LISA
Pathfinder
15
LISA / LIGO Relationship
  • Complementary observations, different frequency
    bands
  • Different astrophysical sources

16
Astrophysical black holes....
  • Black holes are formed throughout the universe as
    the extreme end states of collapse, accretion,
    mergers....
  • There is good evidence for BHs in 3 mass ranges
  • massive black holes (MBHs) M 105 Msun
  • intermediate mass black holes (IMBHs) 102 Msun
    M 104 Msun
  • stellar black holes M 102 Msun
  • BHs are powerful cosmic engines, heating and
    accelerating gas and particles to produce
    impressive displays of electromagnetic energy...
  • When occuring in a binary, BHs are also
    prodigious sources of gravitational waves....

17
Massive Black Holes...first found in active
galaxies..
  • M87 giant elliptical galaxy with jet
  • Cyg-A radio source jet extends
    7 x 105 ly

VLA(top left), HST (top right), VLBI (bottom)
(NASA,NRAO/NSF,STScI/JHU, AUI)
optical (AURA/NRAO/NSF)
(NRAO/AUI)
18
Massive Black Holes....
  • Good evidence for massive dark objects with
    masses 106 Msun lt M lt
    1010 Msun at centers of few dozen galaxies
  • Based on dynamical models, the case for these
    massive dark objects being MBHs is tight for 3
    galaxies...
  • MBH masses correlate with bulge luminosity (left)
    and velocity dispersion (right)

    (Ferrarase Ford 2005)
  • MBH s4 5
  • LISA observations of GW from compact objects
    inspiralling into these objects can falsify the
    hypothesis that they are actually Kerr BHs

19
MBH/MBH binaries.
  • MBHs at the centers of most, if not all, galaxies
  • Most galaxies undergo at least one merger
  • ? MBH binaries
  • Coalescence of MBH binary depends on stellar
    effects, gas, feedback....
  • Chandra X-ray observatory found the first known
    system of 2 MBH starting to merge in the galaxy
    NGC 6240
  • distance 120 Mpc ? close!
  • BHs will merge in few x 108 yrs
  • LISA could observe several tens per year, out
    to redshifts z gt 5 or more

20
Evidence for MBH mergers....
  • Jets emanating from centers of active galaxies
  • believed to result from accretion onto central
    MBH
  • jet directed along spin axis
  • Mergers of spinning BHs can change orientation of
    BH spin axis
  • ? sudden flip in jet direction
  • X-type radio sources may be
    signature
    of MBH merger

(Image courtesy of NRAO/AUI Inset STScI)
(Merritt Ekers, Science, 2002)
21
IMBHs....X-ray sources in dense stellar clusters
  • M82 active star-forming galaxy ?
  • many young, dense stellar clusters luminous
    X-ray sources (ULXs)
  • associate cluster MGG 1 w/ ULX M82 X-1 (near
    center of image)
  • Identify this w/ IMBH of mass M 350 Msun
    (Portegies Zwart, et al)
  • M74 Optical image w/ Chandra X-ray image
    overlaid
  • Sc spiral galaxy with ULX
  • ULX is IMBH candidate

(Optical NOAO/AURA/NSF/T.Boroson X-ray
NASA/CXC/U. of Michigan/J.Liu et al.)
22
IMBH/IMBH binaries.
  • IMBHs can form in dense stellar clusters (Miller,
    Freitag,...)
  • stellar dynamics
  • collisions
  • core collapse of cluster
  • runaway ? form IMBH
  • Can gt 1 IMBH form in a stellar cluster?
  • recent simulations by John Fregeau and
    collaborators find multiple sites for runaway to
    occur in clusters
  • ? multiple IMBHs form, with comparable masses
    m1/m2 lt 10
  • LISA could see as many as several inspirals per
    year, for masses in the range M few x 100 Msun
    103 Msun
  • Advanced LIGO could see binaries with masses in
    the range M (10s 100s)Msun

23
Stellar Black Holes.
  • Form as the end result of massive star evolution
  • Type II supernova
  • collapse of iron core in highly evolved massive
    star
  • outer regions blasted away in supernova explosion
  • core collapses to BH if mass of remnant core M gt
    3 Msun (maximum mass of NS)
  • Evidence for BH strongest in low mass X-ray
    binaries (LMXBs)
  • interacting binary systems with compact object
    and companion star
  • accretion of material from companion onto compact
    object ? X-rays
  • in 17 cases, compact object has
    mass M
    gt 3 Msun ? BH (Orosz)
  • BH/BH binary
  • forms if companion evolves to BH w/out
    disrupting binary
  • no gas ? no EM emission
  • but...detectable by GWs
  • Source for ground based detectors....

(Ihle 2004)
24
Final coalescence of BH binary proceeds in 3
stages . . .
  • GW produced in all three phases of this evolution
    . . .
  • Waveforms and dynamics scale with BH masses and
    spins
  • ? source modeling applicable to
  • stellar BHs, IMBHs MBHs.

strong-field spacetime dynamics, spin flips and
couplings
measure masses and spins of binary BHs
detect normal modes of ringdown to identify final
Kerr BH
(graphic courtesy of Kip Thorne)
25
Focus on the merger stage
  • Inspiral lasts until last stable orbit (LSO)
    ...then BHs leave quasi-static orbits
    and plunge together
  • Need to evolve BH binary for few orbits near
    the LSO at the end of the inspiral,
    through merger and ringdownand extract the GW
    signature
  • Expect several cycles of gravitational
    radiation from merger
  • burst waveform, observable by LISA for
    minutes hours
  • Strong, highly nonlinear, dynamical gravitational
    fields
  • Importance of astrophysical initial data...
  • Requires numerical solution of full Einstein eqs
    in 3-D time
  • Merger can be phenomenologically rich
  • effects of spin spin-spin and spin-orbit
    couplings, spin flips
  • test of GR in the dynamical, nonlinear regime
  • possible ejection of final BH for M1 ? M2 ?
    astrophysics

26
What powers short Gamma-ray bursts?
  • Gamma-Ray Bursts (GRBs) come in 2 types long (gt
    2 sec) and short
  • The burst is followed by a fainter, longer lived
    afterglow
  • By observing their afterglows, long GRBs are
    associated with the collapse of young, massive
    stellar cores
  • Recent observations by HETE Swift allowed fast
    and precise localization of X-ray afterglows of
    some short GRBs
  • Left GRB 050509b observed by Swifts ?-ray
    (blue) X-ray (red) instruments
  • Right GRB 050724 observed by Swifts X-ray
    telescope (red) and the small circles and crosses
    are from optical, X-ray (Chandra) and radio
    observations

27
Short GRBS....NS/NS and NS/BH mergers?
  • These observations of short GRBs are consistent
    with models of NS/NS or NS/BH mergers
  • Such events would also produce GWs that could be
    detectable by ground-based detectors such as LIGO
  • Can tell us about the populations of such
    compact binaries, and the GRB mechanisms
  • Will look for coincidences between Swift and
    HETE events and possible GW signals during the
    upcoming S5 science run

(Nature)
28
Gravitational Waves . . . a new kind of cosmic
messenger
  • Every time you build new tools to see the
    universe, new universes are discovered. Through
    the ages, we see the power of penetrating into
    space.

-- David H. DeVorkin (paraphrasing Sir William
Herschel)
29
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