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Gravity with the SKA
Michael KramerJodrell Bank ObservatoryUniversity of Manchester
WithDon Backer, Jim Cordes, Simon Johnston,
Joe Lazio and Ben Stappers
Gravity Meeting ’06, Birmingham
Strong-field tests of gravity using Pulsars and Black Holes
Outline• Pulsars• Past and present successes• A giant leap - the power of the SKA• Transforming our knowledge offundamental physics, particularly:
- Strong-field tests of gravity- Gravitational wave astronomy
Searching & Timing: see JimGravitational Waves: see Rick
Testing EinsteinExperiments made in Solar System provide accurate tests
…but only in weak gravitational field!
In strong gravitational fields, physics may be different!
Compute energy in gravitational field:
Radiative aspects need to be tested too!
Neutron stars &Black Holes:
5.015.0
≈≈
BH
NS
εε
2mcEgravity=ε
Solar system:
10000000000.00000000001.0
000001.0
≈≈≈
Moon
Earth
Sun
εεε
Pulsars are extreme objects…• Cosmic lighthouses …• Precise clocks …• Almost Black Holes …• Objects of extreme matter …
– 10x nuclear density– B ~ Bq = 4.4 x 1013 Gauss– Voltage drops ~ 1012 V– FEM = 1010-12 Fg– High-temperature & superfluid superconductor
• Massive stable flywheels superb cosmic clocks e.g. period of B1937+21:
P = 0.0015578064924327±0.0000000000000004 s
Precision tools for a wide range of fundamental physics and astrophysics
Strong-field tests using pulsars…
Various approaches:
Theory-independent or phenomenological:Parameterized Post-Keplerian approach
Parameterized Post-Newtonian (PPN)
Binary pulsars
Theory-dependent:Beyond usual post-Newtonian parameters, used forclasses of tensor-scalar theories
Parametrized post-Newtonian (PPN)γ How much space
curvature per unit mass?1 γ-1<2 10-3
γ-1<3 10-4
Viking ranging (time delay)VLBI (light deflect.)
β How much “non-linearity” in the superposition law?
1 β-1<3 10-3 Perihelion shift
ξ Preferred-location effects? 0 | ξ |<3 10-3 Earth tides, Pulsars
α1Preferred-frame effects?Orbital polarization
0 α1 < 10-4
α1 < 1.2 10-4
Lunar ranging (weak) Pulsars (strong)
α2Preferred-frame effects?Spin precession
0 α2 < 4 10-7 Solar alignment
α3Preferred-frame effects?Violation of conversation of total momentum
0 α3 < 4.0 10-20 Pulsars
Will (2002), Stairs (2005)
Plus: limits on violation of SEP: |Δ|<5.5x10-3
…already a success story:The first binary pulsar
Weisberg & Taylor (2004)
• Orbit shrinks every day by 1cm• Confirmation of existence of gravitational waves
Hulse & Taylor (1974)
Tests of General RelativityElegant method to test any theory of gravity: (Damour & Taylor ’92)
• Relativistic corrections to Keplerian orbits measured
• All corrections can bewritten as function ofthe pulsar masses
• Only one true combination of mA and mB should exist
Single unique point in
a mA - mB diagram!
PK1
PK2PK3
Pass!
Tests of General RelativityElegant method to test any theory of gravity: (Damour & Taylor ’92)
• Relativistic corrections to Keplerian orbits measured
• All corrections can bewritten as function ofthe pulsar masses
• Only one true combination of mA and mB should exist
Single unique point in
a mA - mB diagram!
PK3
PK2
PK1
Fail!
Npk – 2 tests possible
…already a success story: The first double pulsar
Kramer et al. (in prep.)
Orbital Phase (deg)
Del
ay (µ
s)
s = sin(i)=0.9997±0.0002
001.0000.1obs
exp
±=ss
Kramer et al.(in prep)
Testing GR:
• most relativistic systems• most over-constrained system:
• Five PK params• Theory independentmass ratio
“Scalarisation”
…already a success story: Scalar-Tensor Theories
ScalarCharge(for β0=-6)
Damour (priv. comm.)
Damour (priv. comm.)
The is more to do:
• The remaining “holy grail”: a pulsar – black hole system!• Wanted: millisecond pulsar around black hole
“…a binary pulsar with a black-hole companion has the potential of providing a superb new probe of relativistic gravity. The discriminating power of this probe might supersede all its present and foreseeable competitors…”
(Damour & Esposito-Farese 1998)
Galactic Census with the SKA• Blind survey for pulsars will discover PSR-BH systems!• Timing of discovered binary and millisecond pulsars to very high precision:
• “Find them!”• “Time them!”• “VLBI them!”
Benefiting from SKA twice:• Unique sensitivity: many pulsars, ~10,000-20,000
incl. many rare & exotic systems!• Unique timing precision and multiple beams!Not just a continuation of what has been done before
- Complete new quality of science possible!
• Galactic probes: Interstellar medium/magnetic fieldStar formation historyDynamicsPopulation via distances (ISM, VLBI)
Pulsar Science with the SKAVery wide range of applications:
Electrondistribution
Magnetic field
Galactic CentreMovement in potential
• Galactic probes• Extragalactic pulsars: Formation & Population
Turbulent magnetized IGM
Pulsar Science with the SKAVery wide range of applications:
Giant pulses
Reach the local group!
Search nearby galaxies!
• Galactic probes• Extragalactic pulsars• Relativistic plasma physics: Radio emission
Resolving magnetospheresRelation to high-energies
Pulsar Science with the SKAVery wide range of applications:
• Galactic probes• Extragalactic pulsars• Relativistic plasma physics• Extreme Dense Matter Physics: Ultra-strong B-fields
Equations-of-StateCore collapsesVariation of G
Pulsar Science with the SKAVery wide range of applications:
• Galactic probes• Extragalactic pulsars• Relativistic plasma physics• Extreme Dense Matter Physics• Multi-wavelength studies: Photonic windows
Pulsar Science with the SKAVery wide range of applications:
• Galactic probes• Extragalactic pulsars• Relativistic plasma physics• Extreme Dense Matter Physics• Multi-wavelength studies: Photonic windows
Non-photonic windows
Pulsar Science with the SKAVery wide range of applications:
• Galactic probes• Extragalactic pulsars• Relativistic plasma physics• Extreme Dense Matter Physics• Multi-wavelength studies• Exotic systems: planets
millisecond pulsarsrelativistic binariesdouble pulsarsPSR-BH systems
Pulsar Science with the SKAVery wide range of applications:
3.Holy Grail: PSR-BH
Double PulsarsPlanets
• Galactic probes• Extragalactic pulsars• Relativistic plasma physics• Extreme Dense Matter Physics• Multi-wavelength studies• Exotic systems• Gravitational physics: - Strong-field tests
- BH properties- Gravitational Waves
Pulsar Science with the SKAVery wide range of applications:
Black Hole spin:
Black Hole properties
•Astrophysical black holes are expected to rotate
2MS
Gc
≡χ S = angular momentum
• Result is relativistic spin-orbit coupling• Visible as a precession of the orbit:
Measure higher order derivatives of secularchanges in semi-major axis and longitude of periastron
• Not easy! It is not possible today!• Requires SKA sensitivity!
See Wex & Kopeikin (1999)xx ,,ω
Black Hole quadrupole moment:
Black Hole properties
•Spinning black holes are oblate
Q = quadrupole moment32
4
MQ
Gcq ≡
• Result is classical spin-orbit coupling
• Visible as transient signals in timing residuals
• Even more difficult! • Requires SKA!
Wex &
Kopeikin (1999):
• For all compact massive, BH-like objects, we’ll be able to measure spin very precisely
• In GR, for Kerr-BH we expect:
1≤χ• But if we measure
χ > 1 ⇔ Event Horizon vanishes ⇔ Naked singularity!
• Then: either GR is wrongor Censorship Conjecture is violated!
Cosmic Censorship Conjecture
No-hair theorem
2χ−≠q• If we measure
either GR is wrong, i.e. “no-hair” theoremis violated
or we have discovered a new kind of object, e.g. a Boson star with
210χ−≤q
Was Einstein right? What are the Black Hole properties? Do naked singularities exist? Do Black Holes have “hairs”?
Fundamental Physics with the SKA Pulsars discovered and observed with the SKA…
• complement studies in other windows • probe wide range of physical problems• New science possible – not just the same:
Work to be done: 2PN timing formulaCalibration techniquesMeans to handle blind surveyEfficient timing methods(LOTS of data, LOTS of pulsars)