Sources of gravitational waves for groundbased detectors - PowerPoint PPT Presentation

1 / 15
About This Presentation
Title:

Sources of gravitational waves for groundbased detectors

Description:

Free precession. Was thought to damp in 1yr (vortex pinning) ... 22, 1825 (2005): Observations say precession lasts 10yr, visible to galactic ... – PowerPoint PPT presentation

Number of Views:23
Avg rating:3.0/5.0
Slides: 16
Provided by: Beno72
Category:

less

Transcript and Presenter's Notes

Title: Sources of gravitational waves for groundbased detectors


1
Sources of gravitational waves for ground-based
detectors
  • Ben Owen
  • Penn State

2
Whats new since Amaldi-5?
(selected highlights)
  • Stochastic
  • Not much in this frequency band
  • Burst
  • Supernova simulations still dont explode, but
  • Inspiral
  • Newly observed binary pulsar increases event
    rates
  • Periodic
  • Several new theories predict big neutron star
    signals

3
Burst sources
  • Short-lived, roughly modeled signals (cant make
    matched filters)
  • Waveforms rough amplitude, band, duration
  • Populations
  • Gamma-ray bursts (NS/NS, BH/NS, hypernovae)
  • Soft gamma repeaters (NS modes)
  • Supernova core collapse
  • Dynamical instabilities in proto-neutron stars
  • Things that go bump in the night

4
Supernova core collapse
  • Ott et al., ApJ 600, 834 (2004) Mueller et al.,
    ApJ 603, 221 (2004)
  • Now realistic equations of state, neutrino
    transport
  • Strain down by 4-10, broad frequency band
  • Signal from post shock convection, modest spin
  • LIGO-I detectability at 10kpc is 10 (angles)
  • But they dont explode!

From Ott et al. 2004
5
Inspiral sources (binaries)
  • Short signals modeled well enough for matched
    filtering (optimal signal-to-noise)
  • Waveforms
  • Analytical post-Newtonian for NS/NS
  • Numerical relativity for BH/BH
  • BH/NS in between
  • Populations
  • NS/NS observed, though only a few (one more now!)
  • BH/NS and BH/BH from stellar evolution simulations

6
PSR J0737-3039
  • Burgay et al., Nature 426, 531 (2003)
  • 2.4hr orbit means 85Myr coalescence time
  • Both neutron stars pulse 22.7ms and 2.8s
  • Dominates statistics (7x old event rate)
  • Factor 3.5 due to short lifetime (total 185Myr)
  • Factor 2 from short orbit spin periods (Doppler
    smearing makes it hard to detect, must be more)
  • Maybe more since its dim? Need statistics

7
Empirical (NS/NS) event rates
  • Kalogera et al., ApJ 601, L179 (2004) erratum
  • Bayesian probability distributions of rates
  • Assume a population (luminosity distribution)
  • Simulate how many pulsars radio surveys have
    found
  • Time between detections
  • Initial LIGO 20yr median, 95 confidence gt 8yr
  • Adv. LIGO 2day median, 95 confidence gt 12hr

8
Population synthesis event rates
  • OShaughnessy et al., astro-ph/0504479
  • Now use distribution of populations
  • For each population, evolve progenitors until
    NS/NS
  • Keep only those populations consistent with
    observed type Ibc supernovae wide NS/NS
    binaries
  • Results
  • BH/NS 0.5 NS/NS (lack of BH/NS observations)
  • BH/BH lt 5 NS/NS (BH masses 7Msun)
  • And NS/NS down by 10 from previous slide!
  • But distribution of populations is from outdated
    data

9
Waveforms
  • Analytical
  • Post-Newtonian is done for ground-based (3.5PN)
    Blanchet et al., PRL 93, 091101 (2004) errata
  • Numerical
  • First BH/BH orbit (or more) Bruegmann et al.,
    PRL 92, 211101 (2004)
  • Waveform extraction remains a problem
  • Some progress on realistic initial data
  • New methods to suppress constraint violations

10
Periodic sources
  • Long-lived, nearly monochromatic, data analysis
    dominated by Doppler shifts
  • Population rotating neutron (or quark) stars
  • Key number is ellipticity e (Ixx Iyy) / Izz
  • Comparable to quadrupole/Izz, DR/R
  • Standard max. e lt few x 10-7 for neutron star
    crust
  • Detectability (initial interferometers)
  • Known pulsars e lt 10-6 (distances few kpc)
  • All-sky unknown pulsar search limited by
    computational cost range lt 1kpc for e lt10-5

11
Magnetic field bumps
  • Cutler, PRD 66, 084025 (2002)
  • Differential rotation makes B field toroidal
  • Toroidal field pinches star
  • Field axis moves toward equator, makes
    ellipticity
  • Max. e lt few x 10-6
  • But field needs to be buried (LMXBs and recycled
    pulsars?)

12
Magnetic bottling
  • Melatos Payne, ApJ 623, 1044 (2005)
  • Accreting ms pulsars
  • Matter crosses field lines very slowly,
    accumulates at magnetic poles
  • Depends on low-density conductivity (robust)
  • Max. e 10-5 if mountain is wide (quadrupole)
  • But e lt few x 10-7 for known stars from x-rays

13
Mountains (solid)
  • Owen, astro-ph/0503399
  • Mostly solid stars
  • Max. e lt few x 10-4 (quarks)
  • Max. e lt 10-5 (hybrid star)
  • Uncertain physics of high density matter
  • LIGO limits already there
  • PRL 93, 181103 (2005) 9 new es within quark
    range
  • But how to get max. e? (many pulsars are lt 10-8)

14
Other asymmetries
  • R-modes (accreting stars)
  • Duty cycle of emission was thought to be low
    (10-7)
  • Wagoner, ApJ 578, L63 (2002) Andersson et al.,
    MNRAS 337, 1224 (2002) accreting stars are good
    sources if exotic particles increase bulk
    viscosity
  • Free precession
  • Was thought to damp in 1yr (vortex pinning)
  • Van den Broeck, CQG 22, 1825 (2005) Observations
    say precession lasts gtgt10yr, visible to galactic
    core with advanced interferometers

15
Summary
  • Theory EM observation both giving good news
  • Recent upper limits are already (borderline)
    astrophysically interesting
  • Initial detectors have a fighting chance (order
    10) of detecting something!
  • (this is where Ladbrokes stopped taking bets)
Write a Comment
User Comments (0)
About PowerShow.com