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May 30, 2006

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May 30, 2006. LIGO-G060282-00-Z. Gravitational Wave ... Oblate shape due to rotation. Oscillation is self-similar and is described by: Quadrupole moment ... – PowerPoint PPT presentation

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Title: May 30, 2006


1
Gravitational Wave Sources near 1 HzAvetis Abel
Sadoyan
  • D.Sedrakian,
  • M.Hairapetyan,
  • K. Shahabasyan
  • Yerevan State University
  • Mathew Benacquista
  • Montana State University-Billings

CRDF/NFSAT Award ARP2-3232-YE-04
2
Outline
  • White dwarf frequencies
  • Gravitational radiation mechanisms
  • Stochastic background level near 1 hz

3
Why White Dwarfs?
NS
WD
4
Why White Dwarfs?
  • White Dwarfs(WD) are stellar configurations with
    central densities 106-109 g/ cm3
    -they are on the border between normal stars and
    relativistic configurations
  • Quadrupole moment of WDs is Q1048g cm2
    - several orders higher then Neutron Stars
    Quadrupole moment

5
Why White Dwarfs ?
  • White Dwarfs(WD) are the most close potential
    sources of GWs
    - there are White Dwarfs at 8 pc
    distance.
  • WD Population is estimated about 108 in the
    Galaxy
  • -WDs are the largest population among
    potential astrophysical sources of GWs

6
Strain Amplitudes
  • Oblate shape due to rotation
  • Oscillation is self-similar and is described by
  • Quadrupole moment

Choose z-axis along rotation axis
Q0zz2Q0xx2Q0yy2Q0
7
Polarizations
  • In TT gauge with z-axis along the wave vector
  • where ? is the angle between the wave vector and
    the white dwarf axis of rotation

8
Gravitational Radiation Intensity
9
White Dwarf Properties and Resonant Frequencies
10
Frequency Range of WD Oscillations
Central density
11
Deformation Energy
  • M and Mo are mass of rotating and non-rotating
    configurations with same complete number of
    baryons N

12
White Dwarfs Maximal deformation Energy versus
Central density
13
GW Amplitudes from WDs rotating with Keplerian
angular velocities
14
Mechanisms of GW Radiation
  • GWs from Magnetized WDs
    -deformation energy is feeding oscillations
    -magnetodipol radiation torque is breaking
    rotation
  • GWs from differentially rotating WDs
  • GWs from triaxial WDs

15
Types of Models of WDs
  • Model 1.a is calculated by requiring that the
    largest Doppler broadening of spectral lines due
    to pulsations be less than thermal Doppler
    broadening
  • Model 1.m is based on assumption that all
    non-dissipated part of deformation energy is
    going to oscillations, it is maximal possible
    model to that sense.

16
GWs from Magnetized WDs 1.a
17
GWs from Magnetized WDs 1.m
18
Differentially Rotating WDs model 2.1
19
Differentially Rotating WDs model 2.2
20
Triaxsial WDs model 3.r
  • Rotating triaxsial ellipsoid

21
Triaxsial WDs model 3.n
  • Non Rotating, oscillating triaxsial ellipsoid

22
Stochastic background level
  • Background is not isotropic Assuming a galactic
    distribution of white dwarfs to follow the disk
    population, we assign a density distribution of
    WDs
  • in galacto-centric cylindrical coordinates, with
    R02.5kpc and h200pc

23
Conclusions
  • Gravitational radiation spectrum near 1 hz is
    inhabited by Isolated White dwarfs
  • Model 1.a hav 8.35 10-27
  • Model 1.m hav 7.94 10-25
  • Model 2.1 hav 2.01 10-25
  • Model 2.2 hav 1.62 10-25
  • Standard inflation gives h10-2710-29 in this
    frequency range.

24
Equation of State for White Dwarfs
  • where
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