APS meeting, Dallas 22/04/06 1 A search for gravitational wave signals from known pulsars using early data from the LIGO S5 run Matthew Pitkin on behalf.

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APS meeting, Dallas 22/04/06 1 A search for gravitational wave signals from known pulsars using early data from the LIGO S5 run Matthew Pitkin on behalf of the LIGO Scientific Collaboration University of Glasgow LIGO-G Z

APS meeting, Dallas 22/04/06 2 Why search for known pulsars? Many millisecond and fast young pulsars have very well determined parameters and are generally very stable - excellent candidates for a targeted search using gravitational detectors! Assuming a neutron star is a rigid, asymmetric triaxial body then it will emit very well modelled gravitational waves at twice the rotation frequency Measurements of gravitational waves emitted via this mechanism would enable us to constrain pulsar ellipticities and possible neutron star equations-of-state Within the LIGO sensitive band (f gw > 50 Hz) there are currently 154 known pulsars (from the ATNF pulsar catalogue) - with 91 in binary systems and 90 within globular clusters Imagine.gsfc.nasa.gov

APS meeting, Dallas 22/04/06 3 Analysis method Heterodyne time domain data using the known phase evolution of the pulsar –Bayesian parameter estimation of unknown pulsar parameters: the gravitational wave amplitude h 0, initial phase  0, polarisation angle  and inclination angle  using data from all interferometers –produce probability distribution functions for unknown parameters and marginalise over angles to set 95% upper limit on h 0 Set limits on the pulsar ellipticity and compare with limits from spin-down arguments i.e. assuming all energy lost as the pulsar spins-down is dissipated via gravitational waves h0h0

APS meeting, Dallas 22/04/06 4 The searches so far… S1 (23 Aug – 9 Sep 2002) – a targeted search for gravitational waves from J using time domain and frequency domain techniques (B. Abbott et al, PRD, 69, 2004) S2 (14 Feb – 14 Apr 2003) – a targeted search for 28 known isolated pulsars with f gw > 50 Hz using the time domain technique (B. Abbott et al, PRL, 2005 ) S3 (31 Oct 2003 – 9 Jan 2004)/S4 (22 Feb – 23 Mar 2005) upper limits for 76 known radio pulsars – 32 isolated + 44 in binary systems; 30 in globular clusters –timing data provided by Pulsar group, Jodrell Bank Observatory and the ATNF, to coherently follow their phases over the run –upper limits on h 0 of a few x , an ellipticity of < for one pulsar, and a result for the Crab pulsar of only a factor 3 above the spin-down upper limit – S3/S4 Paper in preparation Frequency (Hz) h0h0

APS meeting, Dallas 22/04/06 5 Early S5 run Search for 73 pulsars –32 isolated + 41 in binary systems; and 29 in globular clusters –Used parameters provided by Pulsar Group, Jodrell Bank Observatory for S3 – checked for validity over the period of S5 i.e., whether the intrinsic parameter errors or timing noise were enough to possibly decohere our phase model from the true value Analysed from 4 Nov - 31 Dec 2005 using data from the three LIGO observatories - Hanford 4k and 2k (H1, H2) and Livingston 4k (L1) Frequency (Hz) h/Hz 1/2

APS meeting, Dallas 22/04/06 6 Preliminary S5 Results, 95% upper limits h0h0 Pulsars 1x < h 0 < 5x x < h 0 < 1x h 0 > 1x EllipticityPulsars  < 1x x10 -6 <  < 5x x10 -6 <  < 1x  > 1x All values assume I = kgm 2 and no error on distance Lowest h 0 upper limit: PSR J (f gw = Hz, r = 1.6kpc) h 0 = 1.6x Lowest ellipticity upper limit: PSR J (f gw = 405.6Hz, r = 0.25kpc)  = 4.0x10 -7

APS meeting, Dallas 22/04/06 7 h 0 Results Spin-down upper limit calculated with intrinsic spin- down value if available i.e. corrected for Shklovskii transverse velocity effect Closest to spin-down upper limit –Crab pulsar ~ 2.1 times greater than spin-down (f gw = 59.6 Hz, dist = 2.0 kpc) –h 0 = 3.0x10 -24,  = 1.6x10 -3 –Assumes I = kgm 2 Sensitivity curves use: Crab pulsar Frequency (Hz) h0h0

APS meeting, Dallas 22/04/06 8 Crab UL in I-  plane We can use h 0 as an upper limit on the quadrupole moment  can then be plotted on a I-  plane providing exclusion regions Using the range of moments of inertia 3x10 37 – 3x10 38 kgm 2 (Thorne, 300 Years of Gravitation, CUP) we have 1.2 – 4 times the spin-down limit for the Crab pulsar Higher moments of inertia possible for high mass neutron stars – seen with ~ 1.7 M sun (Ransom et al, 2005, Science and Nice et al, 2005, astro- ph/ ) Crab pulsar – 2.0 kpc Excluded ellipticity moment of inertia (kgm 2 )

APS meeting, Dallas 22/04/06 9 Results - astrophysics Our upper limits are generally well above those permitted by spin-down constraints and neutron star equations-of-state they have some astrophysical interest For 29 globular cluster pulsars we provide the limits independent of the cluster dynamics (apparent spin-ups seen due to accelerations within the cluster – cannot set spin-down limits) Our most stringent ellipticities (4.0x10 -7 ) are starting to reach into the range of neutron star structures for some neutron- proton-electron models (B. Owen, PRL, 2005). Crab pulsar is nearing the spin-down upper limit Chandra image: Harvard CfA 2MASS mage: IPAC/Caltech

APS meeting, Dallas 22/04/06 10 Future work These results show the first two months of S5 only, but give an idea of how the rest of the run will progress Goal for the next six months –should have more up-to-date pulsar timings for current pulsars and possibly more objects (e.g. large number of pulsars in GC Terzan 5) –should have amplitudes of < and ellipticities <10 -6 for many objects –should be able to reach the spin-down limit for the Crab pulsar – assuming no glitches Possibility of some more exciting potential targets, e.g. young X-ray pulsars Chandra image: Harvard CfA