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How photon astronomy affects searches for continuous gravitational waves

How photon astronomy affects searches for continuous gravitational waves. Ben Owen. Several ways. We can look for things better if we know more about them from photon astronomy (we think of 4 NS populations )

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How photon astronomy affects searches for continuous gravitational waves

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  1. How photon astronomy affects searches for continuous gravitational waves Ben Owen Gravitational Wave Data Analysis Workshop

  2. Several ways • We can look for things better if we know more about them from photon astronomy (we think of 4 NS populations) • Photon astronomy sets indirect upper limits on GW - milestones for sensitivities of our searches • Theories of neutron star formation and GW emission mechanisms affect where we look • Our interpretation of our results depends on emission mechanisms and indirect upper limits • Some review in Abbott et al, PRD 76, 082001 (2007) Gravitational Wave Data Analysis Workshop

  3. Four types of search • Known pulsars (e.g. Crab) • Position & frequency evolution known (including derivatives, timing noise, glitches, orbit)  Computationally inexpensive • Unseen neutron stars (???) • Nothing known, search over position, frequency & its derivatives  Could use infinite computing power, must do sub-optimally • Accreting neutron stars (LMXBs, e.g. Sco X-1) • Position known, search over orbit & frequency (+ random walk) • Emission mechanisms  different indirect limits • Non-pulsing neutron stars (“directed searches” e.g. Cas A) • Position known, search over frequency & derivatives Gravitational Wave Data Analysis Workshop

  4. Indirect upper limits on GW amplitude • Direct limits are always interesting at some level, but much more interesting if they beat indirect limits… • Known pulsars - “spin-down limit” assumes all df/dt is due to GW emission: • Highest in initial LIGO frequency band is Crab at 1.410-24 • Up by ~2 if you push uncertainties in I and D • Directed searches - same & substitute age = t=f/(4|df/dt|) • Highest well-determined one is Cas A at 1.210-24 • We don’t know if it’s in the LIGO frequency band Gravitational Wave Data Analysis Workshop

  5. Indirect upper limits on GW amplitude • Accreting stars in LMXBs - assume accretion/GW torque balance & take x-ray flux as proxy for accretion rate • Highest is Sco X-1 at 110-26 • Unseen neutron stars - use supernova rate in galaxy & plug into statistical population model • Most optimistic estimate is 410-24 • Statistical estimate with huge uncertainties Gravitational Wave Data Analysis Workshop

  6. If you know what you’re looking for, it’s easier to find it • Coherent integration gains signal-to-noise as T1/2 • OK if you know sky position, frequency, derivatives, … • If you don’t know, integrate for each possible parameter value • Cost may scale as up to T7, so T is computationally limited • Incoherent combination of N coherent pieces gains as N1/4 • Scaling and overall factor depend on parameter space searched - smaller is better! Gravitational Wave Data Analysis Workshop

  7. Known pulsars • What we’ve published: • Limits on 1 pulsar in S1: Abbott et al PRD 2004 • Limits on 28 pulsars in S2: Abbott et al PRL 2005 • Limits on 78 pulsars in S3 & S4: Abbott et al PRD 2007 • Note Kramer & Lyne in “et al”: timing data was crucial! • Best limit was 310-25 for PSR J1603-7202 (few weeks of data) • When it gets interesting: • Last year (S5) for the Crab! Paper soon… Gravitational Wave Data Analysis Workshop

  8. Known pulsars Crab, IL = 710-4 J1952+3252, IL = 110-4 95% confidence threshold by end of S5 J0537-6910, IL = 910-5 Gravitational Wave Data Analysis Workshop

  9. Known pulsars • What we’ve published: • Limits on 1 pulsar in S1: Abbott et al PRD 2004 • Limits on 28 pulsars in S2: Abbott et al PRL 2005 • Limits on 78 pulsars in S3 & S4: Abbott et al PRD 2007 • Note Kramer & Lyne in “et al”: timing data was crucial! • Best limit was 310-25 for PSR J1603-7202 (few weeks of data) • When it’s interesting: • Last year (S5) for the Crab!Paper soon… • Where we’re going: • Now 97 of 160+ pulsars in our band … but want more! Timing! • Further down the road: SKA would provide us with many more Gravitational Wave Data Analysis Workshop

  10. Unseen neutron stars (see next 2 talks) • What we’ve published: • S210 hours coherent search (Abbott et al PRD 2007) • S2few weeks semi-coherent search (Abbott et al PRD 2005) • S4few weeks semi-coherent searches (Abbott et al arXiv:0708.3818) • Best strain upper limit is 210-24 • When it’s interesting: • Already comparable to supernova limit, though that’s fuzzy • Where we’re going: • S5few months (longest coherent integration 25 hours) • Einstein@Home now on S5 - like SETI@Home but LIGO data, download from http://einstein.phys.uwm.edu ! Gravitational Wave Data Analysis Workshop

  11. Accreting neutron stars • What we’ve published (Sco X-1): • S26 hours coherent integration (Abbott et alPRD 2007) • S420 days incoherent “radiometer” (Abbott et al PRD 2007) • Best strain upper limit is 310-24 at 200Hz • When it’s interesting: • 100 lower than that: tricky even with advanced LIGO • What we’re doing: • Working on better analysis methods • Looking at other sources (frequency is known for some) • Coordinating with RXTE (Markowitz poster) & cheering AstroSat Gravitational Wave Data Analysis Workshop

  12. Directed searches • What we’re doing: • Cas A (youngest known neutron star?) ~2 weeks S5 • Galactic center (innermost parsec, good place for unknowns) • When it’s interesting: • Cas A and any ~100yr old star in center have hIL ~ 110-24 • Doable with present sensitivity! Gravitational Wave Data Analysis Workshop

  13. Directed searches IL = 10-4 IL = 10-5 Gravitational Wave Data Analysis Workshop

  14. Directed searches • What we’re doing: • Cas A (youngest known neutron star?) ~2 weeks S5 • Galactic center (innermost parsec, good place for unknowns) • When it’s interesting: • Cas A and any ~100yr old star in center have hIL ~ 110-24 • Doable with present sensitivity! • How photon astronomers can help: • Narrow positions on suspected neutron stars (e.g. HESSChandra): arcminute is OK, arcsecond is better • Find more young isolated neutron stars, small PWNe and SNRs … Gravitational Wave Data Analysis Workshop

  15. Observational interactions • Timing data for known pulsars • Jodrell Bank, several others have agreed to more timing • RXTE: J0537-6910 (Marshall et al) • Timing data for LMXBs • Keeping RXTE alive would be a good thing… • Make friends in India: AstroSat? • New discoveries (& proposed discoveries) • When you hunt new PSRs/CCOs/etc, think of indirect GW limits • Old discoveries • Several NS positions are poorly known (ROSAT/XMM), firming up with Chandra or Hubble would help our searches Gravitational Wave Data Analysis Workshop

  16. Theory(-ish) interactions • Where do we look? • Sky positions likely to have young neutron stars • What frequencies are emitted by LMXBs? • Interpretation of upper limits (right now) • How fuzzy are indirect limits? Distances, braking indices… • Can not rule out equations of state (stars could just be flat) unless we know about mountain building, so what builds mountains? • Interpretation of detections (let’s hope it’s soon!) • High ellipticity means funny equation of state • Somewhat high  means EOS or high internal B field: which? • Frequency reveals emission mechanism, composition (AMSPs) Gravitational Wave Data Analysis Workshop

  17. Wrap • Starting to get interesting sooner than we thought • More interesting faster w/help from photon astronomy • Lots of theory stuff to think about too, even if we don’t see anything until advanced LIGO - party’s just starting! Gravitational Wave Data Analysis Workshop

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