Interactions between gravitational waves and photon astronomy - - PowerPoint PPT Presentation

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Interactions between gravitational waves and photon astronomy - - PowerPoint PPT Presentation

Interactions between gravitational waves and photon astronomy (periodic signals) Ben Owen October 20, 2007 LSC-VIRGO / NS meeting 1 Intro We can look for things better if we know more about them from photon astronomy (we think of 4 NS


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SLIDE 1

October 20, 2007 LSC-VIRGO / NS meeting 1

Interactions between gravitational waves and photon astronomy (periodic signals)

Ben Owen

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SLIDE 2

October 20, 2007 LSC-VIRGO / NS meeting 2

Intro

  • 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

  • GW emission mechanisms influence where we look
  • Our interpretation of our results depends on emission

mechanisms and previous indirect upper limits

  • Some review in Abbott et al gr-qc/0605028
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SLIDE 3

October 20, 2007 LSC-VIRGO / NS meeting 3

GW emission mechanisms

  • Non-accreting stars (indirect limits beatable now!)

– Free precession (looks pretty weak, I’ll skip) – Elastically supported “mountains” - internal too – Magnetically supported mountains (Melatos talk)

  • Accreting stars (indirect limits beatable with advLIGO…?)

– Accretion provides natural mountain building mechanism – R-mode oscillations build themselves (CFS instability) – More likely to radiate at indirect limits

  • All mechanisms: how high is max & how to drive it there?

– Put strength in terms of ellipticity ~ quadrupole, propto h

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October 20, 2007 LSC-VIRGO / NS meeting 4

Elastic mountains

  • How big can they be? (Owen PRL 2005)

– Depends on structure, shear modulus (increases with density)

  • Standard neutron star

– Bildsten ApJL 1998, Ushomirsky et al MNRAS 2000 – Thin crust, < 1/2 nuclear density: < few10-7

  • Mixed phase star (quark/baryon or meson/baryon hybrid)

– Glendenning PRD 1992 … Phys Rept 2001 – Solid core up to 1/2 star, several nuclear density: < 10-5

  • Quark star (ad hoc model or color superconductor)

– Xu ApJL 2003 …, Mannarelli et al hep-ph/0702021 – Whole star solid, high density: < few10-4

  • Also Lin PRD 2007, Haskell et al arXiv:0708.2984
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SLIDE 5

October 20, 2007 LSC-VIRGO / NS meeting 5

Elastic mountains in accreting stars

  • How to build high mountains?
  • Non-uniform accretion flow

hot & cold spots on crust

  • Hot spot at fixed density

faster electron capture layer of denser nuclei moves upward (non-barotropic EOS)

  • If GW balance accretion, is

determined by x-ray flux

  • Best (Sco X-1) is few10-7,

same as predicted max for normal neutron star crust Bildsten ApJL 1998, Ushomirsky et al MNRAS 2000

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SLIDE 6

October 20, 2007 LSC-VIRGO / NS meeting 6

R-modes in accreting stars

  • Complicated phenomenology

(Stergioulas Living Review)

  • 2-stream instability (CFS)
  • Viscosity stabilizes modes
  • Accretion keeps star balanced

at critical frequency … if strange particles are in core

  • Max perturbation v/v ~ 10-5

from coupling to other modes

  • GW frequency = 4/3 spin freq.

minus few % (depends on EOS)

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SLIDE 7

October 20, 2007 LSC-VIRGO / NS meeting 7

Four types of neutron stars

  • Known pulsars (e.g. Crab)

– Position & frequency evolution known (including derivatives, timing noise, glitches, orbit) Computationally inexpensive

  • Unseen neutron stars (e.g. ???)

– Nothing known, search over position, frequency & its derivatives Could use infinite computing power, must do sub-optimally

  • Accreting neutron stars (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

(P>50ms is off our radar)

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SLIDE 8

October 20, 2007 LSC-VIRGO / NS meeting 8

Indirect upper limits

  • Assume quadrupole GW emission
  • Use predicted M, R, I (could be off by 2)
  • Assume energy conservation & all df/dt from GW
  • Known pulsars - “spin-down limit”

– Best is Crab at 1.410-24

  • Non-pulsing NS - substitute age = f/(-4df/dt)

– Best is Cas A at 1.210-24

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SLIDE 9

October 20, 2007 LSC-VIRGO / NS meeting 9

Indirect upper limits

  • Accreting stars - energy conservation violated

– Assume accretion spin-up = GW spin-down (Wagoner ApJL 1984) – Infer accretion rate from x-ray flux – Best is Sco X-1 at 210-26

  • Unknown neutron stars - ???

– Assume simple population model – Plug in supernova rate in galaxy – Most optimistic estimate is 410-24 (Abbott et al gr-qc/0605028)

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SLIDE 10

October 20, 2007 LSC-VIRGO / NS meeting 10

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 PRD 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 310-25 for PSR J1603-7202

  • When it gets interesting:

– Last year (S5) for the Crab! (Pitkin talk)

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SLIDE 11

October 20, 2007 LSC-VIRGO / NS meeting 11

Known pulsars

Crab, IL = 710-4 J0537-6910, IL = 910-5 J1952+3252, IL = 110-4 95% confidence threshold by end of S5

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SLIDE 12

October 20, 2007 LSC-VIRGO / NS meeting 12

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 PRD 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 310-25 for PSR J1603-7202

  • When it’s interesting:

– Last year (S5) for the Crab! (Pitkin talk)

  • 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

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October 20, 2007 LSC-VIRGO / NS meeting 13

Unseen neutron stars

  • What we’ve published:

– S2 10 hours coherent search (Abbott et al gr-qc/0605028) – S2 few weeks semi-coherent search (Abbott et al 2005) – S4 few weeks semi-coherent searches (Abbott et al arXiv:0708.3818) – Best strain upper limit is 210-24 (sky & polarization combo)

  • When it’s interesting:

– Already comparable to supernova limit, though that’s fuzzy

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SLIDE 14

October 20, 2007 LSC-VIRGO / NS meeting 14

Unseen neutron stars

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October 20, 2007 LSC-VIRGO / NS meeting 15

Unseen neutron stars

  • What we’ve published:

– S2 10 hours coherent search (Abbott et al gr-qc/0605028) – S2 few weeks semi-coherent search (Abbott et al 2005) – S4 few weeks semi-coherent searches (Abbott et al arXiv:0708.3818) – Best strain upper limit is 210-24 (sky & polarization combo)

  • When it’s interesting:

– Already comparable to supernova limit, though that’s fuzzy

  • Where we’re going:

– S4 & S5 longer datasets (longest coherent integration 25 hours) – Einstein@Home now on S5 - like SETI@Home but LIGO data, download from http://einstein.phys.uwm.edu

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October 20, 2007 LSC-VIRGO / NS meeting 16

Directed searches

  • What we’re doing:

– Cas A (youngest known neutron star?) ~10 days S5 – Galactic center (innermost parsec, good place for unknowns)

  • When it’s interesting:

– Cas A and any ~100yr old star in center have hIL ~ 110-24 – Doable with present sensitivity! – Anything detectable now would require solid quark matter

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SLIDE 17

October 20, 2007 LSC-VIRGO / NS meeting 17

Directed searches

IL = 10-5 IL = 10-4

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October 20, 2007 LSC-VIRGO / NS meeting 18

Directed searches

  • What we’re doing:

– Cas A (youngest known neutron star?) ~10 days S5 – Galactic center (innermost parsec, good place for unknowns)

  • When it’s interesting:

– Cas A and any ~100yr old star in center have hIL ~ 110-24 – Doable with present sensitivity! – Anything detectable now would require solid quark matter

  • How photon astronomers can help:

– Narrow positions on suspected neutron stars (e.g. HESSChandra): arcminute is OK, arcsecond is better – Find more young isolated neutron stars, small PWNe and SNRs

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SLIDE 19

October 20, 2007 LSC-VIRGO / NS meeting 19

Accreting neutron stars in LMXBs

  • What we’ve published (Sco X-1):

– S2 6 hours coherent integration (Abbott et al gr-qc/0605028) – S4 20 days incoherent “radiometer” (Abbott et al astro-ph/0703234) – Best strain upper limit is 310-24 at 200Hz

  • When it’s interesting:

– 100 lower than that (Watts talk) – What kills our sensitivity? Not knowing frequency (orbit too)

  • What we’re doing:

– Trying to come up with better methods (Krishnan talk) – Other sources? (Chakrabarty talk, Galloway talk)

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October 20, 2007 LSC-VIRGO / NS meeting 20

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 PSR/CCO/etc, think of indirect GW limits

  • Old discoveries

– Several NS positions poorly known (ROSAT/XMM), firming up with Chandra or Hubble would help our searches

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SLIDE 21

October 20, 2007 LSC-VIRGO / NS meeting 21

Theory(-ish) interactions

  • Interpretation of upper limits

– Beating indirect limits on h is more exciting – How fuzzy are indirect limits? Distances, braking indices… – Can’t rule out equations of state (stars could just be flat) unless we know mountain building, so what builds mountains?

  • Interpretation of detections (let’s hope!)

– Frequency confirms emission mechanism (LMXBs) – R-mode signal means strange particles in core – High ellipticity means funny equation of state – Somewhat high means EOS or high internal B field: what max?

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October 20, 2007 LSC-VIRGO / NS meeting 22

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

  • Download Einstein@Home!