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Thanks to: Collaborator: Ingrid Stairs PUPPI: Paul Demorest, Scott Ransom, NRAO Data from Nice et al. 2005: Eric Splaver, Ingrid Stairs, Oliver Lohmer, Axel Jessner, Michael Kramer, Jim Cordes Arecibo Observatory (SRI/USRA/UMET) NSF Orbital Decay and Mass of Relativistic Binary PSR J0751+1807 David Nice Lafayette College Physical Applications of Millisecond Pulsars, Aspen Center for Physics, 22 January 2013 UNDER CONSTRUCTION CAUTION! PRELIMINARY RESULTS

Orbital Decay and Mass of Relativistic Binary PSR J0751+1807aspen13.phys.wvu.edu/aspen_talks/Nice_0751+1807_mass.pdfPSR J0751+1807 in a Nutshell Typical Millisecond Pulsar P = 3.479

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  • Thanks to:

    Collaborator: Ingrid Stairs PUPPI: Paul Demorest, Scott Ransom, NRAO Data from Nice et al. 2005: Eric Splaver, Ingrid Stairs, Oliver Lohmer, Axel Jessner, Michael Kramer, Jim Cordes Arecibo Observatory (SRI/USRA/UMET) NSF

    Orbital Decay and Mass of Relativistic Binary PSR J0751+1807

    David Nice Lafayette College

    Physical Applications of Millisecond Pulsars, Aspen Center for Physics, 22 January 2013

    UNDER  CONSTRUCTION  

    CAUTION!  PRELIMINARY  

    RESULTS  

  • Δ t

    Δ t orbit not edge-on; observed Δ t same as edge-on case, but orbit is larger

    orbit viewed edge-on

    ?

  • ? Companion might be heavy star in small orbit or light star in a large orbit

    2πPb

    ⎝ ⎜

    ⎠ ⎟

    2 a1 sin i( )3

    G= f1 =

    m2 sin i( )3

    m1 +m2( )2

  • Precession

    Shapiro Delay

    Gravitational Radiation

    ( ) [ ] 0 2 3 sin sin 1 ln 2 ϕ ϕ - - = Δ i m c G t

    Grav Redshift/Time Dilation r v

    ( ) 3 1 3 5

    ) ( 1 1

    96 37

    24 73 1

    2 5 192

    2 1 2 1

    2 7 2 4 2 3

    5 5 m m

    m m e

    e e P c G P b b

    + - ⎟ ⎠ ⎞

    ⎜ ⎝ ⎛ + + ⎟

    ⎠ ⎞

    ⎜ ⎝ ⎛

    ⎟ ⎠ ⎞

    ⎜ ⎝ ⎛ - =

    -

    π π

    3 4

    3 2 ) ( 2 2 1 2 1 3

    1 2 m m

    +2m m P c G γ b

    + ⎟ ⎠ ⎞

    ⎜ ⎝ ⎛

    = π

    e ) ( 2 m

    ( ) 3 2

    2 1 2 3 5

    1 1

    2 3 ⎥ ⎦

    ⎤ ⎢ ⎣ ⎡

    + - ⎟ ⎠ ⎞

    ⎜ ⎝ ⎛

    = -

    m m e P b π

    ω 2 c G 2/3

    Second Orbit m  1  m  2  =  

    a  1  sin  i  a  2  sin  i  

  • Figure: Jim Lattimer stellarcollapse.org/nsmasses

  • PSR J0751+1807 in a Nutshell

    Typical Millisecond Pulsar P = 3.479 ms B=2x108 gauss Pdot=7x10-21 Spindown age=7 Gyr

    Tight circular orbit Pb = 6.3 hour e < 1x10-6 no evidence of eclipses or dispersive material in orbit

    Low mass companion m2 ~ 0.14 M optical detection, Bassa et al 2006 faint; surprising lack of hydrogen no evidence for variability

    PSR J0751+1807

  • PSR J0751+1807 Observations

    Arecibo/430 MHz Arecibo/1400 MHz Effelsberg/1400 MHz

    6 day Arecibo campaign (full orbit coverage) 430 MHz PUPPI observations Dumps @ 3 min intervals Residual rms 2.8 µs in 3 min 1400 MHz PUPPI observations Dumps @ 10 sec intervals TOAs in each of 4 subbands Residual rms 6 µs per subband in 10 s

  • PSR J0751+1807 Shapiro Delay

    CAUTION!  PRELIMINARY  

    RESULTS  

  • PSR J0751+1807 Orbit decay due to gravitational wave emission

    Orbit decay rate (95%conf) :

    Pb = – (3.3±0.3)×10–14 .

    CAUTION!  PRELIMINARY  

    RESULTS  

  • PSR J0751+1807 Shapiro Delay+Orbit Decay

    CAUTION!  PRELIMINARY  

    RESULTS  

  • PSR J0751+1807 Shapiro Delay+Orbit Decay

    CAUTION!  PRELIMINARY  

    RESULTS  

  • PSR J0751+1807 Shapiro Delay+Orbit Decay

    Masses (95% conf):

    m1 = 1.34±0.09 M#

    m2 = 0.138±0.006 M

    CAUTION!  PRELIMINARY  

    RESULTS  

  • Figure: Jim Lattimer stellarcollapse.org/nsmasses

    CAUTION!  PRELIMINARY  

    RESULTS  

  • Summmary • Detected Shapiro Delay and Orbit Decay • Masses (95% conf):

    m1 = 1.34±0.09 M #$m2 = 0.138±0.006 M#

    #

    Additional Remarks • Orbital decay precision will soon be dominated by systematics from Galactic acceleration and transverse Doppler shift; distance not presently well known; can be improved by VLBA parallax, timing parallax • Large rotating dipole moments provide interesting GR test but lack of a priori knowledge of m1 and m2 limits the usefulness of PSR J0751+1807 source for this test.

    PSR J0751+1807: Summary & Final Remarks

    CAUTION!  PRELIMINARY  

    RESULTS