Using pulsars to probe the interstellar medium
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Using Pulsars to probe the interstellar medium. Barney Rickett, University of California San Diego Department of Electrical & Computer Engineering. Presentation at PAC 2012 - KIAA/PKU October 2012. Probing the Galaxy with Pulsars big picture.

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Using pulsars to probe the interstellar medium

Using Pulsars to probe the interstellar medium

Barney Rickett,

University of California San Diego

Department of Electrical & Computer Engineering

Presentation at PAC 2012 - KIAA/PKU October 2012


Probing the galaxy with pulsars big picture

Probing the Galaxy with Pulsarsbig picture

  • FAST sensitivity and sky coverage => More pulsars and DMs (DM = ∫ ne dl)

  • Pulsar HI absorption measurements => new pulsar distances

  • More pulsars, DMs & distances

    • => Better model for electron distribution in Galaxy

    • => Better model for 3D distribution of pulsars

  • Pulsar Rotation Measures + better electron model

    • => Better model for Galactic Magnetic Fields


Dm sin b versus latitude b assume stratified disk electron density n e z

DM sin(b) versus Latitude bassume stratified disk => electron density ne(z)

  • DM = ∫ Lp ne dl = ∫ Zp ne(z) dz/sinb

  • DM sinb = ∫ Zpne(z)dz

  • if Zp < Hne DM => Lp ne(0)  Lp

  • if Zp > Hne DM sinb => DM90 = ∫ ∞ne(z)dz ~ ne(0) Hne

z

*

Zp

Hne

Lp

*

ne(z)


Dm versus latitude b

20/sinb

DM versus Latitude b

DM = ∫ ne dl = ∫ ne(z)dz/sinb < DM90 /sinb


Dm sin b versus latitude

DM sin(b) versus Latitude

DM sinb = ∫ Zpne(z)dz < DM90


Delay spectrum jenet et al 2010 psr b1937 21

Delay spectrum (Jenet et al. 2010) PSR B1937+21

Possibility to determine the temperature and number of cool HI clouds.

emission

absorption

delay


H a galactic distribution

H-a Galactic Distribution

Cygnus Region

SMC LMC

Ia ~ ∫ ne2 dl = EM (cm-6 pc)

Large Iacan be a lower bound to EM (due to saturation)


Pulsar dms galaxy h a

FAST: ZA< 40deg

AO: ZA< 20deg

Psrs & high DM in LMC & SMC

Pulsar DMs + Galaxy Ha


Zoom pulsar dms galaxy h a

FAST: ZA< 40deg

AO: ZA< 20deg

Zoom Pulsar DMs + Galaxy Ha


Zoom2 pulsar dms galaxy h a

Zoom2 Pulsar DMs + Galaxy Ha


Probing the galaxy with pulsars

Probing the Galaxy with Pulsars

  • Modelling the electrons in the Galaxy:

  • Taylor & Cordes 1993; Cordes & Lazio 2001-2006

  • Questions:

  • Are pulsars concentrated in spiral arms?

    • At 100 km/sec a psr moves 1kpc in 107 years

  • Is the concentration of psrs near 40deg longitude:

    • a spiral arm? or due to AO observational (sensitivity) bias

  • What is ne between the spiral arms?

  • Are there more pulsars hidden by scattering in the Cygnus region?

  • Better estimates of the perpendicular distribution of pulsars & electron density


  • Spiral structure

    Spiral structure

    42 deg

    Cordes & Lazio 2006


    Cordes lazio n e model 2006

    Cordes Lazio Ne model (~2006)

    Need to compare

    distributions of

    Plasma and Pulsars

    Neutron star distribution as history of star formation ?


    Fast simulation smits et al

    FAST simulationSmits et al.


    Probing the galaxy with pulsars small scale picture

    Probing the Galaxy with Pulsarssmall-scale picture

    • Small-scale structure in the ISM scatters radiowaves

    • Refractive index deviation l2

    • Scattering is typically consistent with Kolmogorov turbulence over scales from 1000 km -> 100 AU (Armstrong et al. 1995)

    • But turbulence level is very inhomogeneous i.e. “patchy”

      • see the Ha maps

    • Turbulence is often anisotropic

    • Probe by pulsar scattering:

      • DM variation

      • Pulse Broadening time & ISS bandwidth

        • Scattering hides pulsars (esp. MSPs)

      • Scintillation Arcs (Stinebring et al.)


    Iss geometry

    ISS Geometry

    From Radio Galaxy Quasar or AGN

    2000

    pc


    Structure function of dispersion measure psr b1937 21 ramachandran et al 2006

    The solid line gives the best fit line with power law index a =1.66 ±0.04 consistent with Kolmogorov a = 5/3

    Ramachandran et al 2006:

    Slope = 1.66

    Structure function of Dispersion Measure PSR B1937+21Ramachandran et al. 2006


    Temporal broadening

    pulsar

    Temporal broadening

    zp

    scattering layer

    zo

    q

    Scattered Image Brightness = B(q,b)

    Scattered Pulse shape:

    P(t) = ∫ 02πB[q=√(2ct/zeff),b] db

    zeff = (zo+zp)(zp/zo)

    Pulse Broadening timetscatt= zeffq2 /2c f -4.4


    Pulse broadening vs frequency

    Pulse Broadening vs frequency


    Using pulsars to probe the interstellar medium

    Scattered pulse shape for PSR J1644-45 observed at 660 MHz at ParkesRickett, Johnston and Tomlinson, 2004

    Kolmogorov:

    Inner scale < 10km

    loge[P(t)]

    Detailed shape is a diagnostic of scattering at high wavenumbers (ie due to very small scales)

    Conclude linner ~ 75 km

    Allowing for anisotropy makes this a lower limit

    This requires very high signal to noise ratio (ie FAST)

    Inner scale > 1000km


    T scatt versus dm

    The uniform Kolmogorov model predicts:tscatt DM2.2

    But the observations show a much steeper dependence on DM. They imply that at larger distances through the electron layer, there is an increasing chance of encountering regions of high density and high turbulence.

    This result is built in to the Galactic electron model of Cordes & Lazio (2003) as a high level of patchy turbulence in the inner Galaxy

    tscatt versus DM

    Note that tscatt responds to a column of density-variance (related to emission measure). Since we expect dne ~ne , tscatt picks out the highest densities along a line of sight.


    Psr b1133 16 at arecibo stinebring et al

    dnd

    PSR B1133+16 at Arecibo(Stinebring et al.)

    Scintillation Arcs

    dtd

    tscatt= 1/(2π dnd)

    “Secondary Spectrum” (S2) with

    three scintillation arcs

    Primary Dynamic Spectrum


    The puzzle of the arc lets

    delay t (µsec)

    Doppler Frequency fD (mHz)

    The Puzzle of the “Arc-lets”

    Hill, Stinebring et al. (2005) showed this example of the arcs observed for pulsar B0834+06. In addition to the main forward arc (following the dotted curve) there are “reverse arclets”. Those labelled a-d are particularly striking.

    They observed them over 25 days and found that they moved in Delay and Doppler, precisely as expected for the known pulsar proper motion.


    The puzzle of the arc lets 2

    The Puzzle of the “Arc-lets” 2

    Doppler Frequency fD (mHz)

    334 MHz

    321 MHz

    Predicted for plasma refraction

    The right plot shows how fD varies with observing frequency.

    Remarkably this shows that the spatial location of the scatterers is independent of frequency. They DO NOT show the expected shift due to the dispersive nature of plasma refraction.

    The left plot shows the angular position of the structures (in mas) responsible for each reverse arclet, mapped from the Doppler frequency fD . The lines have the slope expected for the known pulsar proper motion.


    Vlbi of scintillation arcs brisken et al 2010

    Note reverse arclets and one group at delay of 1 msec

    VLBI of Scintillation Arcs (Brisken et al 2010)


    Scattered brightness from b0834 06

    Note the faint offset scattering responsible for the “1 msec” arclet

    Scattered Brightness from B0834+06

    Scattered image reconstructed by mapping from the secondary spectrum. The phase provides orientation in RA/Dec

    (J-J Gao PhD UCSD)

    Dqdec (mas)

    DqRA (mas)


    Using pulsars to probe the interstellar medium

    Walker’s decomposition of Hill/Stinebring observations of B0834+06 327 MHz Arecibo Imaged by Gao assuming Vpsr

    Doppler Frequency fD (mHz)

    Blue line shows the axis derived from VLBI by Brisken, Gao et al.

    Scattered Brightness is Anisotropic, Asymmetrical & Intermittent


    What do arcs tell us

    • New tool for study of ISM

    • Thin screen model is often remarkably successful => ISM is patchy

    • Examples of thin arcs and multiple “reverse arclets” require:

    • a) Highly anisotropic scattering

    • b) very patchy distribution of “turbulence”

    • Intense turbulent regions ~10 AU dominate in a path of 108 AU !

    • Together these upset the assumptions of isotropy and uniformity in a turbulent & ionized ISM. Instead we have anisotropy and intermittency in the turbulence.

    • It leaves us with fascinating puzzles:

      • What are the astro-physical sites that cause peaks in the scattering?

      • What is the cause of the 1-D fine structure ? What role for magnetic field?

      • What consequences for MSP timing ?

    • New ideas from Cyclo-Stationary spectral analysis

    • New facilities GBT, EVLA, LOFAR, FAST

    What do arcs tell us?


    Summary

    • The sensitivity of the FAST telescope will explore the ISM on the large scale:

    • Spatial distribution of Pulsars

      • Inside and outside of spiral arms

      • More associations with supernova remnants

    • New distance measurements by sensitive HI absorption

      • Delay spectrum as a new probe of HI

    • New DMs improve the modelling of plasma in the Galaxy (Ne2020?)

      • What ionizes the ISM?

      • Influence of HII regions and supernova remnants

    • New Rotation Measures improve knowledge of the Galactic Magnetic Field

      • RM from pulsars, extra-galactic sources and diffuse synchrotron emission

        Scattered pulse shapes and secondary spectra will explore the ISM on the small scale:

    • Monitoring the non-uniform ISM for corrections to pulsar timing

      • DM variation of MSPs for timing correction

    • Particular discrete regions of scattering

      • What is their physical origin?

      • What is their density in interstellar space?

    • Study of turbulence in the interstellar plasma

    Summary


    Planck map

    Planck map


    Using pulsars to probe the interstellar medium

    PSR B1737+13 mjd 53857 Arecibo 320 MHz Stinebring

    In the 1-D scattering we find secondary spectrum:

    S2(t,fD) µ B(t/AfD+AfD) x B(t/AfD-AfD) / |fD|

    in terms of the 1-D brightness function B(q) and a scaling constant A

    Hence from observations of S2 one can fit the observations S2 to a 1-D model and so estimate B(q)


    Using pulsars to probe the interstellar medium

    PSR B1737+13 mjd 53857 Arecibo 320 MHz Stinebring


    Using pulsars to probe the interstellar medium

    PSR B1737+13

    mjd 53857 1700 MHz

    1-dim Scattered Power

    Scattered Brightness is Anisotropic, Asymmetrical & Intermittent


    Secondary spectrum theory 1

    ft

    Relative to a center time t0 and frequency n0, the interference term is:

    Cos[2πfn(n-n0) + 2πft(t-t0)+Df0]

    fn = dt1- dt2 = [q12- q12] (z/2c)

    ft = dn1- dn2 = (q1x- q2x)V/l

    t-t0

    fn

    2DFT

    x

    x

    S1

    S2

    n-n0

    scattering screen

    Secondary spectrum theory 1

    I = |E1 + E2|2 if E1 and E2 are coherent at frequency n:

    = |E1|2 + |E2|2 + 2E1E2cos(Df)

    where Df = 2π(n1t1-n2t2)+f01-f02

    t1 = t+dt1,n1 = n+dn1

    Df = 2π[n(dt1- dt2)+(dn1- dn2)t .. + ..O(dn,dt) + f01-f02]

    V

    where

    dt1 = zq12/2c is the relative time delay

    dn1 = n(V.q1)/c is the relative Doppler frequency


    Arc equations

    V

    q

    2

    z

    q

    1

    scattering screen

    Arc Equations

    t= dt1- dt2 = [q12- q22] (z/2c)

    fD = dn1- dn2 = (q1x- q2x)V/l

    With q2 fixed there is a quadratic relation between t and fD which depends on q1y2. If in addition q1x and q1y lie on a straightline (ie 1-D scattered brightness) the relation is a parabola through the origin => reverse arclet

    b

    In that case the visibility phase on baseline b corresponds to the mean position of the two angles => π (q1+ q2). b/l

    Apex of parabola is where q2=0, hence visibility phase at an apex gives astrometric measure of q1.


    B1737 13 10 weeks of 1 d models

    B1737+13 10-weeks of 1-D models

    Proper motion ~30 mas/yr

    Psr distance 4.8 kpc (DM)

    Angle units ~ mas

    Proper motion predicts

    0.5 mas per week

    No coherent shifts seen

    Some decorrelation even over half-hour


    Alternative geometries for arcs

    Alternative Geometries for Arcs

    Individual scattering centers

    Background of distributed turbulence

    Perpendicular Geometry

    Anisotropic & intermittent - spaghetti-like filaments in SN remnants

    Separate offset feature also needed

    Parallel Geometry

    Isotropic scatterers clumped linearly

    Other clumps too far from line of sight


    Part of cygnus loop supernova remnant age 5 10 kyr

    Part of Cygnus Loop Supernova Remnant age 5-10 Kyr

    ~4 pc

    Bright shell:

    EM ~ 100 pc cm-3

    dL ~ 1 pc

    => max ne ~ 10 cm-3


    Density of galactic plane pulsars vs longitude

    Density of Galactic plane pulsars vs longitude

    Ha intensity ± 5 deg latitude


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