First pulsars in polarisation with LOFAR · 2011. 9. 23. · B1541+09 B1642-03 B1839+56 B1919+21...
Transcript of First pulsars in polarisation with LOFAR · 2011. 9. 23. · B1541+09 B1642-03 B1839+56 B1919+21...
Charlotte Sobey Max-Planck-Institut für Radioastronomie
First pulsars in polarisation with LOFAR Wed 21st September 2011
First pulsars in polarisation
with LOFAR
Charlotte Sobey
Dr. Aris Noutsos & Prof. Michael Kramer
Charlotte Sobey Max-Planck-Institut für Radioastronomie
DFG Research Unit 1254
Magnetisation of Interstellar and Intergalactic Media:
The Prospects of Low-Frequency Radio Observations
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Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
Kick-Off Meeting, Irsee, October 2010
First pulsars in polarisation with LOFAR Wed 21st September 2011
Charlotte Sobey Max-Planck-Institut für Radioastronomie
Outline
First polarisation profiles of pulsars with LOFAR HBA
MKSP & PWG (TKSP)
Why? Pulsars and polarisation
Observation details
Resulting profiles
Application of RM Synthesis
Investigation of current data
including Ionosphere
ASTRON Daily Image 16th February 2011
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
Pulsars and polarisation… Many areas of research:
Determining Faraday Rotation, RM
𝑅𝑀 = 0.810 𝑛𝑒 𝑠 𝐵 𝑠 . 𝑑𝑠
𝑠𝑜𝑢𝑟𝑐𝑒
𝑟𝑒𝑐𝑒𝑖𝑣𝑒𝑟
Magnetic field structure of M.W
Deflection of HECRs, heat transport
Highly polarised, ISM only, many l.o.s
Emission mechanism, Pulsar orientation
ISM: Scattering, Scintillation…
[Van Eck et al. 2010]
[Noutsos et al. 2008]
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
RM Synthesis… Quick intro… Plane of linear polarisation modified
by Faraday rotation, 𝜒 λ = 𝜒0 + 𝑅𝑀 𝜆2
But PA known to modulo 𝜋 radians…
RM synthesis: Burn (1966), Brentjens & De Bryn (2005)
Observed complex polarisation vector: 𝑃 𝜆2 = 𝑝𝐼𝑒2𝑖𝜒
Substitute RM for Faraday depth (𝜙): 𝑃 𝜆2 = 𝐹 𝜙 𝑒2𝑖𝜙𝜆2𝑑𝜙
+∞
−∞
Fourier transform inverted: 𝐹 𝜙 = 𝑃(𝜆2)𝑒−2𝑖𝜙𝜆2𝑑𝜆2
+∞
−∞
Practically, 𝐹𝑊𝐻𝑀 = 3.8Δ𝜆2 hence BW determines accuracy…
LOFAR: Low frequency and large bandwidth (~48 MHz)!
First pulsars in polarisation with LOFAR Wed 21st September 2011
[Wikipedia]
𝜒 λ
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
LOFAR
http://www.astron.nl/~heald/lofarStatusMap.html
First pulsars in polarisation with LOFAR Wed 21st September 2011
Onsala
Chilbolton
Exloo
Nancay
Unterweilenbach
Effelsberg
Juelich
Potsdam
Tautenburg
10 – 90 MHz
110 – 240 MHz
2 x 48
2 x 24
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
RAW Voltages to RMs… Coherent dedispersion with Stokes
[A.Noutsos]
RM synthesis
Freq I Q U V ---------------------------------------------------------------------------------------------------------------
112.0 1.2 0.3 -0.6 0.1
: : : : :
PSRfits
archive
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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[A. Noutsos]
Charlotte Sobey Max-Planck-Institut für Radioastronomie
Polarisation observations – ‘survey’ ‘Survey’ of bright pulsars in raw voltage mode (after I ‘survey’)…
Coherent addition of Superterp stations (12 sub-stations)
Frequency = 136.322 MHz
Bandwidth = 6.250 MHz
(180,0)
(180,60)
(180,-60)
LOFAR HBA
RM
No RM
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
Example Profile…. B0823+26
Pulse Phase
Flu
x (
arb
itra
ry)
P.A
. (d
eg)
Pulse Phase
Flu
x (
arb
itra
ry)
P.A
. (d
eg)
Faraday Depth (rad m-2)
FD
F r
esid
ual
Before RM After RM
RM Synthesis
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
LOFAR Observations I
Flux
B0136+57 B0329+54 B0525+21 B0809+74 B0823+26
B1237+25 B1508+55 B1133+16 B0950+08 B0834+06
P.A. (deg)
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
RM synthesis I
Polarised Pulsars: Observations & applications Wed 14th September 2011
Re
sid
ual F
ara
day D
ispe
rsio
n F
un
ction
(N
orm
alis
ed
)
Faraday Depth (rad m-2)
FWHM = 6.9 rad m-2
B0136+57 B0329+54 B0525+21 B0809+74 B0823+26
B1237+25 B1508+55 B1133+16 B0950+08 B0834+06
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
LOFAR Observations II
Polarised Pulsars: Observations & applications Wed 14th September 2011
P.A. (deg)
Flux
B1541+09 B1642-03 B1839+56 B1919+21 B1929+10
B2111+46 B2217+47 B2224+65 B2306+55 B2315+21
Pmin
DMmax
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
RM synthesis II
Polarised Pulsars: Observations & applications Wed 14th September 2011
Resid
ual F
ara
day D
ispers
ion F
unction (
Norm
alis
ed)
Faraday Depth (rad m-2)
FWHM = 6.9 rad m-2
B1541+09 B1642-03 B1839+56 B1919+21 B1929+10
B2111+46 B2217+47 B2224+65 B2306+55 B2315+21
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
Crab Pulsar Giant Pulses 6 CS, 10 min
Freq = 121.08 MHz
BW = 3.125 MHz
dt = 82 μs
P.A. (deg)
Flux
Tim
e [
min
s]
Pulse phase = 20 x PCrab (673 ms) [A. Noutsos]
Flu
x [k
Jy]
[Jessner et al. 2010]
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
RM stability… B0834+06 12 CS, 10 min
Freq = 122.650 MHz
BW = 6.250 MHz
FWHM = 6.9 rad m-2
18:40 19:40 23:40 00:40 20:40 21:40 22:40
Local Time
FDF
First pulsars in polarisation with LOFAR Wed 21st September 2011
P.A. Flux
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
RM stability… B0834+06 (II)
SS = Sunset
T[C,N,A] = Twilight [Civil, Nautical, Astronomical]
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
Ionospheric effects
𝑅𝑀 = 0.810 𝑛𝑒 𝑠 𝐵 𝑠 . 𝑑𝑠 𝑠𝑜𝑢𝑟𝑐𝑒
𝑟𝑒𝑐𝑒𝑖𝑣𝑒𝑟
TECU = 1016 e- m-2
|B| ≈ 50,000 nT
ΘB ≈ +65 deg
RM variation of ~1 rad m-2 ≈ 10 TEC
More sensitive than GPS data
Future calibration essential… [British Geological Survey 2010]
[Stappers et al. 2011]
First pulsars in polarisation with LOFAR Wed 21st September 2011
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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Charlotte Sobey Max-Planck-Institut für Radioastronomie
Pulsar polarisation observations with LOFAR HBAs!
Observations, analysis and investigation...
Ionospheric variation – calibration…
LOFAR future: discoveries of ~250 by 12.12.12!
SKA
Pulsar discoveries (1000s)
RM precision improved (BW 250 MHz & SNR)
Thank you for listening!!
First pulsars in polarisation with LOFAR Wed 21st September 2011
Conclusions
Intro Polarisation LOFAR Observations RM synthesis Analysis Conclusion
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