the pogolite balloon-borne soft gamma-ray polarimeter
TRANSCRIPT
![Page 1: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/1.jpg)
The PoGOLite balloon-borne
soft gamma-ray polarimeter
Mózsi Kiss
Experimentalist for the
PoGOLite Collaboration
Royal Institute of Technology,
Stockholm
© NASA/HST/CXC/ASU/J. Hester et al.
![Page 2: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/2.jpg)
Outline
• Polarization – a new window on the universe
• The PoGOLite instrument
• Performance: prototype testing and simulation results
• The PoGOLite Pathfinder and plans for the future
![Page 3: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/3.jpg)
PtrE ˆ,,ˆ,M. Owen, J. Blondin, North Carolina State University
trE ,ˆ,
Polarization – a new window on the universe
“Most instruments”:
Polarimeters:
• Photons can be characterized by their energy, direction, time of detection and
polarization, but polarization is usually not measured. So far, only one
significant measurement in the X-ray/gamma-ray band, from 1976:
photons up to 5 keV from the Crab (M. Weisskopf et al., ApJ 208 L125, 1976)
• Measuring polarization gives two new observational parameters:
polarization angle and degree
• X-ray polarimetry can be used to probe sources new information about the
emission mechanisms, geometries and magnetic fields of the observed sources
![Page 4: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/4.jpg)
A. Harding, NASA Goddard Space Flight Center (2004)
caustic
Charged particles near surface emitting synchrotron radiation
Charged particles confined between last open B-field lines
Acceleration in outer magneto-sphere pair prod. cascades
Polarization – the Crab pulsar
• One of the prime targets for polarimetry
• Three main emission models: polar cap, outer gap, caustic
• Models predict different emission mechanisms and location of emission
![Page 5: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/5.jpg)
PoGOLite collab.
Polarization – Crab pulsar emission models
Polar cap Outer gap Caustic
• All models have similar predictions for the intensity
• Different predictions for polarization angle and degree
polarimetry can be used to identify the correct model
PoGOLite collab.
![Page 6: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/6.jpg)
Direct soft photons
Cold outer disc
Scattered hard photons
Black hole
Hot inner disc
A. A. Zdziarski, et al. (2002)
Accretion discs• Primary component of photons directly from the accretion disc – unpolarized• Secondary component of photons reflected in the accretion disc – polarized• Polarization information about the geometry and inclination of the disc• Prime target: Cygnus X–1
Neutron stars• QED predicts absorption of photons polarized perpendicular to the magnetic field lines reconstruct the geometry of the magnetic fields
• Prime target: Hercules X–1
Astrophysical jets• Polarization observed in radio and UV range, polarization of HE emission unknown study emission mechanisms and magnetic field of the host galaxy
• Prime target: Markarian 501
Polarization – Other sources of interest
![Page 7: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/7.jpg)
Polarization – List of potential targets
• The Crab (pulsar) identify HE emission mechanism• Cygnus X–1 (accreting BH) study geometry and inclination of accretion disc• Hercules X–1 (accreting NS) orientation of rotation axis and B-field lines• Markarian 501 (blazar) study jets during high state• V0332+53 (accreting X-ray pulsar) study cyclotron features during outburst• 4U0115+63 (accreting NS) study physical processes under extreme conditions• GRS 1915+105 (microquasar) study direction of the magnetic field during burst
Crab
Hercules X–1
Cygnus X–1W. Forman, et al., Fourth Uhuru Catalog (1978)
![Page 8: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/8.jpg)
• Currently under construction to address these questions
• Balloon-borne experiment – measure polarization of hard X-rays/soft gamma-rays 25–80 keV
• International collaboration: United States, Japan, Sweden, France
• Excellent background reduction: active collimation, active and passive shielding
• PoGOLite uses coincident detection of Compton scattering and photoabsorption in an array
of plastic scintillators (low cost, low weight, prototype successfully tested in beam tests)
217 well-type
Phoswich
Detector Cells
Photomultiplier tubes
Side Anticoincidence
shield (BGO crystals)
PoGOLite – The Polarized Gamma-ray Observer
![Page 9: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/9.jpg)
PoGOLite – Performance characteristics
• Measure 10% polarization from a 200 mCrab source in a 6 h flight
• Field of view: 1.25 msr (2.0 degrees x 2.0 degrees)
• Pointing accuracy: better than 5% of the field of view
• Geometric area of detector: 994 cm2
• Effective area for polarimetry: 228 cm2 at 40 keV
• Energy range 25–80 keV
![Page 10: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/10.jpg)
Modulation factor:
M = difference / average
Polarization – detection principle
Polarization angle and degree can both be determined from the modulation:
Polarization degree:
(M100: modulation factor for a 100% polarized source, obtained using a beam with
a known polarization degree)
Polarization angle: phase of the fitted modulation curve
100MMPsource
The Compton scattering process is governed by the Klein-Nishina formula photons
have a higher probability to scatter perpendicularly to the incident polarization vector
Distribution of observed azimuthal scattering angles modulated by the polarization
Azimuthal scat. angle (degrees)
Co
un
t ra
te (
arb
. u
nit
s)
Distr. of azimuthal scat. angles
![Page 11: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/11.jpg)
The PoGOLite instrument (1)
Fast scintillators
(active detectors)
PMTs
Side anticoincidence
shield (BGO crystals)
Pivot axis
(elevation pointing)
Rot. axis (remove systematical bias)
Neutron shield
(10 cm polyethylene)
Slow scintillators
(active collimators)
1 m
![Page 12: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/12.jpg)
The well-type Phoswich Detector Cell (PDC). 217 of these cells in PoGOLite.
Pulse shape discrimination used to identify signals from different components
BGO crystal
Solid “fast”
plastic scintillator
Hollow
“slow” plastic
scintillator
84 cm
The PoGOLite instrument (2)
Photomultiplier
tube
20 cm
60 cm
4 cmBGO
Fast plastic
scintillator
Slow plastic
scintillator
collimator
High-Z metal
collimator foil
High-Z metal
collimator foil
Fast plastic
scintillator
Slow plastic
scintillator
collimator
27 mm 2 mm
![Page 13: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/13.jpg)
The PoGOLite instrument (3)
Simplified sketch of the detector array
• Fully contained events:
Compton scattering and
photoelectric absorption
• Relative energy deposition
used to reconstruct the
path of the photons
• Polarization modulation
in observed distribution of
azimuthal scattering angles
• Off-axis events give signal
in slow scintillator, SAS or
BGO and are rejected
![Page 14: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/14.jpg)
The PoGOLite prototype (1)
19 units
19 phoswich
detector cells
1 segment of the side
anticoincidence shield
Flight-version front-end electronics
Several prototype tests to date: synchrotron photons, radioactive sources, accelerator protons, neutrons…
![Page 15: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/15.jpg)
The PoGOLite prototyope (2)
MF
29.8 +- 0.4%
37.1 +- 0.7%
39.5 +- 0.8%
Inner 6 units
Outer 12 units
19 units
• Latest test: Feb. 2008, KEK “Photon Factory” in Tsukuba, Japan• Synchrotron photons, 50 keV, (90 ± 1)% linear polarization• Array rotated in 30 degree steps (like flight-version)• Observed modulation factor consistent with simulations
![Page 16: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/16.jpg)
Simulated observation data
• Monte Carlo simulations show that atmospheric neutrons
dominate the background. The PoGOLite model in Geant4
• With the 10 cm thick polyethylene shield, the background
can be reduced to less than a 100 mCrab level in the
PoGOLite energy range (25–80 keV)
Differential flux as a function
of the detected energy
![Page 17: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/17.jpg)
The Crab pulsar – Observation with PoGOLite
caustic
A. Harding, NASA Goddard Space Flight Center (2004)
• Three main emission models: the polar cap model, outer gap model
and the caustic model
• Six hour measurement with PoGOLite enough to identify correct
model or to put severe constraints on future models if all three
models turn out to be incorrect
![Page 18: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/18.jpg)
• 61 unit proof-of-principle “pathfinder” instrument currently under construction
• Measure polarization from the Crab nebula at a 7 level
• Detect as low as 10% polarization from Cygnus X–1 in the hard state
• Study in-flight background from neutrons, cosmic rays, gamma-rays
• First flight from Esrange in Sweden in August 2010
The PoGOLite Pathfinder
![Page 19: The PoGOLite balloon-borne soft gamma-ray polarimeter](https://reader031.vdocuments.site/reader031/viewer/2022012301/61e2029fc673584ea223a630/html5/thumbnails/19.jpg)
Short flights (6 – 8 hours)
• E.g. from Sweden or the US
• Proof-of-principle, evaluate background
• Observe the Crab pulsar
Long duration flights (5 days)
• From Esrange (Sweden) to western Canada
• Better statistics. Time variation.
• Multiple targets: the Crab, Cyg X-1, Her X-1...
Flights of opportunity
• No consumables can be launched when
an interesting event is detected by GLAST or
SWIFT
Esrange,
Sweden
Canada
• Next step after the Pathfinder mission: 217-unit full-scale instrument
• Numerous interesting targets – pulsars, accreting black holes, active galaxies, etc.
• Different flight types foreseen:
Outlook