bowman_hubble_2010
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The Dawn of 21 cm Cosmology
with EDGES
Judd D. Bowman
Caltech
Alan E. E. Rogers
Haystack Observatory
21 cm cosmology
75% Hydrogen WFC3/HUDF09, z = 7-8
(by mass)
Illingworth
Image: Scientific American 2006
21 cm hyperfine line of hydrogen
• For a cloud of hydrogen gas between us and a radiation source,
21 cm scattering changes the observed brightness temperature:
standard model
local
cosmology
over-density
spin
neutral temperature
fraction
• Universal radiation source: Cosmic Microwave Background
21 cm Background
“Science with the MWA”
Greenhill, Bowman, et al. (2010, in prep)
Figure by Matt McQuinn
Science, Vol. 325. no. 5948, pp. 1617 – 1619, 25 September 2009
CMB Spin, TS
Kinetic
Ionized fraction
xi = 1 - xHI
Mean brightness
temperature
Pritchard & Loeb 2008
Why global 21 cm?
• Straightforward probe of mean neutral fraction and HI gas
temperatures (spin + kinetic)
• Star formation history, galaxy evolution, early feedback
mechanisms, etc.
• Direct constraint on redshift and duration of reionization
• “Simpler” than imaging/power spectrum
– Average over large solid angle
– Signal fills aperture of any antenna – a single dipole is sufficient
– Ignore ionospheric distortions
– Polarized foregrounds reduced
• The only feasible probe of the Dark Ages (z>15) IGM for at
least the next decade
Foregrounds for 21 cm cosmology
z
Milky Way – synchrotron emission
100-1000 K @ 200 MHz Foregrounds
|21 cm|
TF() [MHz]
Haslam et al. (1982)
Experiment to Detect the
Global Epoch of Reionization Signature
(EDGES)
EDGES
Spectral band: 90-205 MHz
Spectral resolution: 13 kHz
FOV: ~80 deg (FWHM)
Dynamic range: >106
Antenna RFI trailer
EDGES block diagram
Bowman & Rogers (in prep)
Comparison-switched spectrometer
• 3-position switch to measure (cycle every 10s):
• Solve for antenna temperature:
(Tcal > TL 300 K, TA 250 K, TR 20 K)
• Limitations:
– Total power differences between TL and TA produce residuals
– Temporal variations: comparing measurements distinct different times
Comparison-switched spectrometer
Noise source (p1)
Internal load (p0)
Antenna (p2)
“Calibrated” sky spectrum p1– p0
RFI filtering sky spectrum
w/“Calibrated”and integration
T_A ~ (p2 – p0) / (p1 – p0) p2 – p0
EDGES Latest Results
Measured spectrum
Murchison Radio-Astronomy
Observatory (MRO)
Aug 20 – Oct 20, 2009
1440 wall-clock hours on sky
~500 hours after RFI filtering
~50 hours actual integration
Total power in band vs. time (Aug 23, 2009)
Average antenna temperature 90-205 MHz
Integration… rms vs. time
w/ baseband removal
20 Oct 2009
RMS [K]
Systematic free performance level:
RMS = 30 mK in 13 kHz channels (thermal)
~5 mK in 2 MHz bins
Integration time [hours]
Model fitting
11
• Polynomial term: p an n to account for impedance
mismatch + galactic spectrum
n 0
T21
• Simple step model of reionization: m erfc 0
2
“instantaneous” reionization
T21
3 science parameters: T21, , and 0
12 nuisance parameters: an (ACKK!!)
Was reionization instantaneous?
Fit for T21
with fixed = ∞
Test all 0
Confidence intervals on T21 with fixed =
October 2009
reionization
barrier
yellow: 68%
gray: 95%
Bowman & Rogers (in prep)
Pace of progress
September 2008
February
August
Bowman et al. 2009
reionization
barrier
yellow: 68%
gray: 95%
How long was reionization?
Fit for
with fixed T21 = CDM
Test all 0
Confidence intervals on dx/dz with fixed T21
Δz> 0.4 Δz> 0.2
Bowman & Rogers (in prep)
21 cm derivative: constraints and forecasts
z=6 z=13 z=25
Feb 2009 NOT
reionization…
absorption
Oct 2009
anticipated systematic
limit (no/low RFI)
Integrate +
improve bandpass
Summary
• Concluded 3 month deployment in MRO
– Deepest broadband spectrum ever acquired: 5 mK rms
– Instantaneous reionization ruled out: 21 cm rapid step
constrained to <30 mK between 6<z<13
– First direct dxi/dz constraints on diffuse IGM
• The next step:
– Upgrade digital backend; exploring Berkeley CASPER open
architecture boards for high throughput
– Redesign antenna to improve impedance match (use lower
order polynomial for continuum removal)
– Attempt detection of z>15-25 absorption feature to “set clock”
for interpreting reionization
The end
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