Presentation is loading. Please wait.

Presentation is loading. Please wait.

On the Doorstep of Reionization Judd D. Bowman California Institute of Technology August 27, 2009.

Similar presentations


Presentation on theme: "On the Doorstep of Reionization Judd D. Bowman California Institute of Technology August 27, 2009."— Presentation transcript:

1 On the Doorstep of Reionization Judd D. Bowman California Institute of Technology August 27, 2009

2 1.Redshifted 21 cm global signal 2.Experiment to Detect the Global Epoch of Reionization Signature (EDGES) 3.EDGES latest results

3 The History of Hydrogen Gas Image: Scientific American 2006

4 When did reionization occur? How long did it last? Furlanetto, Oh, & Briggs 2006

5 21 cm Overview Spin-flip hyperfine transition of neutral hydrogen =21 cm (rest-frame), =1420 MHz At z = 6: =1.5 m, = 203 MHz At z = 15: =3.4 m, = 89 MHz 5’9” = 1.75 m  z=7.3 Use CMB as a “backlight”, then brightness temperature is:

6 Kinetic CMB Ionized fraction x i = 1 - x HI Mean brightness temperature Spin, T S Pritchard & Loeb 2008

7 Localized bubbles Mesinger & Furlanetto 100 Mpc z = 10x HI =0.89 Ionizing photons escape… Mesinger & Furlanetto 100 Mpc z = 9x HI =0.74 Bubbles grow and merge… Mesinger & Furlanetto 100 Mpc z = 8.25x HI =0.53 Mesinger & Furlanetto 100 Mpc z = 7.25x HI =0.18 On local scales, a more complex picture Reionization fronts X-ray background UV backgrounds

8 Local patchy evolution… MWA’s objective Primarily density fluctuations Early times (z > 15) Late times (z < 6) (z < 6) Ionized regions Furlanetto et al. 2004 5 arcmin

9 Big Bang! Today Pritchard & Loeb 2008 10010 z [redshift] 50 0 -50 -100 T b [mK] 21 cm global brightness temperature 5001005010  [MHz]

10 Modeling reionization history The main astrophysical parameters are: N_ion f_esc f_star f_lya f_xray - Number of ionizing photons per baryon in star formation - Escape fraction of ionizing photons from galaxies (probably between 0.02 and 0.2) - Star forming efficiency by mass (uncertain to order of magnitude) - Number of Ly-  photons per baryon in stars (popII) (uncertain to a factor of few) - X-ray luminosity relative to value extrapolated from Glover and Brand (uncertain to more than order of magnitude)

11 Modeling reionization history Code from J. Pritchard

12 Key reionization-era science questions: When did reionization occur? What sources were responsible for reionization? – Properties of ionizing sources; connect galaxy-scale physics to large-scale events by e.g. anti-correlation of 21 cm maps with galaxy formation (near-IR surveys) How did the cosmic web evolve? – Topological transition from ionized bubbles into the filamentary web seen in Ly-alpha forest How did first quasars form? What were their properties? – Large HII regions, even after quasars dormant, able to image and constrain emission mechanisms, lifetimes, luminosity function, evolution When did first black holes form? What were their properties? – X-ray heating of IGM near galaxies hosting first black holes and supernovae produces distinctive features in power spectrum (troughs, large amplitudes), z~15 How does radiative feedback affect high-z galaxy formation? – Directly probe UV and X-ray backgrounds in IGM that regulate star formation and its end products, structure formation, clumping. Soft-UV background z>15 decouples 21 cm spin temperature from CMB See decadal science review: “Astrophysics from the Highly-Redshifted 21 cm Line”, Furlanetto et al. (2009) 21 cm global vs. local science

13 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 In principle, a simple experiment: No imaging required! – Signal fills aperture of any antenna – a single dipole is sufficient – Ignore ionospheric distortions – Ignore polarized foregrounds The only feasible 21 cm probe of the Dark Ages (z>15) IGM for the next decade

14 2. Experiment to Detect the Global Epoch of Reionization Signature (EDGES) with Alan E. E. Rogers (MIT/Haystack)

15 All-sky spectrum 21 cm global signal All-sky radio spectrum (100-200 MHz) RFI Instrument bandpass Total spectrum components: Diffuse Galactic (200K to >1000K) - Synchrotron (99%) - Free-free (1%) Sun (variable) Extragalactic sources (~50K) CMB (2.7K) Galactic RRLs (< 1 K) 21 cm (10 mK)

16 EDGES approach Trade-off: Compared to MWA, we’ve lost extreme difference in spectral coherence between foreground and signal Constrain the derivative of the 21 cm brightness temperature contribution to <1 mK/MHz between 50 and 200 MHz Furlanetto 2006 Frequency derivative Mean brightness temperature

17 AEER EDGES block diagram

18 “Four-point” antenna Ground screen balun Analog electronics enclosures

19 in from antenna to 2 nd stage calibration source 2 nd stage amp dithering noise source to digitizer LNA switch

20 Acqiris DP310: 12-bit, 420 MS/s bandpass filter/ analog electronics voltage supply in from frontend

21 RFI trailer MWA fiber CSIRO “hut”

22 antenna RFI trailer

23 Murchison Radio-Astronomy Observatory, Boolardy Station, Western Australia

24 Radio Frequency Interference (RFI)

25 US radio “pollution”

26 West Forks, Maine (Jan 2009)

27 Orbcom LEO satellite constellation

28 Site selection: Local environment (< 1 mK) Antenna beam pattern: CasA (1400 Jy)  ~50 K

29 Comparison Switch Scheme 3-position switch to measure (cycle every 10s): Solve for antenna temperature: (T cal > T L  300 K, T A  250 K, T R  20 K) Limitations: – Total power differences between T L and T A produce residuals – Temporal variations: comparing measurements distinct different times

30 Antenna (p2) Internal load (p0) Noise source (p1) p1– p0 p2 – p0 “Calibrated” sky spectrum T_A ~ (p2 – p0) / (p1 – p0) “Calibrated” sky spectrum w/ RFI filtering and integration The Joy of Calibration

31 EDGES: Antenna Impedance Match

32 EDGES: Absolute Calibration Fully calibrated, western Australia  = 2.5  0.1 (3 sigma) T gal = 237  10 K (3 sigma) @ 150 MHz Long cable between antenna & LNAs to measure reflection coefficient in situ Rogers & Bowman 2008

33 EDGES: Drift Scans Rogers & Bowman 2008

34 3. EDGES Latest Results

35 Measured spectrum Murchison Radio-Astronomy Observatory (MRO) Jan 25 – Feb 14, 2009 10 days: - 50 wall-clock hours on sky - ~7 integrated hours

36 Integration… rms vs. time w/ baseband removal

37 19 mK rms – thermally limited Green = 100 kHz Black = 2 MHz Characterizing progress Jan/Feb 2009 Bowman et al. 2008 75 mK rms – systematic limited

38 Model fitting Polynomial term: Simple step model of reionization: 2 science parameters: T 21 and 0 12 nuisance parameters: a n (ACKK!!) “instantaneous” reionization  T 21 to account for impedance mismatch + galactic spectrum

39 Model fitting

40 Confidence intervals on T 21 (as of February 2009) Constraints scale linearly with thermal noise Low-level RFI contamination apparent? 68% 99% z=13z=6 < 90 mK reionization barrier

41 Confidence intervals on T 21 (as of last night!) reionization barrier

42 21 cm derivative: constraints and forecasts Current worst-case anticipated systematic limit Integrate + improve bandpass fastest plausible reionization z=13z=6z=25 NOT reionization… absorption

43 EDGES status & future work Current: – 19 mK rms in measured spectrum – 21 cm step constrained to <90 mK between 7<z<10 – 21 cm derivative <40 mK / MHz between 7<z<10 (w/ caveats) Aug-Dec 2009: unattended deployment – Cross 30 mK reionization “barrier” to rule out rapid reionization The next 3 years (funded by NSF!): – Replace digital backend with Berkeley CASPER open architecture boards for high throughput, but performance – 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

44 HI “Observation of a Line in the Galactic Radio Spectrum: Radiation from Galactic Hydrogen at 1,420 Mc./sec” “Doc” Ewen & Purcell 1951 CMB “A Measurement of Excess Antenna Temperature at 4080 Megacycles per Second” Penzias & Wilson 1965 EoR First detection of reionization?… Bowman & Rogers ???? A final thought…

45 The end This scientific work uses data obtained from the Murchison Radio-astronomy Observatory. We acknowledge the Wajarri Yamatji people as the traditional owners of the Observatory site.

46

47 EDGES: Site Selection Variations on the Radar Equation… Scattered sky noise: Scattered receiver noise: Couple spectral structure in scattering coefficient, , to spectrum Structure + ripple

48 EDGES: Combined x HI Limits Furlanetto, Oh, & Briggs 2006 Dunkley et al. 2008

49 21 cm landscape - science Inflationary physics and cosmology 30  > 7 MHz Probe of the matter power spectrum at very small scales ℓ > 10 4 to 10 6 Perturbations to primordial power spectrum and spatial curvature: n s,  Neutrino masses, non-Gaussianity, etc. Baryon collapse Reionization and the Dark Ages 6  > 46 MHz Spin and kinetic temperature history of the IGM Reionization history, Stromgren spheres (quasar proximity zones) Star formation history / models for ionizing sources Abundance of mini-halos Magnetic fields in IGM Cosmology Large scale structure/galaxy evolution z  > 203 MHz Dark Energy through BAOs, cosmology, neutrino masses, etc. HI in galaxies/halos, masses of DLAs at z = 3 Indirectly see helium reionization


Download ppt "On the Doorstep of Reionization Judd D. Bowman California Institute of Technology August 27, 2009."

Similar presentations


Ads by Google