Unveiling the Secrets of the Cosmos with the Discovery of the Most Distant Object in the Universe

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Unveiling the Secrets of the Cosmos with the Discovery of the Most Distant Object in the Universe Alexander Fritz INAF IASF Milano Cucchiara et al. 2011, ApJ, 736, 7 Astro-Siesta, INAF-IASF Milano

Outline Introduction Probing the high-redshift universe: why and how Discovery of the most distant object in the universe Conclusions

Sketch of a GRB

What is the best probe at high-z? Poor understanding of early universe (<1 Gyr after Big Bang) Galaxies/quasars probe e.g.: baryon content, SFR, UV BG, re-ionization New (refurbished) instruments of HST/ACS+WFC3 allow to study LF and galaxy evolution up to z~10 with Ly-α break Ly-α z~8.6 z~10 Lehnert et al. 2010 Bouwens et al. 2010, 2011 z~8.6

What is the best probe at high-z? Galaxies Gamma-ray bursts PROS Multi-band data available (some) Refurbished HST Do not fade(-out) Different technique (LBG, Ly-α em) CONS Small sky area Very faint objects Several hours of deep observations Galaxy populations complex (SFRs, age/metallicities, dust, etc) PROS Very bright Random location and time Fast follow-up (space & ground) Simple spectrum (synchrotron, PL) Better constraints on τ HI possible CONS Rare objects (few good ones) Fade fast, identify position in ~min Require multi-band observations

SWIFT STRIKES AGAIN! Multi-wavelength campaign for GRB 090429B 2.2M/GROND SWIFT HST UKIRT VLT GEMINI

GRB 090429B: A brief history of its discovery Swift alert: April 29, 2009 - Constellation Canes Venatici Credit: NASA / Swift

GRB 090429B: A brief history of its discovery Swift alert: April 29, 2009 - Constellation Canes Venatici -T 90 = 5.5 sec burst Long-GRB Host or No-host? What is the Redshift? Credit: NASA / Swift / Stefan Immler

Swift alert: April 29, 2009 -T 90 = 5.5 sec - BAT fluence: 3.1 x 10-7 erg/cm 2 -E peak = 49 kev - lag32/(1+z) = 58 ± 27 ms Swift - BAT E iso > 10 53 erg/s Meszaros et al. 2011

Swift - XRT - Observations began 104 sec after trigger - Rising as t +0.96 followed by t -1.20 - N(HI) excess: 10.1 (-5.3,+4.6) x 10 20 cm -2 2.7 σ higher than galactic N(HI) (1.2 x 10 20 cm -2 ) t +0.96 t -1.20 Campana et al. 2009

Optical and X-ray data UVOT observed right after XRT GROND observed within 14 min VLT observed at T ~ 1 hr after (R, z ) Gemini-GMOS obs at T ~ 3 hr (z, i ) GROND: ß OX < 0.1 Dark burst Only upper limits in Optical and NIR We activated our Gemini ToO program Using NIRI in JHK we identified a fading counterpart (two days apart) Gemini Gemini VLT

UVOT observed right after XRT GROND observed within 14 min VLT observed at T ~ 1 hr after (R, z ) Gemini-GMOS obs at T ~ 3 hr (z, i ) Optical and X-ray data Only upper limits in Optical and NIR K F K ~ t-0.53± 0.10 JH i z We activated our Gemini ToO program Using NIRI in JHK we identified a fading counterpart (two days apart) Bad weather No spectrum

Photometric redshift model Photometric redshift analysis of the first night data using the Hyperz tool (Bolzonella et al. 2000) by modeling the JHK detections using different dust extinction laws GRB 090429B SED ß IR =0.5±0.17 K H J z i ß X =1.0±0.12 X-ray

Photometric redshift model Photometric redshift analysis of the first night data using the Hyperz tool (Bolzonella et al. 2000) by modeling the JHK detections using different dust extinction laws Need to understand: GRB 090429B SED Error budget NIR δ K =0.04 m ß IR =0.5±0.17 Intrinsic dust and extinction-laws Temporal decay index (α) K H ß X =1.0±0.12 Opt-NIR spectral index (ß) J z i X-ray

Photometric calibration Gemini-N/GMOS r 0.4" seeing, T=14 d GBR properties: Gemini-N/GMOS: r >27.07 m No evidence for host galaxy Using UKIRT/WFCAM, GROND, Gemini-NIRI acq images, and stars B + C photometric errors were reduced to: δ J =0.16, δ H =0.05, δ K =0.04

Photometric redshift model Photometric redshift analysis of the first night data using the Hyperz tool (Bolzonella et al. 2000) by modeling the JHK detections using different dust extinction laws Need to understand: GRB 090429B SED Error budget NIR δ K =0.04 m ß IR =0.5±0.17 Intrinsic dust and extinction-laws Temporal decay index (α) K H ß X =1.0±0.12 Opt-NIR spectral index (ß) J Infer from data: z Absence of optical afterglow z >6.3 i If J-H color Ly-break: 8 < z < 10.5 X-ray Explore different extinction-laws, α and ß ranges

SED of GRB 090429B SMC dust extinction-law and tested most challenging scenarios: 0 < A V < 12 Based on previous observations and assuming a break between optical and X-ray (e.g. Δβ ~ 0.5): 0.3 < β < 0.85 No assumption on temporal index (excluding steep rising/decay): -1< α < +1 Best fit A V = 10.6 ruled out at 99.9%

SED of GRB 090429B SMC dust extinction-law and tested most challenging scenarios: 0 < A V < 12 Based on previous observations and assuming a break between optical and X-ray (e.g. Δβ ~ 0.5): 0.3 < β < 0.85 No assumption on temporal index (excluding steep rising/decay): -1< α < +1 Best fit Best solution is z = 9.36 and A V =0.1, ß=0.51 with 99% c.l. at z > 7.7 (and A V =0.5)

The low-z solution The low-redshift solution describes a highly extincted host galaxy Thanks to ACS/WFC3 HST program by Nial Tanvir and Andrew Levan No z<1 host detected! Even a dusty host at z<1 is very unlikely fainter V-R Y-z H M B > -15.5 (L 0.001 L* @ z=1) At z = 9.4 M 1500Å > -19.95 Consistent with Bouwens et al. 2010 Non detection of the host down to deep limits allows us to exclude the low-z solution!!

The low-z solution The low-redshift solution describes a highly extincted host galaxy Thanks to ACS/WFC3 HST program by Nial Tanvir and Andrew Levan No z<1 host detected! Even a dusty host at z<1 is very unlikely fainter V-R Y-z H z = 9.4: M 1500Å > -19.95 M B > -15.5 (L 0.001 L* @ z=1) At z = 9.4 M 1500Å > -19.95 Consistent with Bouwens et al. 2010 Non detection of the host down to deep limits allows us to exclude the low-z solution!! Bouwens +2010

Comparison with other probes Credit: Fox / Cucchiara / Levan / Tanvir

Conclusions We detected the afterglow of GRB 090429B with Gemini-NIRI in JHK No host galaxy has been found with HST: M B > -15.5 (L 0.001 L* @ z=1) We performed a photometric redshift analysis and tested a large range of physical parameters for the afterglow and different dust extinction laws: NIR + high-energy data exclude z < 5, photometric fit: 7.7 < z < 9.5 (99%) Dust properties of the host or extreme physical parameters of the afterglow emission do not significantly impact our results (no high dust destruction) GRB properties similar to other long-duration GRBs: progenitor Pop II star GRB090429B is z = 9.36 (-0.3/+0.14 @ 90% c.l.) Age of Universe = 520 Myrs, size < 10%