ガンマ線バーストによる宇宙再電離の研究: GRB 050904 _ z=6.3 からの制限
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The First Constraint on the Reionization
from GRBs: the Case of GRB 050904
Tomonori Totani (Kyoto)
Nobuyuki Kawai, George Kosugi, Kentaro Aoki,
Toru Yamada, Masanori Iye, Kouji Ohta,
Takashi Hattori
To Appear in PASJ (astro-ph/0512154)
STScI workshnop “The End of the Dark Ages”
2006, March 13-15
Why GRBs? a Unique Reionization Probe
Brightness
detectable to very high redshift of z>~10
much brighter than LAEs/LBGs and even than QSOs if observed
quickly enough
less biased, probing more normal IGM
most likely, simply tracing SFR
QSOs and bright galaxies normally in strongly biased, clustered regions
host galaxy luminosity irrelevant for GRB detection
No proximity effect that is a major problem for quasars
Clean spectrum
almost single power-low SED, in contrast to QSOs or LAEs
GRBs are the best astronomical source for searching the red
damping wing of HI absorption in IGM
Probing the Reionization by the Red Damping
wing
GP trough in QSOs only gives a lower
limit of xHI >~10-3
The red damping wing, if detected, would
flux
GP trough
give a precise measurement of xHI
since optically thin, it is insensitive to any red damping wing
clumpiness of IGM
However, this method is problematic in wavelength
QSOs, since: 1215 (1+z) Å
proximity effect
complicated intrinsic spectra
GRBs are an ideal object to search this
red damping wing! (Milarda-Escude
1998)
GRB 050904 @ z=6.3
Swift Detection
Cusumano et al. ’05
GRB 050904, 3.4 days
(Kawai et al. ’06)
photometric colors of optical afterglows indicating z~6
Haislip et al. ’05, Price et al. ’05, Tagliaferri et al. ’05
optical spectroscopic observation by Subaru
3.4 days after the burst, z’ = 23.7
confirmed z=6.3 by: Haislip et al. ‘05
clear Lyman break
metal absroption line systems at z=6.295 ± 0.002
Signature of the Damping Wing!
Analysis of the Red Damping Wing to
Constrain the Reionization
two possibilities for the origin of the damping wing:
A damped Lyα system (DLA) associated with the host
galaxy
DLAs often found in GRB afterglows
log NHI (cm-2) ~ 21-22 GRB 030323 at z=3.372
(Vreeswijk et al. 2004)
IGM neutral hydrogen (damping wing of GP trough)
If detected, it would give a crucial information on xHI
Model Fitting
Intrinsic GRB afterglow spectrum
β= - 1.25±0.25 power-law (Fν∝ν-β)
~0.5 day observations by Haislip et al., Tagriaferri et al.
spectral change by cooling frequency break passage is unlikely
no evidence for extinction assume AV=0 at host (check later)
Galactic Extinction: E(B-V) = 0.066 mag
Absorptions by DLA and IGM
4 model parameters: zDLA, NHI, zIGM,u, xHI
DLA: τ= NHI σ[(1+z)νobs]
damping width >> reasonable velocity dispersion (<~200 km/s)
IGM: Formula of Miralda-Escude 1998
uniform IGM distributed from zIGM,l to zIGM,u
zIGM,l = 6.0 assumed in the baseline model
redshift range of IGM contributing the
damping wing at z~6.3
more than 80% (half) of IGM
optical depth is by IGM at z > 6
(6.2)
(zIGM,u = 6.3)
zDLA versus zmetal
zmetal = 6.295 ± 0.002 (no other redshift around z~6.3) ‘03
Mirabal+
fine-structure Si* detected ~pc scale from the burster
zDLA vs. zmetal?
zDLA = zmetal : straightforward, the baseline model
[S/H] ~ -1.3, [Si/H] ~ -2.9 for log NHI ~ 21.6
(large Si depletion is not rare in GRB afterglows)
zDLA = zhost, but different from zmetal
host galaxy must be very low metallicity of [Si/H] < -3 ... likely?
| zDLA – zhost | < ~ 0.005 (~200 km/s)
zmetal – zhost < ~ 0.07 (~3,000 km/s, by accelerated metal absorbing shell
around the GRB)
Vreeswijk et al. ‘04
-0.005 < zDLA – zmetal < +0.07
zIGM,u versus zmetal
zIGM,u vs. zmetal?
zIGM,u vs. zhost
ionized bubble size: zIGM,u – zhost ~ 0.02 (LAEs), 0.003 (theory for
typical GRBs at z~6; Barkana & Loeb 2004)
IGM gas infall to GRB host galaxies: negligible (Δz < 0.001)
-0.02 < zIGM,u – zmetal < +0.07
+0.07 comes from the possible accelerated shell for zmetal
Fitting Results: DLA? IGM? (1)
Totani et al. 2005
DLA model with z=6.295, log NHI = 21.62
Fitting Results: DLA? IGM? (2)
Both the DLA and IGM models can
explain the damping wing
(degeneracy!) zmetal = 6.295±0.002
marginally zDLA=zmetal allowed for
DLA
If IGM, zmetal must be blueshifted by
about 3,000 km/s
possible in GRBs!
First detection of almost
neutral IGM!?
Discrimination by LyβFeature
The degeneracy can be broken
by Lyβ profile!
The IGM model inconsistent
with the data
upper limit zIGM,u < 6.314
DLA is dominant under this
constraint
DLA
the plausible model: (zDLA=6.295)
zDLA=zmeteal = 6.295 IGM
xHI = 0 consistent with the data (zIGM,u=6.36)
but xHI=1 with zIGM,u=6.295
would affect the damping wing
Constraint on xHI?
What xHI is preferred, when NHI is
treated as a free parameter without any
prior? zero level: best fit with xHI=0
solid: best fit with xHI=1
zIGM,u = zDLA = 6.295
best fit xHI = 0.00 ± 0.17 The data obey to Gaussian well
xHI < 0.60 (95% C.L.)
The first upper limit on xHI at z>6!
Uncertainty Check
check done for spectral index, dust in host galaxy, redshift
parameters, weak absorption lines, and time variability
Totani et al. 2006, PASJ in press
Comparison with other Malhotra & Rhoads ’05
Stern et al. ’05
constraints Haiman & Cen ‘05
The constraint of xHI<0.6 at z=6.3 LAE statistics
GRB 050904
is consistent with those derived
from QSO (HII region size etc.)
and LAE statistics
The strength of the GRB
constraint :
derived directly from absorption
optical depth (like GP trough)
model uncertainty is very small
insensitive to clumpiness, giving
mass-averaged xHI along the sight
Fan et al. 2006
line
Prospects for future observations
low NHI GRBs?
only weak constraint on xHI when log NHI > 21.5
However, there are GRBs with log NHI <~ 20
promising chance for a better constraint on xHI
solid: DLA
long-dashed:
IGM+DLA(20.0)
Vreeswijk et al. ‘04
Prospects for future observations (2)
How often do we expect events like GRB 050904?
spectrum of GRB 050904 was 3.4 days. It would be x10 brighter if
0.5 day
If GRB 050904 occurred at z=1, R=17.9, F~0.2 mJy at 1 day one of
the brightest optical afterglows
NIR flash of GRB 050904 was as bright as the opt. flash of GRB
GRB050904
990123 (Boer et al. 05) rare object?
NIR spectroscopy necessary at z>7 lower sensitivity than optical
Panaitescu & Kumar 01
Fynbo et al. 01
Conclusions
GRB 050904 gave us the first constraint on reionization from
GRBs
Opened a new era of GRB cosmology
degeneracy: the red damping wing can be explained by DLA
or IGM
Lyβ feature can be used to break this degeneracy
In the case of GRB 050904, the DLA is dominant
Lower xHI at z~6-6.3 is preferred from our data
xHI = 0.00 ± 0.17, xHI < 0.60 (95% C.L.)
The IGM was largely reionized at z=6.3
The first quantitative upper limit on xHI at z>6 by a direct method
Identified Absorption Lines
Kawai et al. 2006
Prospects for future observations
low NHI GRBs?
only weak constraint on xHI when log NHI > 21.5
However, there are GRBs with log NHI <~ 20
promising chance for a better constraint on xHI
Lyα line emission from host galaxies?
line emissivity affected by xHI , giving a probe for reionization
solid: DLA
GRB host galaxies may have strong Lyα emission (in EW) (Jakobsson
long-dashed:
IGM+DLA(20.0)
et al. 2005)
Vreeswijk et al. ‘04
Lyα emission search for GRB host galaxies may also be interesting
For GRB 050904, we set upper limit on Lyα corresponding to SFR <
0.8 Msun/yr
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