2005ApJ...627....1F


Query : 2005ApJ...627....1F

2005ApJ...627....1F - Astrophys. J., 627, 1-25 (2005/July-1)

Toward a more standardized candle using gamma-ray burst energetics and spectra.

FRIEDMAN A.S. and BLOOM J.S.

Abstract (from CDS):

The use of gamma-ray burst (GRB) energetics for cosmography has long been advanced as a means to probe out to high redshifts, to the epoch of deceleration. However, although relatively immune to systematic biases from dust extinction, the prompt energy release in GRBs, even when corrected for jetting geometry, is far from being a standard candle. In this work we explore the cosmographic potential of a GRB standard candle based on the newly discovered relation by Ghirlanda and coworkers between the apparent geometry-corrected energies (Eγ) and the peak in the rest-frame prompt-burst spectrum (Ep). We present an explicit, self-consistent formalism for correcting GRB energies with a thorough accounting for observational uncertainties. In contrast to other work, we demonstrate that the current sample of 19 GRBs is not yet cosmographically competitive with results from Type Ia supernovae (SNe Ia), large-scale structure, and the microwave background. Although the Ep-Eγrelation is a highly significant correlation across a range of cosmologies [0≤ΩM, ΩΛ≤2], the goodness of fit of the data to a power law (Ep∝Eηγ) depends strongly on input assumptions. The most important of these assumptions concern the unknown density (and density profile) of the circumburst medium, the efficiency of converting explosion energy to gamma rays, data selection choices for individual bursts (some of which were not included in similar work), and assumptions in the error analysis. Independent of assumptions, with very few low-z bursts, the current sample is most sensitive to ΩMbut essentially insensitive to ΩΛ(let alone the dark energy equation of state w). The relation clearly represents a significant improvement in the search for an empirical GRB standard candle but is further hindered by an unknown physical basis for the relation, the lack of a low-z training set to calibrate the relation in a cosmology-independent way, and several major potential systematic uncertainties and selection effects. Until these concerns are addressed, a larger sample is acquired, and attempts are made to marginalize or perform Monte Carlo simulations over the unknown density distribution (which itself may evolve with redshift), we urge caution concerning claims of the utility of GRBs for cosmography and especially attempts to combine the results from GRBs with those of SNe Ia.

Abstract Copyright: ∼

Journal keyword(s): Cosmology: Cosmological Parameters - Cosmology: Observations - Gamma Rays: Bursts

Nomenclature: Table 1: XRF YYMMDDA N=52.

Simbad objects: 53

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Number of rows : 53
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 GRB 021004 gB 00 26 54.68 +18 55 41.6           ~ 560 0
2 GRB 041006 gB 00 54 50.17 +01 14 07.0           ~ 202 2
3 GRB 000210 gB 01 59 15 -40 40.0           ~ 175 0
4 GRB 040924 gB 02 06 22.52 +16 08 48.8           ~ 169 1
5 GRB 000911 gB 02 18 42 +07 48.0           ~ 163 0
6 GRB 970228 gB 05 01 46.7 +11 46 53           ~ 650 1
7 GRB 991216 gB 05 09 31.2983 +11 17 07.262           ~ 430 0
8 GRB 990705 gB 05 09 54.5 -72 07 53           ~ 229 1
9 GRB 000131 gB 06 13 31.08 -51 56 41.7     24.7     ~ 172 1
10 GRB 970508 gB 06 53 49.2 +79 16 19           ~ 883 1
11 GRB 980329 gB 07 02 41 +38 50.7           ~ 276 1
12 SN 2003lw SN* 08 02 30.1 -39 51 03       20.23   SNIc: 576 0
13 SN 2002lt SN* 08 08 59.858 +06 43 37.52           SNIc: 363 1
14 GRB 980326 gB 08 36 34.3 -18 51 24           ~ 268 0
15 GRB 020124 gB 09 32 50.8 -11 31 11           ~ 155 0
16 GRB 980613 gB 10 17 57.8 +71 27 26           ~ 204 1
17 SN 2003dh SN* 10 44 50.030 +21 31 18.15     16.2     SNIcpec 1261 1
18 GRB 030323 gB 11 06 09.4 -21 46 13           ~ 138 1
19 GRB 011211 gB 11 15 16 -21 56.0           ~ 305 0
20 GRB 030115 gB 11 18 32.6 +15 02 59           ~ 90 1
21 GRB 030226 gB 11 33 04.9 +25 53 56           ~ 212 0
22 GRB 011121 gB 11 34 26.67 -76 01 41.6       23.0   ~ 286 1
23 GRB 990506 gB 11 54 41 -26 45.0           ~ 169 1
24 GRB 971214 gB 11 56 26.4 +65 12 01           ~ 445 1
25 GRB 030328 gB 12 10 48.4 -09 20 51           ~ 148 0
26 GRB 030429 gB 12 13 07.495 -20 54 49.54     23.70     ~ 132 0
27 GRB 000418 gB 12 25 21 +20 05.0           ~ 219 0
28 SN 1997ff SN* 12 36 44.10 +62 12 44.7         26.77 SNIa 67 1
29 GRB 020331 gB 13 16 09.5 -17 55 16           ~ 40 0
30 GRB 030324 gB 13 37 04.4 -00 15 34           ~ 36 0
31 GRB 990510 gB 13 38 07.64 -80 29 48.8           ~ 499 1
32 GRB 020405 gB 13 58 03.12 -31 22 22.2   21.9 21.5     ~ 259 1
33 GRB 000630 gB 14 47.2 +41 13           ~ 53 1
34 GRB 040511 gB 14 47.8 -44 15           ~ 20 0
35 GRB 010222 G 14 52 12.5 +43 01 06           ~ 364 1
36 GRB 990123 gB 15 25 29 +44 45.0     8.95     ~ 1012 1
37 GRB 000301C gB 16 20 18.5 +29 26 35           ~ 361 0
38 GRB 991208 gB 16 33 53.51 +46 27 21.5           ~ 269 1
39 GRB 030528 gB 17 04 00.3 -22 37 10           ~ 90 1
40 GRB 000926 gB 17 04 15 +51 46.0           ~ 373 0
41 GRB 970828 gB 18 08 31.6 +59 18 51           ~ 353 1
42 GRB 000214 gB 18 54 27.0 -66 27 30           ~ 92 0
43 SN 1998bw SN* 19 35 03.17 -52 50 46.1   14.09       SNIc 1928 2
44 GRB 020813A gB 19 46 41.874 -19 36 04.81           ~ 316 0
45 GRB 040701 G 20 47 46.3 -40 14 13           ~ 45 1
46 GRB 030723 gB 21 49 24.40 -27 42 47.4           ~ 130 0
47 GRB 020427 gB 22 09 28.3 -65 19 32           ~ 50 0
48 GRB 990712 gB 22 31 53.061 -73 24 28.58           ~ 268 1
49 GRB 020903 gB 22 48 42.34 -20 46 09.3           ~ 248 1
50 GRB 010921 gB 22 55 59.90 +40 55 52.9           ~ 173 1
51 GRB 980519 gB 23 22 21.5 +77 15 43           ~ 203 0
52 GRB 981226 gB 23 29 37.2 -23 55 54           ~ 108 1
53 GRB 980703 gB 23 59 06.7 +08 35 07           ~ 453 1

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