2018ApJ...852L..11S


Query : 2018ApJ...852L..11S

2018ApJ...852L..11S - Astrophys. J., 852, L11-L11 (2018/January-1)

The dispersion of fast radio bursts from a structured intergalactic medium at redshifts z < 1.5.

SHULL J.M. and DANFORTH C.W.

Abstract (from CDS):

We analyze the sources of free electrons that produce the large dispersion measures, DM~300–1600 (in units of cm–3 pc), observed toward fast radio bursts (FRBs). Individual galaxies typically produce DM∼25–60 cm–3 pc from ionized gas in their disk, disk-halo interface, and circumgalactic medium. Toward an FRB source at redshift z, a homogeneous intergalactic medium (IGM) containing a fraction fIGM of cosmological baryons will produce DM=(935 cm–3 pc)fIGM h70–1I(z), where I(z)=(2/3Ωm)[Ωm(1+z)3+ΩΛ1/2-1]. A structured IGM of photoionized Lyα absorbers in the cosmic web produces similar dispersion, modeled from the observed distribution, fb(N,z), of H I (Lyα-forest) absorbers in column density and redshift with ionization corrections and scaling relations from cosmological simulations. An analytic formula for DM(z) applied to observed FRB dispersions suggests that zFRB ~0.2–1.5 for an IGM containing a significant baryon fraction, fIGM=0.6 ±0.1. Future surveys of the statistical distribution, DM(z), of FRBs identified with specific galaxies and redshifts can be used to calibrate the IGM baryon fraction and distribution of Lyα absorbers. Fluctuations in DM at the level ±10 cm–3 pc will arise from filaments and voids in the cosmic web.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): cosmological parameters - cosmology: observations - intergalactic medium - ultraviolet: galaxies - ultraviolet: galaxies

CDS comments: FRB 101125 is a probable misprint for FRB 010125 and FRB 131014 is a probable misprint for FRB 131104.

Simbad objects: 25

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Number of rows : 25
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 FRB 010724 rB 01 18 06.0 -72 12 19           ~ 94 1
2 FRB 090625 rB 03 07 47.0 -29 55 35           ~ 39 0
3 FRB 20181119D rB 05 31 58.6980 +33 08 52.588           ~ 933 0
4 FRB 131104 rB 06 44 10.4 -51 16 40           ~ 83 0
5 FRB 150418 rB 07 16 30.9 -19 02 24           ~ 120 0
6 FRB 160608 rB 07 36 42.0 -40 47 52           ~ 17 0
7 FRB 160317 rB 07 53 47.0 -29 36 31           ~ 22 0
8 FRB 160410 rB 08 41 25.0 +06 05 05           ~ 18 0
9 FRB 130628 rB 09 03 02.0 +03 26 16           ~ 42 0
10 FRB 151230 rB 09 40 50.0 -03 27 05           ~ 31 0
11 FRB 150610 rB 10 44 26.0 -40 05 23           ~ 19 0
12 FRB 170107 rB 11 23 10 -05 01.0           ~ 27 0
13 FRB 130729 rB 13 41 21.0 -05 59 43           ~ 46 0
14 FRB 130626 rB 16 27 06.0 -07 27 48           ~ 40 0
15 FRB 121002 rB 18 14 47.0 -85 11 53           ~ 57 0
16 NAME FRB J1852-08 rB 18 52 05.0 -08 29 35           ~ 54 0
17 FRB 010125 rB 19 06 53.00 -40 37 14.4           ~ 46 1
18 FRB 151206 rB 19 21 25.0 -04 07 54           ~ 18 0
19 FRB 110626 rB 21 03 43.0 -44 44 19           ~ 49 1
20 FRB 110523 rB 21 45 31.0 -00 15 23           ~ 91 0
21 FRB 140514 rB 22 34 06.20 -12 18 46.5           ~ 80 0
22 FRB 110220 rB 22 34 38.0 -12 33 44           ~ 82 0
23 FRB 20160102A rB 22 38 49.0 -30 10 50           ~ 41 0
24 FRB 120127 rB 23 15 06.0 -18 25 37           ~ 51 0
25 FRB 110703 rB 23 30 51.0 -02 52 24           ~ 54 0

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