2025ApJ...995L..53G


Query : 2025ApJ...995L..53G

2025ApJ...995L..53G - Astrophys. J., 995, L53 (2025/December-3)

The Formation Rate and Luminosity Function of Fast X-Ray Transients from Einstein Probe.

GUO Y., ZENG H., WEI J., ZHOU H., JIN Z., WU X. and WEI D.

Abstract (from CDS):

Following its launch on 2024 January 9, the Einstein Probe (EP) telescope has detected hundreds of fast X-ray transients (FXTs), yet their physical origins remain elusive. Understanding their luminosity function and formation rate is crucial for elucidating their nature. Recently, the EP team has provided the latest catalog of EP-detected FXTs. Based on this catalog, we present a model-independent nonparametric approach to derive the luminosity function and formation rate of FXTs. Our analysis reveals significant cosmological luminosity evolution, characterized by a scaling relationship of (1 + z)3.58. After accounting for this evolution, we establish that the local luminosity function is best represented by a broken power law, with a break luminosity of (4.17 ± 0.34) × 1046 erg s–1. The formation rate exhibits a broken power law as ρ(z) ∝ (1 + z)–4.25 at z ⪅ 0.9 and ρ(z) ∝ (1 + z)–0.26 at z ⪆ 0.9, yielding a local rate of approximately $153.{8}_{-95.1}^{+249.4}$ Gpc–3 yr–1. This rate is higher than that of long gamma-ray bursts (LGRBs). Our findings indicate that a component of FXTs is associated with LGRBs.

Abstract Copyright: © 2025. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): X-ray astronomy - X-ray transient sources - Gamma-ray bursts

Simbad objects: 39

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Number of rows : 39
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 EP 250827a ev 00 13 57 -56 27.8           ~ 3 0
2 EP 240806a ev 00 45 58 +05 05.5           ~ 4 0
3 EP 241021a ev 01 55 23.4 +05 56 18           ~ 17 0
4 EP 241107a ev 02 20 02.50 +03 20 01.8           ~ 5 0
5 EP 250827b ev 02 26 19 +37 29.9           ~ 3 0
6 EP 241217a ev 03 07 50 +30 54.1           ~ 6 0
7 SN 2025kg SN* 03 42 28.389 -22 30 21.28           SNIc-BL 26 0
8 GRB 241217A gB 05 36 40 -25 16.9           ~ 4 0
9 EP 250223a ev 06 33 02 -22 25.9           ~ 4 0
10 GRB 250205A gB 07 33 50 +32 21.9           ~ 2 0
11 EP 250205a ev 07 34 05 +32 21.8           ~ 4 0
12 GRB 250404A gB 08 20 14.4 -35 31 42           ~ 6 0
13 EP 241113a ev 08 47 59.1 +52 22 53           ~ 5 0
14 EP 240315a ev 09 26 35 -09 32.8           ~ 59 0
15 EP 250215a ev 10 25 22.3 -27 42 14           ~ 3 0
16 GRB 250215A gB 10 30 -34.5           ~ 3 0
17 EP 240408a ev 10 35 22 -35 44.9           ~ 12 0
18 GRB 240315C gB 10 37 22.0 +10 50 04           ~ 21 0
19 EP 250207b ev 11 10 03.1 -07 52 10           ~ 6 0
20 EP 250302a ev 11 18 03.580 +33 35 09.06           ~ 4 0
21 EP 250125a ev 11 41 27.39 -21 42 51.5           ~ 4 0
22 GRB 250321D gB 11 46 37 +10 21.1           ~ 1 0
23 EP 250321a ev 11 57 03.0 +17 21 46           ~ 4 0
24 SN 2024gsa SN* 12 46 01.669 -09 43 08.88           SNIc-BL 32 0
25 EP 250304a ev 13 53 35 -42 49.1           ~ 10 0
26 EP 240506a ev 14 15 54 -16 42.4           ~ 3 0
27 GRB 250226A gB 14 48 +23.8           ~ 3 0
28 EP 250226a ev 14 57 06 +20 58.4           ~ 5 0
29 EP 250430a ev 15 33 36 -18 07.8           ~ 1 0
30 GRB 250430A gB 15 33 43.0 -18 04 59           ~ 1 0
31 GRB 250416C gB 17 05 36 +25 46.1           ~ 3 0
32 GRB 250427A gB 18 29 07 +07 34.2           ~ 4 0
33 EP 250821a ev 19 19 25 -43 24.6           ~ 3 0
34 GRB 241026A gB 19 33 36.2 +57 59 09           ~ 6 0
35 GRB 250704B gB 20 03 29 +12 01.8           ~ 4 0
36 GRB 241025A gB 22 13 19 +83 34.0           ~ 3 0
37 EP 241025a ev 22 15 03 +83 34.0           ~ 2 0
38 GRB 240804B gB 22 30 35 -39 07.3           ~ 5 0
39 EP 240801a gB 23 00 34 +32 36.6           ~ 16 0

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