2024ApJ...963L..46L


Query : 2024ApJ...963L..46L

2024ApJ...963L..46L - Astrophys. J., 963, L46 (2024/March-2)

Stochastic Wave Dark Matter with Fermi-LAT γ-Ray Pulsar Timing Array.

LUU H.N., LIU T., REN J., BROADHURST T., YANG R., WANG J.-S. and XIE Z.

Abstract (from CDS):

Pulsar timing arrays (PTAs) can detect disturbances in the fabric of spacetime on a galactic scale by monitoring the arrival time of pulses from millisecond pulsars (MSPs). Recent advancements have enabled the use of γ-ray radiation emitted by MSPs, in addition to radio waves, for PTA experiments. Wave dark matter (DM), a prominent class of DM candidates, can be detected with PTAs due to its periodic perturbations of the spacetime metric. In response to this development, we perform in this Letter a first analysis of applying the γ-ray PTA to detect the ultralight axion-like wave DM, with the data of Fermi Large Area Telescope (Fermi-LAT). Despite its much smaller collecting area, the Fermi-LAT γ-ray PTA demonstrates a promising sensitivity potential. We show that the upper limits not far from those of the dedicated radio-PTA projects can be achieved. Moreover, we initiate a cross-correlation analysis using the data of two Fermi-LAT pulsars. The cross-correlation of phases, while carrying key information on the source of the spacetime perturbations, has been ignored in the existing data analyses for the wave DM detection with PTAs. Our analysis indicates that taking this information into account can improve the sensitivity to wave DM by ≳50% at masses below 10–23 eV.

Abstract Copyright: © 2024. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Pulsar timing method - Gamma-ray astronomy - Dark matter

Simbad objects: 16

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Number of rows : 16
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 PSR J0030+0451 Psr 00 30 27.42348 +04 51 39.7144           ~ 596 1
2 2FGL J0312.5-0914 gam 03 12 06.2 -09 21 56           ~ 39 0
3 PSR B0613-02.0 Psr 06 13 43.977070 -02 00 47.34294           ~ 319 1
4 PSR J0614-3329 Psr 06 14 10.3479 -33 29 54.116           ~ 134 1
5 PSR J1231-1411 Psr 12 31 11.3069 -14 11 43.628           ~ 139 0
6 PSR J1513-2550 Psr 15 13 23.32059 -25 50 31.2850           ~ 35 0
7 PSR J1543-5149 Psr 15 43 44.145289 -51 49 54.71350           ~ 41 1
8 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
9 PSR J1630+3734 Psr 16 30 36.4672852 +37 34 42.101440           ~ 48 0
10 PSR J1741+1351 Psr 17 41 31.1499024 +13 51 44.279709           ~ 122 0
11 PSR J1858-2216 Psr 18 58 04.42 -22 19 13.7           ~ 39 0
12 PSR J1902-5105 Psr 19 02 02.8476 -51 05 56.969           ~ 64 0
13 PSR B1937+21.4 Psr 19 39 38.560096 +21 34 59.13552           ~ 1142 0
14 PSR J1959+2048 Psr 19 59 36.7643141520 +20 48 14.896407996   21.08 20.16 19.53 18.79 G: 854 3
15 PSR J2034+3632 Psr 20 34 59.9926758 +36 32 20.721130           ~ 30 0
16 PSR J2302+4442 Psr 23 02 46.9789 +44 42 22.102           ~ 124 0

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