2023MNRAS.525.2054L


Query : 2023MNRAS.525.2054L

2023MNRAS.525.2054L - Mon. Not. R. Astron. Soc., 525, 2054-2068 (2023/October-3)

EOS-dependent millihertz quasi-periodic oscillation in low-mass X-ray binary.

LIU H., GAO Y., LI Z., DOHI A., WANG W., LU G. and XU R.

Abstract (from CDS):

We studied the frequency and critical mass accretion rate of millihertz quasi-periodic oscillations (mHz QPOs) using a one-zone X-ray burst model. The surface gravity is specified by two kinds of equation of states: neutron star (NS) and strange star (SS). The base flux, Qb, is set in the range of 0-2 MeV nucleon–1. It is found that the frequency of mHz QPO is positively correlated to the surface gravity but negatively to the base heating. The helium mass fraction has a significant influence on the oscillation frequency and luminosity. The observed 7-9 mHz QPOs can be either explained by a heavy NS/light SS with a small base flux or a heavy SS with a large base flux. As base flux increases, the critical mass accretion rate for marginally stable burning is found to be lower. Meanwhile, the impact of metallicity on the properties of mHz QPOs was investigated using one-zone model. It shows that both the frequency and critical mass accretion rate decrease as metallicity increases. An accreted NS/SS with a higher base flux and metallicity, combined with a lower surface gravity and helium mass fraction, could be responsible for the observed critical mass accretion rate ($\dot{m}\simeq 0.3\dot{m}_{\rm Edd}$). The accreted fuel would be in stable burning if base flux is over than ∼2 MeV nucleon–1. This finding suggests that the accreting NSs/SSs in low-mass X-ray binaries showing no type I X-ray bursts possibly have a strong base heating.

Abstract Copyright: © 2023 The Author(s) Published by Oxford University Press on behalf of Royal Astronomical Society

Journal keyword(s): accretion - stars:neutron star - X-rays: burst

Simbad objects: 15

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Number of rows : 15
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 V* V1037 Cas LXB 00 29 03.06 +59 34 19.0           ~ 283 1
2 V* V635 Cas HXB 01 18 31.9704955824 +63 44 33.072603144 17.05 16.64 15.19 14.34 13.22 B0.2Ve 791 0
3 PSR J0348+0432 Psr 03 48 43.6363173480 +04 32 11.461921260           ~ 311 2
4 HD 245770 HXB 05 38 54.5748918624 +26 18 56.836952784 9.30 9.84 9.39 8.77 8.30 O9/B0III/Ve 1045 0
5 PSR J0740+6620 Psr 07 40 45.799 +66 20 33.60           ~ 395 0
6 V* UY Vol LXB 07 48 33.71 -67 45 07.7 16.10 17.00 16.9 16.7 17.05 ~ 660 0
7 4U 1323-62 LXB 13 26 37.0 -62 08 09           ~ 192 0
8 V* QX Nor LXB 16 12 43.0 -52 25 26           ~ 946 1
9 PSR J1614-2230 Psr 16 14 36.50974 -22 30 31.5420           ~ 452 1
10 V* V801 Ara LXB 16 40 55.5976953528 -53 45 04.948107156 17.50 18.20 17.5   17.07 ~ 921 0
11 4U 1730-22 LXB 17 33 57.00 -22 02 07.0           ~ 64 0
12 IGR J17480-2446 LXB 17 48 04.831 -24 46 48.87           ~ 204 0
13 1RXS J180408.9-342058 LXB 18 04 08.9 -34 20 58           ~ 75 0
14 V* V4634 Sgr LXB 18 29 28.8 -23 47 48 18.90 19.40 19     ~ 399 0
15 X Aql X-1 LXB 19 11 16.0571313336 +00 35 05.868232692           ~ 1186 1

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