The advection-dominated accretion flow for the anti-correlation between the X-ray photon index and the X-ray luminosity in neutron star low-mass X-ray binaries

preprint2020arXivOpen access

Abstract

Observationally, an anti-correlation between the X-ray photon index ΓΓ (obtained by fitting the X-ray spectrum between 0.5 and 10 keV with a single power law) and the X-ray luminosity L0.5−10keVL_{\rm 0.5-10keV}, is found in neutron star low-mass X-ray binaries (NS-LMXBs) in the range of L0.5−10keV∼1034−1036 erg s−1L_{\rm 0.5-10keV}\sim 10^{34}-10^{36}\ \rm erg\ s^{-1}. In this paper, we explain the observed anti-correlation between ΓΓ and L0.5−10keVL_{\rm 0.5-10keV} within the framework of the self-similar solution of the advection-dominated accretion flow (ADAF) around a weakly magnetized NS. The ADAF model intrinsically predicts an anti-correlation between ΓΓ and L0.5−10keVL_{\rm 0.5-10keV}. In the ADAF model, there is a key parameter, fthf_{\rm th}, which describes the fraction of the ADAF energy released at the surface of the NS as thermal emission to be scattered in the ADAF. We test the effect of fthf_{\rm th} on the anti-correlation between ΓΓ and L0.5−10keVL_{\rm 0.5-10keV}. It is found that the value of fthf_{\rm th} can significantly affect the anti-correlation between ΓΓ and L0.5−10keVL_{\rm 0.5-10keV}. Specifically, the anti-correlation between ΓΓ and L0.5−10keVL_{\rm 0.5-10keV} becomes flatter with decreasing fthf_{\rm th} as taking fth=0.1,0.03,0.01,0.005f_{\rm th}=0.1, 0.03, 0.01, 0.005, 0.0030.003 and 00 respectively. By comparing with a sample of non-pulsating NS-LMXBs with well measured ΓΓ and L0.5−10keVL_{\rm 0.5-10keV}, we find that indeed only a small value of 0.003≲fth≲0.10.003\lesssim f_{\rm th}\lesssim 0.1 is needed to match the observed anti-correlation between ΓΓ and L0.5−10keVL_{\rm 0.5-10keV}. Finally, we argue that the small value of fth≲0.1f_{\rm th}\lesssim 0.1 derived in this paper further confirms our previous conclusion that the radiative efficiency of NSs with an ADAF accretion may not be as high as ε∼M˙GMR∗/M˙c2∼0.2ε\sim {\dot M GM\over R_{*}}/{\dot M c^2}\sim 0.2.

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