# Observing the transient pulsations of SMC X-1 with NuSTAR

## TL;DR

This study uses NuSTAR observations to analyze transient pulsations in SMC X-1, revealing that pulsation variability is likely caused by changing obscuration rather than flux changes, and suggesting parallels with ultraluminous X-ray pulsars.

## Contribution

It demonstrates that pulsation appearance in SMC X-1 is linked to obscuration effects, providing insights into the variability mechanisms of high-luminosity X-ray pulsars.

## Key findings

- Pulsations switch on and off without large flux changes.
- Spectral shape remains consistent across states, with variability due to obscuration.
- SMC X-1's luminosity suggests it as an analog to ULXPs.

## Abstract

We report on NuSTAR observations of transient pulsations in the neutron star X-ray binary SMC X-1. The transition from non-pulsing to pulsing states was not accompanied by a large change in flux. Instead, both pulsing and non-pulsing states were observed in a single observation during the low-flux super-orbital state. During the high-state, we measure a pulse period of $P = 0.70117(9)\,\mathrm{s}$ at $T_{ref} = 56145\,\mathrm{MJD}$. Spectral analysis during non-pulsing and pulsing states reveals that the observations can be consistently modeled by an absorbed power law with a phenomenological cutoff resembling a Fermi-Dirac distribution, or by a partially obscured cutoff power law. The shapes of the underlying continua show little variability between epochs, while the covering fraction and column density vary between super-orbital states. The strength of pulsations also varies, leading us to infer that the absence and reemergence of pulsations are related to changing obscuration, such as by a warped accretion disk. SMC X-1 is accreting near or above its Eddington limit, reaching an unabsorbed X-ray luminosity of $L_{\rm X}({\rm 2-10~keV}) \approx 5 \times 10^{38}\, {\rm erg}\, {\rm s}^{-1}$. This suggests that SMC X-1 may be a useful local analog to ultraluminous X-ray pulsars (ULXPs), which likewise exhibit strong variability in their pulsed fractions, as well as flux variability on similar timescales. In particular, the gradual pulse turn-on which has been observed in M82 X-2 is similar to the behavior we observe in SMC X-1. Thus we propose that pulse fraction variability of ULXPs may also be due to variable obscuration.