A Search for Radio Pulsations from Neutron Star Companions of Four

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A Search for Radio Pulsations from Neutron Star Companions of Four Astronomy & Astrophysics manuscript no. 16098˙arxiv c ESO 2018 November 15, 2018 A search for radio pulsations from neutron star companions of four subdwarf B stars Thijs Coenen1, Joeri van Leeuwen2,1, and Ingrid H. Stairs3 1 Astronomical Institute ”Anton Pannekoek,” University of Amsterdam, P.O. Box 94249, 1090 GE, Amsterdam, The Netherlands 2 Stichting ASTRON, PO Box 2, 7990 AA Dwingeloo, The Netherlands 3 Dept. of Physics and Astronomy, University of British Columbia, 6224 Agricultural Road, Vancouver, B.C., V6T 1Z1 Canada ABSTRACT We searched for radio pulsations from the potential neutron star binary companions to subdwarf B stars HE 0532-4503, HE 0929- 0424, TON S 183 and PG 1232-136. Optical spectroscopy of these subdwarfs has indicated they orbit a companion in the neutron star mass range. These companions are thought to play an important role in the poorly understood formation of subdwarf B stars. Using the Green Bank Telescope we searched down to mean flux densities as low as 0.2 mJy, but no pulsed emission was found. We discuss the implications for each system. 1. Introduction Several such binary formation channels have been hypoth- esized. For an sdB to form, a light star must lose most of its The study of millisecond pulsars (MSPs) enables several types hydrogen envelope and ignite helium in its core. In these binary of research in astrophysics, ranging from binary evolution (e.g. systems, sdB stars can be formed through phases of Common Edwards & Bailes, 2001), to the potential detection of back- Envelope evolution where the envelope is ejected, or through ground gravitational radiation using a large set of pulsars with stable Roche Lobe overflow stripping the donor star of its hydro- stable timing properties (Jaffe & Backer, 2003). Furthermore, gen envelope. Binary population synthesis models for the above high-precision timing provides opportunities for fundamental scenarios in the case of white-dwarf companions were recently physics research: by measuring and modeling pulse arrival times compared by Han et al. (2003) and Hu et al. (2007). from binary systems, one can constrain neutron star masses and Specifically interesting for finding new millisecond pul- equations of state (Demorest et al., 2010), or study strong-field sars, is the channel that leads to short-period binary systems general relativity (Taylor & Weisberg, 1989). containing an sdB star and a neutron star or a black hole Finding such millisecond pulsars is done through wide-area (Podsiadlowski et al., 2002; Geier et al., 2010). Here, the binary surveys or through targeted surveys, each with specific advan- system contains a star that is massive enough to evolve into a tages: with limited telescope time, a directed search can afford neutron star or a black hole and a secondary, lighter star that is to dwell on a specifically interesting part of the sky for longer the progenitor of the sdB star. The secondary is in a wide or- than an undirected search. A directed search is therefore more bit with a period of about 20 years. The system undergoes two sensitive to faint pulsars in specific locations than an undirected phases of common envelope evolution, a supernova and a short search would be that only incidentally scans oversuch a location. X-ray binary phase. A first common envelope phase starts soon An undirected search however covers a larger area. Directed after the primary becomes a red supergiant and starts overflow- searches have targeted sources associated with MSPs, such as ing its Roche Lobe. During this first common envelope phase globular clusters (Ransom et al., 2005), steep spectrum sources the orbit of the binary shrinks. After the subsequent supernova, (Backer et al., 1982), unidentified Fermi sources (Ransom et al., the primary leaves a neutron star or black hole. This neutron 2011) and low mass-white dwarfs (van Leeuwen et al., 2007; star remains visible as a normal radio pulsar for on average Ag¨ueros et al., 2009). Here we report the results of a directed 107−8 years, and turns off. Once the secondary evolves off the arXiv:1106.2053v1 [astro-ph.GA] 10 Jun 2011 search for radio pulsations from four short-orbit sub-luminous B main sequence the second phase of mass transfer starts when the dwarf (sdB) binaries identified through spectroscopy as possibly secondary begins to overflow its Roche Lobe. The system un- containing neutron stars (Geier et al., 2008). dergoes a short X-ray binary phase, in which the neutron star Sub-luminous B dwarfs are some of the most abundant faint is recycled (Bhattacharya & van den Heuvel, 1991). The second blue objects (Green et al., 1986). They are thought to be light common-envelope phase starts shortly thereafter, further shrink- (about 0.5 M⊙) core helium burning stars with very thin hy- ing the orbit of the binary and dissipating the envelope of the drogen envelopes. After the helium burning in the core stops, secondary. The secondary, which is now mostly stripped of its sdB stars evolve directly to the white dwarf cooling sequence hydrogen envelope, ignites helium in its core and continues its (cf. a recent review by Heber, 2009). In their survey of sub- evolution as a sdB star (Podsiadlowski et al., 2002; Geier et al., dwarf B stars Maxted et al. (2001) find that 2/3 of field sdB 2010). From population modeling, Pfahl et al. (2003) find that stars are in short-orbit (P <∼ 10 days) binaries. Taking into ac- about 1% of sdB stars evolve as outlined above and orbit a neu- count the insensitivity of their survey to longer-period binaries, tron star or black hole. In such systems the secondary is an sdB Maxted et al. (2001) conclude that binary star evolution is fun- star for ∼ 108 years (Heber, 2009), before evolving to a white damental to the formation of sdB stars. dwarf. 2 Thijs Coenen et al.: A search for radio pulsars in four subdwarf B star binaries While low-mass companions (white dwarfs, main se- Object tint P DM Peak S/N −3 quence stars) to sdB stars have been optically confirmed (e.g. (s) (ms) (pc cm ) Geier et al., 2010), the unambiguous identification of a high- PSR J0034-0534 60 1.877 13.8 22 PSR B0450-18 30 549.0 39.9 115 mass companion in the form of a radio pulsar would provide PSR B1257+12 30 6.219 10.2 15 further constraints on the relative likelihood of different binary evolution models (as was similarly done for companions of low- Table 2. List of the previously known pulsars that were used as a mass white dwarfs in van Leeuwen et al., 2007). Furthermore, check of the telescope, back-end and pulsar-search systems. Test timing of a possible MSP companion will likely provide an sdB source PSRJ0034-0534 is in a short-orbit 1.6-day binary witha mass measurement, either through the modeling of the orbital 0.16 M⊙ companion (Bailes et al., 1994). parameters, or more directly and precisely through a Shapiro delay measurement (e.g. Ferdman et al., 2010). As millisec- ond pulsars can turn on shortly after the cessation of accretion 8 (Archibald et al., 2009) and can shine for more than the ∼ 10 For each system in our sample, we derived the expected year sdB star lifetime, MSPs will be active throughout the sdB dispersion measures (DM) from their measured distance, us- star phase. Thus, non-detections of radio pulsations from these ing the NE 2001 free electron model (Cordes & Lazio, 2002). systems could mean the absence of any neutron star, the pres- These expected DMs, listed in Table 1, are all well below ence of only a very weak radio pulsar, or of a brighter one that 100pc cm−3. Up to 200pccm−3 the trial DMs were spaced is beamed away from Earth. Non-detections in a large enough such that our search remains sensitive to pulsars with rota- sample of sdB stars eventually provide statistics on sdB forma- tional periods down to 1 ms; faster pulsars are not generally tion channels. expected (Chakrabarty et al., 2003). Beyond 200pc cm−3 the In Section 2 we describe how sources were selected; in intra-channel smearing begins to dominate, so trial DMs up to Section 3 our observing and data reduction setup is outlined. 1000pc cm−3 where created at a lower time resolution. We next Section 4 contains our results. In Section 5 we discuss these searched these trial DMs for pulsar signals, in both the time and results and compare to recent optical results on some of our frequency domain, using the PRESTO data reduction package sources. (Ransom, 2001). In the time domain we searched for single dis- persed pulses of radio emission. In the frequency-domainsearch 2. Source selection we have to take into account the acceleration present in these binary systems. One could potentially derive the neutron-star or- Our source selection was based on the report by Geier et al. bital phase from the optical modulation of the sdB star, and thus (2008) of the detection of the first four sdB systems that possibly estimate the acceleration at the time of the observations. This contain a neutron star or black hole companion: HE0532-4503, however relies on the assumption that there is no lag between HE0929-0424, TONS183 and PG1232-136. the optical light curve and the orbital motion. We have taken the These candidate sdB - neutron star (sdB-NS) systems were conservative approach to search over the full range of possible identified through spectroscopic observations of sdB binaries accelerations throughout the orbit. As each integration time tint (Geier et al., 2008).
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