Detection of White Dwarf Companions to Blue Stragglers in the Open
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Draft version May 6, 2018 A Preprint typeset using LTEX style emulateapj v. 5/2/11 DETECTION OF WHITE DWARF COMPANIONS TO BLUE STRAGGLERS IN THE OPEN CLUSTER NGC 188: DIRECT EVIDENCE FOR RECENT MASS TRANSFER Natalie M. Gosnell1, Robert D. Mathieu1, Aaron M. Geller2,3, Alison Sills4, Nathan Leigh5,6, Christian Knigge7 Draft version May 6, 2018 ABSTRACT Several possible formation pathways for blue straggler stars have been developed recently, but no one pathway has yet been observationally confirmed for a specific blue straggler. Here we report the first findings from a Hubble Space Telescope ACS/SBC far-UV photometric program to search for white dwarf companions to blue straggler stars. We find three hot and young white dwarf companions to blue straggler stars in the 7-Gyr open cluster NGC 188, indicating that mass transfer in these systems ended less than 300 Myr ago. These companions are direct and secure observational evidence that these blue straggler stars were formed through mass transfer in binary stars. Their existence in a well-studied cluster environment allows for observational constraints of both the current binary system and the progenitor binary system, mapping the entire mass transfer history. Subject headings: open clusters and associations: individual (NGC 188) — binaries: spectroscopic — blue stragglers — white dwarfs — ultraviolet: stars 1. INTRODUCTION eccentricity distributions provide clues to their formation Blue straggler stars (BSSs), originally defined to be histories (Mathieu & Geller 2009, 2013). Of the 16 NGC anomalous stars more luminous and bluer than the main 188 BSSs in binaries, all but three have orbital periods sequence (MS) of a star cluster, are now known to near 1000 days. Statistical analysis of their secondary- be present in open star clusters (Johnson & Sandage mass distribution suggests that the companions to these 1955), globular clusters (Sandage 1953; Ferraro et al. BSSs have masses around 0.5 M⊙ (Geller & Mathieu 1999), the Galactic field (Preston & Sneden 2000), and 2011). Such masses suggest white dwarf (WD) compan- dwarf spheroidal galaxies (Momany et al. 2007). They ions, whose presence would indicate mass transfer as the define an alternative stellar evolution path, yet not a dominant BSS formation mechanism in NGC 188. rare one; BSSs comprise 25% of the evolved popula- The presence of a WD is detectable as an excess of tion in NGC 188 (Geller et al. 2008). Even so, the UV emission above the expected emission from a BSS formation of BSSs has been a puzzle for almost six alone. In this Letter we present the first results from decades. Recent work has identified several possible a Hubble Space Telescope (HST ) program searching for formation pathways, including mergers in hierarchical WD companions to the BSSs in NGC 188. We outline triples (Perets & Fabrycky 2009), collisions during dy- the observational design in § 2, the WD detections in namical encounters (Knigge et al. 2009; Leigh & Sills § 3, implications of these detections in § 4, mass transfer 2011), and mass transfer on the red giant branch (RGB) histories in § 5, and summarize our results in § 6. or asymptotic giant branch (AGB; Chen & Han 2008). 2. Yet no one pathway has yet been observationally con- OBSERVATIONS firmed for a specific BSS. NGC 188 contains 20 BSSs8 determined to be The open cluster NGC 188 contains one of the most three-dimensional members from radial-velocity (RV) thoroughly studied populations of BSSs in our Galaxy. and proper-motion (PM) studies (Platais et al. 2003; arXiv:1401.7670v1 [astro-ph.SR] 29 Jan 2014 Spectroscopic studies reveal that 80% of the BSSs in Geller et al. 2009). The population consists of 2 double- NGC 188 are in binaries, and their remarkable period and lined spectroscopic binaries, 14 single-lined spectroscopic binaries, and 4 stars that do not show velocity varia- This is WIYN Open Cluster Survey paper LVIII tions. In addition, there is one BSS candidate (WOCS [email protected] 1 4230) that is a PM member and velocity variable but Department of Astronomy, University of Wisconsin - Madi- son, 475 N. Charter St., Madison, WI 53706 whose rapid rotation does not permit sufficiently pre- 2 Center for Interdisciplinary Exploration and Research in As- cise velocities for a secure RV membership determina- trophysics (CIERA) and Department of Physics and Astronomy, tion. We observed the 14 single-lined binaries, the 4 Northwestern University, 2145 Sheridan Rd, Evanston, IL 60208 3 non-velocity variable BSSs, and WOCS 4230 using the Department of Astronomy and Astrophysics, University of Chicago, 5640 S. Ellis Avenue, Chicago, IL 60637 Advanced Camera for Surveys (ACS) Solar Blind Chan- 4 Department of Physics and Astronomy, McMaster Univer- nel (SBC) onboard HST. The non-velocity variable BSSs sity, 1280 Main St. W, Hamilton, ON L8S 4M1, Canada may still have very wide binary companions beyond the 5 Department of Physics, University of Alberta, CCIS 4-183, Edmonton, AB T6G 2E1, Canada RV sensitivity, so they are included in our observational 6 Department of Astrophysics, American Museum of Natural History, Central Park West and 79th Street, New York, NY 8 After the HST observations we discovered a V -band photomet- 10024 ric error for WOCS 1947, previously categorized as a BSS, which 7 School of Physics and Astronomy, University of Southamp- revealed it to be a RGB star. It is no longer considered a member ton, Highfield, Southampton, SO17 IBJ, UK of the NGC 188 BSS population (Mathieu & Geller 2013). 2 GOSNELL ET AL. study. We did not observe the two double-lined BSS bi- 18 naries as they have almost equal-mass companions that 11000 13250 15500 17750 20000 are already known to not be WDs. Each BSSs was White Dwarf Temperature (K) WOCS 4540 observed in a separate visit of 2 orbits, for a total of WOCS 5379 38 orbits (GO:12492, PI: Mathieu), using the F140LP, 20 F150LP, and F165LP filters with total exposure times of WOCS 4348 2040 s, 2380 s, and 1564 s, respectively. 2.1. Aperture Photometry F150N 22 % We use the astrodrizzle routine to create master driz- 30 % zled images in each filter for each target with a result- 90 ′′ −1 99% ing pixel scale of 0.025 pixel . We carry out aperture 50% 24 70% photometry using the IRAF package daophot with an aperture radius of 6 pixels, or an angular radius of 0.15′′. We then apply an encircled energy fraction correction to 0 1 2 3 4 our count rates based on aperture photometry of nor- F150N - F165LP malized TinyTim-modeled point sources9. We apply the same drizzling routine to the TinyTim source and carry Fig. 1.— Far-UV color-magnitude diagram showing the positions out aperture photometry, from which we calculate the of WOCS 4540, 5379, and 4348, each shown with 2-sigma error fraction of flux missed by our aperture. We find and ap- bars. The grey contours show the expected density distribution of ply encircled energy corrections of 0.83, 0.84, and 0.85 for single BSSs with temperature and luminosity distributions match- F140LP, F150LP, and F165LP, respectively. We calcu- ing the BSS population in NGC 188 (Mathieu & Geller 2009). The outermost contour encompasses 99% of single BSSs. The colored late our corrected count rates by dividing the measured lines track synthetic BSS-WD pairs with increasing WD tempera- count rate by the encircled energy correction. We con- ture as indicated by the color bar. The lower and upper solid lines vert our corrected count rates to instrument fluxes using follow binaries with BSS temperatures of 6,000 K and 6,500 K, re- the conversion factors given in the ACS Data Handbook spectively (Rodr´ıguez-Merino et al. 2005). The dashed lines track constant WD temperature from 11,000 K to 20,000 K in increments (Gonzaga et al. 2013). of 1,000 K (P. Bergeron, private communication). Comparing the The nested bandpasses of the HST /ACS/SBC long- observations with the synthetic BSS-WD models we determine that pass filters provide an opportunity to isolate the all three systems have WD companions with temperatures of ap- bluest UV flux. As shown in previous studies (e.g., proximately 13,000 K and above, which corresponds to an age of Dieball et al. 2005), one can difference the count rates less than 300 Myr. from the long-pass filters to create derived narrow band- 10,000 times and synthetically observed using the syn- passes. We create the derived filters of F140N = phot package to create the density contours plotted in (F140LP−F150LP) and F150N = (F150LP−F165LP). To photometer the count rates for these derived filters Figure 1. The outermost contour contains 99% of the ex- we difference the corrected long-pass filter count rates pected single-BSS distribution. The three detected BSSs and calculate fluxes by applying conversion rates of are much brighter and bluer than the single-BSS dis- tribution; they must have an additional source of UV −17 2 −1 −1 PHOTLAMSBC/F140N = 7.0631 × 10 erg cm A˚ count emission. × −17 2 ˚−1 −1. To illustrate that the UV fluxes for these sources are PHOTLAMSBC/F150N = 6 4868 10 erg cm A count straightforwardly explained by the presence of young, hot We find the conversion rates using the IRAF package WD companions, in Figure 2 we show model spectra of synphot and the tasks calcband and bandpar. After a BSS-WD binary compared to the narrow-band pho- finding the narrow-band fluxes we calculate magnitudes tometry for each of the three sources. The WD and BSS in all filters using STMAG = −2.5 log (flux) − 21.1. components are shown in blue and red, respectively, with 10 the combined spectrum shown in grey.