The Curious Case of ASAS J174600-2321.3: an Eclipsing Symbiotic Nova in Outburst?
Stefan Huemmerich, Sebastian Otero, Patrick Tisserand, Klaus Bernhard
HHümmerich, et al. , JAAVSO Volume 43, 2015 1
1. Introduction
ASAS J174600-2321.3 = EROS2-cg1131n13463 = 2MASS J17460018-2321163, which is situated in Sagittarius at position (J2000) R.A. 17 h m s Dec. –23º 21' 16.37" (UCAC4; Zacharias et al. et al. et al. et al.
The Curious Case of ASAS J174600-2321.3: an Eclipsing Symbiotic Nova in Outburst?
Stefan Hümmerich
Stiftstr. 4, Braubach, D-56338, Germany; American Association of Variable Star Observers (AAVSO), Cambridge, MA;Bundesdeutsche Arbeitsgemeinschaft für Veränderliche Sterne e.V. (BAV), Berlin, Germany; [email protected]
Sebastián Otero
Olazabal 3650-8 C, Buenos Aires, 1430, Argentina; American Association of Variable Star Observers (AAVSO), Cambridge, MA
Patrick Tisserand
Sorbonne Universités, UPMC Univ Paris 06, UMR 7095, Institut d’Astrophysique de Paris, F-75005 Paris, France;CNRS, UMR 7095, Institut d’Astrophysique de Paris, 98 bis Boulevard Arago, F-75014 Paris, France
Klaus Bernhard
Kafkaweg 5, Linz, 4030, Austria; American Association of Variable Star Observers (AAVSO), Cambridge, MA;Bundesdeutsche Arbeitsgemeinschaft für Veränderliche Sterne e.V. (BAV), Berlin, GermanyReceived October 15, 2014; revised November 25, 2014; accepted December 15, 2014
Abstract
The star ASAS J174600-2321.3 was found to exhibit peculiar photometric variability (conspicuous brightening of ~4 magnitudes (V), fast luminosity declines, intrinsic pulsations). It was rejected as an RCB candidate in recent investigations on spectroscopic grounds. We have collected and present all available data from public sky surveys, photometric catalogues, and the literature. From an analysis of these data, we have identified ASAS J174600-2321.3 as a long-period eclipsing binary (P orb = 1,011.5 days). The primary star, which is probably a white dwarf, is currently in outburst and exhibits the spectral characteristics of a reddened, early F-type supergiant; the secondary star is a giant of spectral type late M. We discuss the possible origin of the observed brightening, which is related to the primary component. ASAS J174600-2321.3 is most certainly an eclipsing symbiotic binary—probably a symbiotic nova of GCVS type NC—that is currently in outburst. However, further photometric and spectroscopic data are needed to confirm this.
Table 1. Identifications and coordinates of ASAS J174600-2321.3. Positional data were taken from UCAC4. Identifiers R.A. (J2000) Dec. (J2000) Galactic Galactic h m s º ' " Longitude (º) Latitude (º)
ASAS J174600-2321.3 17 46 00.180 –23 21 16.37 2.829 4.814
EROS2-cg1131n13463 2MASS J17460018-2321163
USNO-B1.0 0666-0562145 various sky surveys, photometric catalogues, and the literature; they are presented in Section 2 and analyzed and interpreted in Section 3. Possible reasons for the rise in magnitude and probable classifications are discussed in Section 4. We conclude in Section 5.
2. Observations et al. ümmerich, et al. , JAAVSO Volume 43, 20152 measured and predicted colors of a star. Their results prefer an R V = 3.1 Fitzpatrick (1999) reddening law. Based on the calculations of Schlafly and Finkbeiner (2011), we estimate an interstellar extinction of A V ≈ 2.4 mag. and E(B–V) ≈ 0.78 mag. for the sky area of our interest. The extinction values in different bandpasses, which have been used for the reddening correction in the present paper, were accessed through the NASA/IPAC Infrared Science Archive (http://irsa.ipac.caltech.edu/applications/DUST/). If not indicated otherwise, the light curves illustrated in this and the following sections are based on non-corrected data. In order to achieve a long time baseline, we have combined photometric observations from the EROS-2 project (Renault et al. et al. et al. (2007):R eros = I C B eros = V J − 0.4(V J − I C ) (1)The obtained results are accurate to a precision of 0.1 mag. (Tisserand et al. E data after HJD 2452200. Thus, no contemporaneous R E measurements were available to transform the B E values after HJD 2452200 using Equation (1). The missing data have been linearly interpolated in such a way that the resulting data forms a continuity with the preceding EROS-2 and succeeding ASAS-3 measurements. We have achieved this by using Equation (2), which has been derived from the conversion of data before HJD 2452200. As the system brightened considerably during the time of the missing R E measurements, and the brightening is obviously related to the hot primary component, we have also taken into account the resulting color changes and have adapted the equation accordingly. (As primary star, we define the star which is the seat of the observed brightening and which we propose as possible accretor in a symbiotic binary scenario.)ΔI C = 0.57 × ΔB E (2)As can be seen from the resulting light curve, there is very good agreement between the converted EROS-2 and ASAS-3 data. Furthermore, the derived color index from the resulting data, (V–I C ) eros = 1.9 mag. at V ≈ 13.0 mag., is consistent with the index derived from APASS photometry at maximum brightness, (V–I C ) apass = 1.5 mag. at V ≈ 12.2 mag. We thus feel confident about the applicability of our solution. The combined light curve of ASAS J174600-2321.3, based mainly on sky survey data from EROS-2, ASAS-3, and APASS, is shown in Figure 1; APASS measurements are presented in Table 2. During the beginning of EROS-2 coverage, the star’s brightness varied slowly around 16.5 mag. (V). A rise in magnitude set in at around HJD 2451240, with the system reaching 15 mag. (V) about 350 days later. After a short plateau and the eclipse at around HJD 2452100, ASAS J174600-2321.3 continued to brighten in V during the rest of EROS-2 and the beginning of ASAS-3 coverage, rising by about three magnitudes in ~500 days. The star reached ~12.2 mag. (V) at about HJD 2452600, around which it has apparently remained up to the present time. Interestingly, the conspicuous brightening is not seen at longer wavelengths; the mean brightness of the corresponding EROS-2 I C measurements increased by only 0.2 mag., although—as mentioned above—there exists no I C photometry for the most dramatic part of the brightening between about HJD 2452200 and HJD 2452680 because of the missing R E measurements after HJD 2452200. In order to derive an approximate amplitude in I C , we have transformed APASS photometry at maximum using Equation (3) of Jester et al. (2005; especially their Table 1):R – I = 1.00(r – i) + 0.21 (3)From this, we derive I C = 10.6 mag. at maximum, which indicates a total amplitude of ~2 mag. in this band—less than half of the amplitude in V. 2.2. The observed outburst and a historical light curve As becomes obvious from Figure 1, the system shows complex photometric variability on different timescales. The most striking feature of the light curve is the already mentioned drastic increase in visual brightness related to the primary component. This outburst has been accompanied by a blueward color evolution. Before the rise in brightness (HJD < 2451112), we derive a mean extinction corrected color index of (V–I C ) ≈ 3.0 mag., which is consistent with a spectral type of ~mid-M (Ducati et al. C measurements at HJD 2452200.542—after the system had already brightened by ~1.5 mag. (V)—the color index became bluer, to (V–I C ) ≈ 1.8 mag. Finally, at maximum visual light, Figure 1. Light curve of ASAS J174600-2321.3, based on EROS-2, ASAS-3, and APASS data. EROS-2 B E and R E magnitudes have been transformed to Johnson V and Cousins I, respectively; Cousins I values have been derived from APASS photometry using the equations in Jester et al. (2005); see text for details. Also included is a transformed observation from CMC14 (Evans et al. been removed from the ASAS-3 dataset. The epochs of the spectra are indicated by arrows; magnitudes were not corrected for extinction (see text for details). ümmerich, et al. , JAAVSO Volume 43, 2015 3 the derived color index, (B–V) ≈ 0.2 mag., is in agreement with a late A- / early F-type supergiant (see sections 3.2 and 3.3). In order to investigate the long-term photometric variability of ASAS J174600-2321.3, we have constructed a light curve including historical data from various catalogue sources, which is shown in Figure 2. Archival plate measurements and other observations over the years indicate that the star’s magnitude has been found between magnitudes 17 and 18 on several occasions on blue-sensitive photographic plates (Table 3), which is about 4 to 5 magnitudes fainter than the observed maximum B magnitude of 13.2 from APASS—a value well beyond any possible error in plate reductions. No bright states seem to have been recorded in the past. However, as there are only a few scattered measurements in different passbands before the onset of the EROS project, the evidence is tentative, at best.2.3. Spectroscopic observations During a search for new RCB stars in the EROS-2 database, Tisserand et al. (2008) identified ASAS J174600-2321.3 as a likely candidate on grounds of its RCB-like photometric variability (fast brightness declines; slow, RCB-like recovery at the beginning of ASAS-3 coverage, intrinsic pulsations). A spectrum of the object was obtained using the Dual-Beam Table 2. Photometric measurements of ASAS J174600-2321.3 from APASS. I C values have been derived from APASS photometry using the equations in Jester et al. (2005). Passband HJD–2400000 Magnitude Error
APASS B 56008.7946 13.208 0.006 56040.7133 13.189 0.006 56085.5371 13.347 0.010 56086.5358 13.476 0.007 56105.6268 15.992 0.060 APASS V 56008.7942 12.179 0.005 56040.7128 12.176 0.005 56085.5366 12.275 0.007 56086.5353 12.398 0.006 56105.6263 14.753 0.042 APASS i' 56008.7968 11.098 0.006 56040.7154 11.274 0.008 56085.5544 11.342 0.018 56086.5379 11.368 0.015 56101.8428 12.445 0.026 56102.8404 12.562 0.026 56103.8376 12.609 0.028 56105.6939 12.502 0.029 APASS g' 56040.7159 12.681 0.004 56085.5422 12.817 0.006 56086.5410 12.878 0.004 56105.6293 15.373 0.035 56134.6033 16.700 0.109 APASS r' 56040.7141 11.778 0.005 56085.5379 11.861 0.006 56086.5366 12.020 0.006 56105.6276 14.123 0.037 56134.6016 14.689 0.060 APASS I C Value Source Epoch Remarks
Spectrograph (DBS; Rodgers et al. et al. (2013). This renewed the interest in the object and, accordingly, it was re-investigated and a spectrum with broad wavelength coverage was obtained. Spectroscopic observations were performed with the Wide Field Spectrograph (WiFeS) instrument (Dopita et al. ümmerich, et al. , JAAVSO Volume 43, 20154 along each of the twenty-five 38" × 1" slitlets. The visible wavelength interval is divided by a dichroic at around 600 nm feeding two essentially similar spectrographs. The spectrum, which comprises a 2-pixel resolution of 2 Å, was taken at maximum visual brightness on HJD ~2455762.9661 (the “2012 spectrum”); a segment is shown in Figure 10 (5700 Å < λ < 9700 Å), the entire spectrum is given in Figure 11. The epochs of both spectra are indicated in Figure 1.
3. Data analysis and interpretation
We interpret the light curve characteristics (brightening, eclipses, pulsations), the spectral energy distribution, and the spectra as being due to the fact that ASAS J174600-2321.3 is made up of two components. In the following sections, the observed phenomena are discussed in that context.3.1. Orbital period and eclipse characteristics Three conspicuous fading episodes were covered to varying degrees by ASAS-3; a fourth one is evident from recent APASS data (Figure 1). From their rapid declines, symmetric recoveries, and strict periodicity, we conclude that these events represent deep eclipses with a period of P orb = 1,011.5 days and an eclipse duration of 111 days, which corresponds to ~11% of the period. No trace of a secondary eclipse could be found. A phase plot illustrating the deep eclipses is shown in Figure 3. The following elements have been derived:HJD (Min I) = 2456142 + 1011.5 × E (4) We have searched for additional eclipses of low amplitude in EROS-2 data (i.e., before the most dramatic part of the brightening). There is another eclipse at around HJD 2452100 (“the 2001 eclipse”) which exhibits evidence of a pronounced time of totality, during which the primary star is completely hidden by the eclipsing body. It is interesting to note that the pulsational variability—which will be discussed in section 3.4—continues during the observed time of totality (Figure 4). No other clearly defined eclipses could be found. However, there is a curious, “V-shaped” fading near the expected time of eclipse at around HJD 2451050 (“the 1998 fading”; Figure 5). This is likely not an actual eclipse (it occurs 76.5 ± 25 days before the computed time of minimum as determined by
Figure 3. Phase plot of ASAS J174600-2321.3, based on ASAS-3, APASS V, and transformed CMC14 data, and folded with the ephemeris given in Equation (4). Only data > HJD 2452700 have been considered for the phase plot. Figure 4. Close-up view of the 2001 eclipse. In order to preserve a maximum number of datapoints, the plot has been based on EROS-2 instrumental B E magnitudes. Note the continuance of pulsations during the time of totality.Figure 5. Close-up view of the 1998 fading. In order to preserve a maximum number of datapoints, the plot has been based on EROS-2 instrumental B E magnitudes.Figure 6. Phase plot of ASAS J174600-2321.3, illustrating all primary eclipses; also included is the 1998 fading episode. The plot has been based on EROS-2, ASAS-3, and APASS V data and folded with the elements given in Equation (4). EROS-2 B E magnitudes have been transformed to Johnson V (see text for details). In order to facilitate comparison, the resulting EROS-2 V magnitudes have been shifted by the indicated amounts to match V magnitudes from ASAS-3 and APASS. ümmerich, et al. , JAAVSO Volume 43, 2015 5 which is equivalent to 36.414 days before mid-eclipse, indicate a B–V index of 1.24 mag. (approximating to (B–V) ≈ 0.5 mag.) and a decrease of 2.6 mag. in V and 1.15 mag. in the Sloan i' band relative to the maximum magnitude. Additional observations at phase φ ≈ 0.993 (7.081 days before mid-eclipse) show the star below the detection limit in the B and V bands while the observed decrease in brightness relative to the measurements at phase φ ≈ 0.964 are only 1.3 mag. and 0.57 mag. in the g' and r' bands, respectively, which confirms the shrinking of the amplitude towards the red end of the spectrum. This is illustrated in Figure 7, which shows a detailed view of the primary eclipse based on BVg'r'i' photometry from APASS and V data from ASAS-3. These findings are also confirmed by EROS-2 data; the amplitude of the 2001 eclipse is 0.2 mag. (I C ) and 0.9 mag. (V), respectively. Figure 7. Close-up view of the primary eclipse. The plot is based on ASAS-3 V and APASS multi-color photometry, as indicated in the legend on the right side. The data have been folded with the ephemeris given in Equation (4). Note the decreasing amplitude of the eclipse towards longer wavelengths.Table 4. Recent photometric measurements of ASAS J174600-2321.3. Catalogue data have been accessed through VizieR and corrected for interstellar extinction using the estimates of Schlafly and Finkbeiner (2011), which have been accessed through the NASA/IPAC Infrared Science Archive (http://irsa.ipac.caltech.edu/applications/DUST/). The listed error margins are taken directly from the corresponding catalogues.
Passband Source Magnitude (Error)
B APASS (max. vis. light) 9.99 (±0.02)
B APASS (φ orb ~ 0.964) 12.78 (±0.02)
V APASS (max. vis. light) 9.75 (±0.00)
V APASS (φ orb ~ 0.964) 12.33 (±0.00) g' APASS (max. vis. light) 9.69 (±0.01) g' APASS (φ orb ~ 0.964) 12.39 (±0.01) r' APASS (max. vis. light) 9.71 (±0.01) r' APASS (φ orb ~ 0.964) 12.06 (±0.01) i' APASS (max. vis. light) 9.65 (±0.13) i' APASS (φ orb ~ 0.964) 11.07 (±0.13)
J 2MASS 9.27 (± 0.022) H 2MASS 8.35 (± 0.044) K s Color Index Remark (V–I C ) ≈ 3.0 mean value at minimum visual light (HJD < 2451112.53) (B–V) ≈ 0.2 epoch: HJD 2456008.7942 (maximum visual light) (B–V) ≈ 0.5 at φ orb ≈ 0.964 (J–K s ) ≈ 1.2 epoch: HJD 2450963.8408 (φ orb ≈ 0.88) (shortly before the rise in mean mag.) Equation (4), the uncertainty arising mostly from the pulsations) but might be due to the beating of multiple pulsation modes; however, similar phenomena have been reported in the literature for symbiotic binaries (Skopal 2008, for example). Thus, we feel justified in calling attention to this phenomenon, which will be further discussed in section 4. A phase plot of all eclipses which also includes the 1998 fading is shown in Figure 6. From the considerable increase in eclipse amplitude after the system’s rise in mean magnitude, it becomes obvious that the observed brightening is restricted to the primary star of the system. The contribution of the secondary star, whose light dominates at longer wavelengths, remains practically constant, as can be inferred from the EROS-2 I C measurements (Figure 1). Obviously, the contribution of the secondary star to the total flux of the system at visual wavelengths is negligible after the considerable brightening. This is further substantiated by the absence of a secondary minimum and an analysis of recent APASS multi-color photometry, which indicates that the system, as expected, gets redder during eclipses, and the amplitude of the eclipses decreases towards longer wavelengths. The (B–V) index at maximum light is around 1.0 magnitude, which—after correcting for line-of-sight extinction (section 2.1)—corresponds to (B–V) ≈ 0.2 mag., getting progressively redder as eclipse sets in. Although there are no observations at mid-eclipse, APASS measurements at a phase of φ ≈ 0.964, 3.2. Spectral energy distribution Recent photometric measurements from various online catalogue sources are presented in Table 4. Because of the significant line-of-sight dust extinction to ASAS J174600-2321.3 (A V ≈ 2.4 mag. and E(B–V) ≈ 0.78 mag.; Schlafly and Finkbeiner (2011); section 2.1), extinction-corrected values are given for the wavelength range 0.43 μm (Johnson B) < λ < 7.68 μm (GLIMPSE [8.0]). The spectral energy distribution (SED) of ASAS J174600-2321.3, based on the extinction-corrected values, is shown in Figure 8. APASS data in all five passbands were available from two epochs; APASS data taken at maximum visual light are denoted by triangles, APASS data taken near mid-eclipse at an orbital phase of φ ≈ 0.964 (italicized in Table 4), which corresponds to 36.414 days before mid-eclipse, are denoted by squares. According to our expectations, the hot component, which—anticipating our results —is likely a white dwarf (WD), dominates the system’s emission at maximum visual light, contributing strongly to the short wavelength region and being thus responsible for the observed rise in visual brightness. The red giant, on the other hand, dominates at longer wavelengths, peaking in flux at about 1.65 μm. Near mid-eclipse (orbital phase ümmerich, et al. , JAAVSO Volume 43, 20156 φ ≈ 0.964), however, the continuum bluewards of λ ~ 1 μm drops off dramatically as the WD is eclipsed by the red giant star, which dominates the system’s optical brightness during this part of the orbital cycle. This confirms the simultaneous presence of two different temperature regimes in ASAS J174600-2321.3, which is typical for symbiotic stars (Allen 1984, for example).3.3. Spectroscopic characteristics and the types of the primary and secondary stars The most striking features of the 2007 spectrum (shown in Figure 9) are the sodium (Na I) doublet lines at 5889 Å and 5895 Å, and H-alpha (Hα) absorption at 6563 Å. There is also structure due to titanium oxide (TiO) around 6300 Å, 7200 Å, as well as vanadium oxide (VO) absorption at around 7450 Å. The spectrum in this wavelength region resembles that of an M-type giant; consequently, ASAS J174600-2321.3 was classified as spectral type M0 and rejected as an RCB candidate by Tisserand et al. (2008). The increased wavelength coverage (3400 Å < λ < 9600 Å) of the 2012 spectrum (shown in Figures 10 and 11), which includes the Balmer and Paschen lines of hydrogen, shed new light on the star. Based on the 2012 spectrum, which is in agreement with the general characteristics of the 2007 spectrum, the star was re-classified as a highly reddened supergiant of spectral type F0 (Tisserand et al. ≈ 0.2 mag. (section 2.2). It is interesting to note that, in contrast to the 2007 spectrum, the 2012 spectrum displays Hα in emission. Additionally, as in the 2007 spectrum, there is clearly structure due to TiO absorption around 6300 Å, 7200 Å, 7800 Å, and 8300 Å; VO features are present around 7450 Å and, possibly, 7900 Å (Figure 10). The spectrum is obviously composite, the observed TiO and VO absorption being due to the presence of the cool giant, which agrees well with the observed binarity of the system. Judging from the presence of VO bands, which set in at around M7 and increase in strength with declining temperature (Gray and Corbally 2009, for example), the observed (V–I C ) index at minimum light (section 2.2), Figure 8. Spectral energy distribution (SED) of ASAS J174600-2321.3 from optical (Johnson B) to mid-infrared (WISE [22]). APASS data taken at maximum visual light are denoted by triangles, APASS data taken near mid-eclipse at an orbital phase of φ ≈ 0.964 are denoted by squares. Figure 9. The 2007 spectrum of ASAS J174600-2321.3 (Tisserand et al. et al. (2013; ©2013 The Authors. By permission of Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved. For permissions, please email: [email protected]).Figure 10. Segment of the 2012 spectrum of ASAS J174600-2321.3 (5700 Å < λ < 8700 Å; Tisserand et al. et al. (2013; ©2013 The Authors. By permission of Oxford University Press on behalf of the Royal Astronomical Society. All rights reserved. For permissions, please email: [email protected].). Note the CCD fringing that affects the reddest part of the spectrum. The Paschen lines, however, emerge well above the fringing level for a confident identification. Figure 11. The 2012 spectrum of ASAS J174600-2321.3 to about 8200 Å. The spectrum was taken by Tisserand et al. (2013) outside of an eclipse on HJD ~2455762.9661 and encompasses a wavelength range of 3400 Å < λ < 9600 Å. ümmerich, et al. , JAAVSO Volume 43, 2015 7 and the SED (section 3.2), we conclude that the secondary component of ASAS J174600-2321.3 is a late-M giant (~M7), which perfectly fits all observed parameters.3.4. Pulsation study In addition to the mean brightness changes, ASAS J174600-2321.3 also shows semiregular pulsations, which are most obvious in EROS-2 I C data, for example in and around the 2001 eclipse at around HJD 2452100 (Figure 12). It is obvious that the pulsations continue during the total phase of the observed eclipse, which is proof that the pulsations arise in the late M-type secondary component, as would be expected. Although rather ill-defined throughout most of the covered timespan, there is possible pulsational activity with a timescale around 50 to 60 days in EROS-2 data. After the significant rise in mean brightness related to the primary star, the oscillations are much less clear but still readily visible during maximum light in the ASAS-3 V light curve. However, a period of about 80 to 90 days is now prevalent, especially around HJD 2453500 (Figure 13). While there is no doubt that the pulsations arose in the secondary star before the observed brightening, it is open to debate where they stem from after this event. As the expected contribution of the secondary star at visual wavelengths will now be negligible, the observed pulsations after the brightening are likely to arise in the F-type primary star, which might explain the apparent change in period; however, more data are needed to resolve this matter. As will be shown in the discussions in section 4, the primary star is likely a WD currently in outburst. In this respect, it is interesting to mention that—according to theoretical considerations—the outer portion of the white dwarf envelope might become pulsationally unstable during the first few months after visual maximum has been reached in a symbiotic nova eruption (Kenyon and Truran 1983). Pulsations of comparable period and amplitude have, for example, been observed during the maximum of the symbiotic nova PU Vul (P ≈ 80 d; ΔV ≈ 0.15 mag.; see Kenyon 1986 and references therein). An analysis of EROS-2 I C data with different period search algorithms (CLEANest (Foster 1995) and ANOVA (Schwarzenberg-Czerny 1996), as implemented in peranso (Vanmunster 2007); period (Lenz and Breger 2005)) suggests a dominant signal at P ≈ 56 days (Figure 14). Although the amplitude of the signal is rather weak and the error margin is considerable due to the semiregular nature of the variability, we adopt this value as a starting point for the computation of distance and other stellar parameters in the following section. 3.5. Distances3.5.1. Distance in a high extinction area We have estimated the distance to ASAS J174600-2321.3 using the period-luminosity (P-L) relations for M-type semiregular variables based on Hipparcos parallaxes proposed by Yeşilyaprak and Aslan (2004). Assuming that the M giant dominates the system’s light before the outburst in V and, especially, in I C , we have derived mean magnitudes of ASAS J174600-2321.3 in both passbands from converted EROS-2 observations before the onset of the brightening at around HJD 2451240 (V = 16.3 mag.; I C = 12.2 mag.). We have used the Figure 12. Semiregular pulsations of ASAS J174600-2321.3, based on EROS-2 data (2451726 < HJD < 2452200). EROS-2 R E magnitudes have been transformed to Cousins I C (see text for details). Note the continuance of the pulsations during the 2001 eclipse at around HJD 2452100.Figure 13. Semiregular pulsations of ASAS J174600-2321.3 after the dramatic brightening, based on ASAS-3 data (2453409 < HJD < 2453673).Figure 14. period Fourier graph and period fit (upper panels), based on an analysis of EROS-2 I C data. The corresponding phase plot (lower panel, with fit curve) is folded with a period of P = 56 days. EROS-2 R E magnitudes have been transformed to Cousins I (see section 2.1 for details). Note the changes in mean magnitude which are evident from the period fit and phase plot. ümmerich, et al. , JAAVSO Volume 43, 20158 corresponding P-L relations for the Johnson V and Cousins I bands (Yeşilyaprak and Aslan 2004; especially their Table 2), adopting a period value of P = 56 days (section 3.4):M V = 2.89 (±0.49) × log(P) – 5.30 (±0.85) (5)M Ic = 0.83 (±0.48) × log(P) – 4.79 (±0.85) (6) From this, we derive absolute magnitudes of M V ≈ –0.25 mag. and M Ic ≈ –3.35 mag. for the red giant component of ASAS J174600-2321.3. Taking into account the line-of-sight extinction A V ≈ 2.4 mag. and A I ≈ 1.4 mag., calculated using the estimates of Schlafly and Finkbeiner (2011), we derive distances of ~6.7 kpc and ~6.8 kpc from Equations (5) and (6), respectively. Similar results are obtained using the Hipparcos K-band P-L diagram for semiregular variables from Bedding and Zijlstra (1998), which further substantiates our estimates. Considering the sources of error (intrinsic uncertainties of the P-L relations, conversion of EROS data to standard passbands, semiregularity of the period), it becomes obvious that our distance estimate is only a first approximation that further studies may build upon in the future. However, we feel justified in concluding that ASAS J174600-2321.3 (Galactic coordinates l, b = 2.829°, 4.814°) is situated in the Galactic Bulge, at a distance of about 2 kpc from the Galactic Center.3.5.2. M giant radius, mass estimates, and orbital distance We have assessed the effective temperature of the red giant from the proposed spectral class of ~M7 (section 3.3) and derive T eff ≈ 3,150 K. From period and amplitude of the observed pulsations, we have assessed the luminosity of the giant at log (L / L ) ≈ 3.64 using Figure 6.2 of Fraser (2008). By comparing these results to the evolutionary tracks for AGB stars of about solar metallicity (Marigo et al. et al. g ≈ 1.5 M for the red giant star (Figure 15), which is in good agreement with the mass estimates for symbiotic binaries compiled from the literature by Mikołajewska (2003, 2010). Based on the aformentioned sources, we furthermore adopt a mass of M wd ≈ 0.5 M for the white dwarf. Assuming that the red giant star pulsates in the first overtone, as is observed and proposed for many semiregular variables of similar period (for example, Percy and Parkes 1998; Soszyński et al. ) − 0.51 log(M / M ) − 1.60 (7)Using P = 56 days and M g = 1.5 M , we derive a radius of R g ≈ 145 R , which is in accordance with the values gleaned from the “Catalogue of Apparent Diameters and Absolute Radii of Stars” (Pasinetti Fracassini et al. Figure 15. Stellar evolutionary tracks for AGB stars of about solar metallicity and different masses, adapted from Marigo et al. (2008) and Girardi et al. (2010) and accessed through http://stev.oapd.inaf.it/cgi-bin/cmd. The position of the red giant component of ASAS J174600-2321.3 is marked by the diamond.
WD to be R ≈ 2.5 AU. This results in an essentially consistent picture that is in general accordance with the data compiled by Mikołajewska (2003) for other systems. Furthermore, the adopted configuration is able to reproduce the observed eclipse duration of about 111 days (section 3.1). We used a simplified model, therefore the given values have to be treated with caution and serve only as a first approximation. For example, it is possible that the radius of the red giant star has been underestimated because of the unknown exact orbital inclination of the system. Only detailed studies will be able to shed more light on the system’s parameters.
4. Discussion ümmerich, et al. , JAAVSO Volume 43, 2015 9
Symbiotic stars (GCVS-type ZAND; Samus et al. et al. et al. II region, whose nebular radiation—according to Skopal (2008)—is the source of the orbitally related variations. Other phenomena, like ellipsoidal variations, might be involved (Gromadzki et al. II region has an asymmetrical shape due to orbital motion and interaction with the stellar winds. The nebular emission varies as a function of orbital phase, producing broad, flat minima during quiescence, which occur prior to the time of spectroscopic conjunction at an orbital phase of φ ≈ 0.9 (for a more detailed discussion, see Skopal 1998 and Skopal 2008). This leads to systematic changes in the O–C residuals of the minima times in eclipsing symbiotic binaries (for example, Skopal 2008, especially section 6). As has been described in section 3.1, the “V-shaped” 1998 fading occurred at an orbital phase of φ ≈ 0.9. It is comparable in amplitude and shape to what has been described for other symbiotic binaries (Skopal 2008). It is thus intriguing to interpret the 1998 fading in this vein; however, as has been pointed out above, it may simply be the result of the interference of different pulsation modes. Only long-term light curve studies will be able to shed more light on this issue. (c) With the onset of activity in the system, the optical region usually becomes dominated by the radiation from the pseudophotosphere of the compact object and a narrow, “Algol-like” eclipse is observed at the inferior conjunction of the giant (Skopal 2008). This is exactly what has been observed in the present object after the onset of activity that led to the dramatic brightening of the primary component. (d) Several types of brightenings are observed in symbiotic binaries (for example, Leibowitz and Formiggini 2006; Skopal et al. Figure 16. Light curve of ASAS J174600-2321.3, based on EROS-2, ASAS-3 and APASS V data. Symbols and data sources are the same as in Figure 1. The epochs of the spectra are indicated by arrows (see section 3.3 for details). Several light curve features, discussed in the text, are marked by lowercase letters. ümmerich, et al. , JAAVSO Volume 43, 201510 objects, which we adhere to throughout this paper; the latter group is of no interest in the analysis of the present object. Symbiotic novae eruptions develop very slowly; the systems may remain at maximum light for decades, after which they fade very slowly. Apart from that, symbiotic novae share common properties with classical symbiotic stars: they are always long-period (P orb ≥ 800 days; Mikołajewska 2010), interacting binary stars comprising an M giant. In fact, there exists no clear cut boundary between classical symbiotic stars and symbiotic novae (Skopal et al. et al.
5. Conclusion
By an analysis of all available data from the literature, public sky surveys, and photometric catalogues, we have identified the star ASAS J174600-2321.3 as a long-period eclipsing binary with an orbital period of P orb = 1,011.5 days. The primary star, which is likely a white dwarf in outburst, exhibits spectral characteristics of a reddened, early F-type supergiant at visual maximum light; the secondary star is a giant of spectral type late M (~M7). The system underwent a significant increase in brightness (~4 mag (V)) during the recent past, which is related to the primary component. We have discussed the origin of the observed brightening and favor the scenario of an eclipsing, symbiotic binary, which is capable of explaining the observed, complex light curve features. Because of the peculiarities of the observed outburst (large amplitude, duration, slow development) and spectral characteristics, we propose ASAS J174600-2321.3 as a symbiotic nova of type NC. Magnitude range, periods, stellar parameters, and binary separation of ASAS J174600-2321.3, as derived in the present paper, are presented in Table 5. The outburst has already lasted for more than ~4,100 days and seems to continue to the present day. We have started a long-term photometric monitoring of the system, the results of which will be presented in an upcoming paper.
6. Acknowledgements
This research has made use of the SIMBAD and VizieR databases operated at the Centre de Données Astronomiques (Strasbourg) in France. This work has also made use of EROS-2 data, which were kindly provided by the EROS collaboration. The EROS (Expérience pour la Recherche d’Objets Sombres) project was funded by the CEA and the IN2P3 and INSU CNRS institutes. Furthermore, this research has employed data products from the Two Micron All Sky Survey, which is a joint project of the University of Massachusetts and the Infrared Processing and Analysis Center/California Institute of Technology, funded by the National Aeronautics and Space Administration and the National Science Foundation, and the
Figure 17. Historical light curve of RR Tel, adapted from Mayall (1949; data prior to 1948 are photographic from Harvard College Observatory plates; 1948 data are visual observations from the AAVSO). ümmerich, et al. , JAAVSO Volume 43, 2015 11
Wide-field Infrared Survey Explorer, which is a joint project of the University of California, Los Angeles, and the Jet Propulsion Laboratory/California Institute of Technology, funded by the National Aeronautics and Space Administration. This research has also made use of the NASA/IPAC Infrared Science Archive, which is operated by the Jet Propulsion Laboratory/California Institute of Technology, under contract with the National Aeronautics and Space Administration. The authors would like to thank Franz-Josef (Josch) Hambsch, Belgium, for acquiring photometric observations of our target, and the anonymous referee for helpful comments and suggestions that helped to improve the paper.
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Table 5. Magnitude range, periods, stellar parameters, and binary separation of ASAS J174600-2321.3, as derived in the present paper.
Parameter Value
Magnitude Range (V) 11.9–16.9 mag. Orbital Period 1,011.5 days Stellar Parameters (Red Giant) M g ≈ 1.5 M R g ≈ 145 R T eff ≈ 3,130 K Spectral type ~M7 (White Dwarf) M wd ≈ 0.5 M