brite and ground-based photometry and spectroscopy of ...modes. it is also a run-away star (toala et...

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BRITE and Ground-based Photometry and Spectroscopy of the β Cephei Star Persei El˙ zbieta Zoclo´ nska 1 and the BRITE Team 1. Nicolaus Copernicus Astronomical Center Bartycka 18, 00–716 Warszawa, Poland [email protected] Persei was observed for a second time by the BRITE satellites from 9th Septem- ber 2016 to 6th March 2017. We organized a ground-based spectroscopic cam- paign in order to determine the modes of pulsation and properties of the star simultaneously with the space photometry. The goal of our study is to find pulsation frequencies and amplitudes, to identify pulsation modes, to verify the orbital period and to find properties of Persei, i.e. core and envelope rotation, angular speed and exact evolution phase. First results are presented. 1 Persei (HD24760) Persei (HD24760) is a triple star system. The main component Persei A is a β Cephei type star. Its spectral type is B1.5III (Abt & Cardona, 1983). The second component Persei B is a star of spectral type A6 or B9 IV(Abt & Cardona, 1983). The spectral type of the third component Persei C is not well established. The orbital period of the second component is equal to 14.069 days, the orbital period of the third component is around 25.8 years (Libich et al., 2005). Persei A (hereafter referred to as Persei) is a fast rotating star (projected rotational velocity v sin i between 130–153 km/s, Abt et al., 2002; De Cat et al., 2000) with multiple pulsation modes. It is also a run-away star (Toal´ a et al., 2017). Its variability has been the subject of several studies. The most recent work devoted to close binary orbital period determination was done by Libich et al. (2005). In that paper all references, information and a summary concerning former spectroscopic research of the star by Gies & Kullavanijaya (1988), Tarasov et al. (1995), and by De Cat et al. (2000) can be found. Per was used to understand line profile variations in hot stars by Gies & Kullavanijaya (1988). Persei was observed for the second time by the BRITE satellites (Weiss et al., 2014; Pablo et al., 2016) from 9th September 2016 to 6th March 2017. We organized a ground-based spectroscopic campaign in order to determine the pulsation modes and properties of the star simultaneously with the space photometry. Per A is a supernova type II progenitor. We intend to determine the core and envelope rotation (long-period gravity modes excited in the star carry information about the stellar core, acoustic oscillation modes about the stellar envelope), angular speed and exact evolution phase. 94 ? PTA Proceedings ? August, 2018 ? vol. 8 pta.edu.pl/proc/v8p94

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Page 1: BRITE and Ground-based Photometry and Spectroscopy of ...modes. It is also a run-away star (Toala et al., 2017). Its variability has been the subject of several studies. The most recent

BRITE and Ground-based Photometryand Spectroscopy of the β Cephei Star εPersei

Elzbieta Zoc lonska1 and the BRITE Team

1. Nicolaus Copernicus Astronomical CenterBartycka 18, 00–716 Warszawa, [email protected]

ε Persei was observed for a second time by the BRITE satellites from 9th Septem-ber 2016 to 6th March 2017. We organized a ground-based spectroscopic cam-paign in order to determine the modes of pulsation and properties of the starsimultaneously with the space photometry. The goal of our study is to findpulsation frequencies and amplitudes, to identify pulsation modes, to verify theorbital period and to find properties of ε Persei, i.e. core and envelope rotation,angular speed and exact evolution phase. First results are presented.

1 ε Persei (HD24760)

ε Persei (HD24760) is a triple star system. The main component ε Persei A is aβ Cephei type star. Its spectral type is B1.5III (Abt & Cardona, 1983). The secondcomponent ε Persei B is a star of spectral type A6 or B9 IV(Abt & Cardona, 1983).The spectral type of the third component ε Persei C is not well established. Theorbital period of the second component is equal to 14.069 days, the orbital period ofthe third component is around 25.8 years (Libich et al., 2005). ε Persei A (hereafterreferred to as ε Persei) is a fast rotating star (projected rotational velocity v sin ibetween 130–153 km/s, Abt et al., 2002; De Cat et al., 2000) with multiple pulsationmodes. It is also a run-away star (Toala et al., 2017). Its variability has been thesubject of several studies. The most recent work devoted to close binary orbitalperiod determination was done by Libich et al. (2005). In that paper all references,information and a summary concerning former spectroscopic research of the star byGies & Kullavanijaya (1988), Tarasov et al. (1995), and by De Cat et al. (2000) canbe found. ε Per was used to understand line profile variations in hot stars by Gies& Kullavanijaya (1988).

ε Persei was observed for the second time by the BRITE satellites (Weiss et al.,2014; Pablo et al., 2016) from 9th September 2016 to 6th March 2017. We organizeda ground-based spectroscopic campaign in order to determine the pulsation modesand properties of the star simultaneously with the space photometry.

ε Per A is a supernova type II progenitor. We intend to determine the core andenvelope rotation (long-period gravity modes excited in the star carry informationabout the stellar core, acoustic oscillation modes about the stellar envelope), angularspeed and exact evolution phase.

94 ? PTA Proceedings ?August, 2018 ? vol. 8 pta.edu.pl/proc/v8p94

Page 2: BRITE and Ground-based Photometry and Spectroscopy of ...modes. It is also a run-away star (Toala et al., 2017). Its variability has been the subject of several studies. The most recent

BRITE and Ground-based Photometry and Spectroscopy of ε Per

2 Spectroscopic observations

In 2016 ε Persei was re-observed by both professional and amateur astronomers usingground-based spectrographs as well as in 2014. In 2016, we obtained additional datafrom McDonald Observatory. The full list of spectroscopic observations is as follows:

• GATS - Krzysztof Kaminski, Wojciech Dimitrov, Monika Kaminska, Mag-dalena Polinska (Polinska et al., 2014)

• AAVSO:

– Austria, Germany - Berthold Stober, Manfred Schwarz, Siegfried Hold,Ulrich Waldschlager

– China - Dong Li– France (La Tourbiere) - Olivier Garde– USA (Baltimore)

• Lithuania (Moletai) - Erika Pakstiene, Sarunas Mikolaitis• Slovakia (Stara Lesna Observatory) - Ernst Paunzen• USA (McDonald Observatory) - Elzbieta Zoc lonska

2.1 Spectroscopic observations at McDonald Observatory

McDonald Observatory is located in Texas in the USA. The 2.1-m Otto StruveTelescope was used for 12 nights of observations from 12 Nov 2016 to 23 Nov 2016(UTC) but only 10 were usable for science observations. The Sandiford Cassegrain

Echelle Spectrometer was used to gather spectra in the range of 4341–4861A with aresolution of R=60,000. All spectra were reduced and normalized with IRAF1. TheSi III λ4553 line A was studied so far. An example spectrum is shown in Fig. 1.

4550 4560 4570 4580 4590Wavelength [Å]

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Fig. 1: Spectrum of HD24760 from McDonald Observatory taken on 2457706.86357745 JD,exposure time = 48 s. The three spectral lines are due to doubly ionized silicon (Si III atλ4553, 4568, 4574 A).

We obtained 1210 high quality spectra of HD24760 during 10 consecutive nightsstarting on 14 Nov 2016. This high resolution time series spectroscopy is being usedfor mode identification. The variation of the flux profile of Si III spectral lines will beused to identify the modes. Line profile variations measured during the night of 16

1IRAF is distributed by the National Optical Astronomy Observatory, which is operated by theAssociation of Universities for Research in Astronomy (AURA) under cooperative agreement withthe National Science Foundation

pta.edu.pl/proc/v8p94 PTA Proceedings ?August, 2018 ? vol. 8 ? 95

Page 3: BRITE and Ground-based Photometry and Spectroscopy of ...modes. It is also a run-away star (Toala et al., 2017). Its variability has been the subject of several studies. The most recent

Elzbieta Zoc lonska, the BRITE Team

November 2016 are shown in Fig. 2. Consecutive spectra are shifted in the verticaldirection according to time. We can see that the line profile shape and depth changewith time due to stellar oscillations.

4546 4548 4550 4552 4554 4556 4558 4560Wavelength [Å]

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Fig. 2: Variation of the Si III 4553 A line profile in the spectrum of HD 24760 onHJD 2 457 708/709

Using FAMIAS (Zima, 2008) we converted the wavelength scale to Doppler ve-locity and calculated radial velocities. Fig. 3 shows an example. One can again seethat the effect of the pulsations is visible in the line profile.

Fig. 3: Line profile of HD24760 in heliocentric velocity space

To find periodicities we performed a time series analysis of the line profile vari-ations. The radial velocity curve from all 10 nights of data is shown in Fig. 4. Theradial velocity curve from our data phased with the orbital period equal to 14.069days found by Libich et al. (2005) is presented in Fig. 5. The FAMIAS software will

96 ? PTA Proceedings ?August, 2018 ? vol. 8 pta.edu.pl/proc/v8p94

Page 4: BRITE and Ground-based Photometry and Spectroscopy of ...modes. It is also a run-away star (Toala et al., 2017). Its variability has been the subject of several studies. The most recent

BRITE and Ground-based Photometry and Spectroscopy of ε Per

2457708 2457710 2457712 2457714 2457716

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Fig. 4: Radial velocity curve of ε Per Fig. 5: Radial velocity of ε Per phased with theorbital period of 14.069 days

be used to identify the pulsation modes as well.

3 Photometric observations by BRITE

In 2014, during 168 days, four BRITE Constellation satellites observed ε Persei froma low earth orbit: BRITE-Austria, UniBRITE, BRITE Lem and BRITE Toronto.In 2016, during 179 days, only BRITE Lem and BRITE Toronto were observing thefield with ε Per. Analysis of the 2016 data is still in progress. Preliminary resultsfrom BRITE-Toronto 2016 observations are shown in Fig. 6. Frequencies in boldframes are the ones found in both our photometry and spectroscopy. We used thefdecomp software (R. Smolec, priv. comm.) for finding frequencies.

Fig. 6: Preliminary frequency spectrum of HD24760

Some additional decorrelation of the BRITE data still needs to be done. We areplanning to recalculate all frequencies with a new approach and then identify thepulsation modes using FAMIAS.

Acknowledgements. We thank Radek Smolec for providing his “fdecomp software” for

frequency calculation and light curve analysis. We gratefully acknowledge the efforts of

the AAVSO observers: Berthold Stober, Manfred Schwarz, Siegfried Hold, Ulrich Wald-

schlager, Dong Li, Olivier Garde, the GATS team: Krzysztof Kaminski, Wojciech Dim-

pta.edu.pl/proc/v8p94 PTA Proceedings ?August, 2018 ? vol. 8 ? 97

Page 5: BRITE and Ground-based Photometry and Spectroscopy of ...modes. It is also a run-away star (Toala et al., 2017). Its variability has been the subject of several studies. The most recent

Elzbieta Zoc lonska, the BRITE Team

itrov, Monika Kaminska, Magdalena Polinska, the Moletai Observatory observers: Erika

Pakstiene, Sarunas Mikolaitis and Ernst Paunzen for observations at Stara Lesna Observa-

tory. We thank Barbara Castanheira, John Kuhne and Dave Doss (without them obtaining

1210 high quality HD24760 spectra would not have been possible) for supporting the obser-

vations of McDonald Observatory. The operation of the Polish BRITE satellites is funded

by a SPUB grant by the Polish Ministry of Science and Higher Education (MNiSW). The

author’s participation in this conference was supported by the Polish National Science

Center (NCN), grants no. 2011/01/M/ST9/05914 and 2015/18/A/ST9/00578. This paper

is based on data collected by the BRITE Constellation satellite mission, designed, built,

launched, operated and supported by the Austrian Research Promotion Agency (FFG),

the University of Vienna, the Technical University of Graz, the Canadian Space Agency

(CSA), the University of Toronto Institute for Aerospace Studies (UTIAS), the Foundation

for Polish Science & Technology (FNiTP MNiSW), and National Science Centre (NCN).

References

Abt, H. A., Cardona, O., ApJ 272, 182 (1983)

Abt, H. A., Levato, H., Grosso, M., ApJ 573, 359 (2002)

De Cat, P., Telting, J., Aerts, C., Mathias, P., A&A 359, 539 (2000)

Gies, D. R., Kullavanijaya, A., ApJ 326, 813 (1988)

Libich, J., et al., VizieR Online Data Catalog 344 (2005)

Pablo, H., et al., PASP 128, 12, 125001 (2016), arXiv: 1608.00282

Polinska, M., et al., in J. A. Guzik, W. J. Chaplin, G. Handler, A. Pigulski (eds.) PrecisionAsteroseismology, IAU Symposium, volume 301, 475–476 (2014)

Tarasov, A. E., et al., A&AS 110, 59 (1995)

Toala, J. A., Oskinova, L. M., Ignace, R., ApJ 838, L19 (2017), arXiv: 1703.04059

Weiss, W. W., et al., PASP 126, 573 (2014), arXiv: 1406.3778

Zima, W., User manual for FAMIAS and DAS : frequency analysis and mode identi-fication for asteroseismology and database with time series for asteroseismology, de-veloped in the framework of the FP6 European Coordination Action HELAS, Com-munications in Asteroseismology, Austrian Acad. of Sciences Press (2008), URLhttps://books.google.pl/books?id=ZBwcnwEACAAJ

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