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Observations of H??, iron, and oxygen lines in B, Be, and shell stars

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We have carried out a spectroscopic survey of several B, Be, and shell stars in optical and near-infrared regions. Line profiles of the Hα line and of selected Fe II and O I lines are presented.
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arXiv:astro-ph/0512619v1 27 Dec 2005
Astronomy & Astrophysics
manuscript no. beir9101 February 3, 2008
(DOI: will be inserted by hand later)
Observations of Hα, iron, and oxygen lines in B, Be, and shell
stars
S. M. Saad1,2, J. Kub´at1, D. Korˇakov´a1, P. Koubsk´y1, P. ˇ
Skoda1, M. ˇ
Slechta1, A. Kawka1, A. Budoviˇcov´a1,
V. Votruba3,1, L. ˇ
Sarounov´a1, M. I. Nouh2
1Astronomick´y ´ustav, Akademie vˇed ˇ
Cesk´e republiky, CZ-251 65 Ondˇrejov, Czech Republic
2National Research Institute of Astronomy and Geophysics, 11421 Helwan, Cairo, Egypt
3´
Ustav teoretick´e fyziky a astrofyziky PˇrF MU, Kotl´rsk´a 2, CZ-611 37 Brno, Czech Republic
Received 23 August 2004 / Accepted 21 December 2005
Abstract. We have carried out a spectroscopic survey of several B,Be, and shell stars in optical and near-infrared regions.
Line profiles of the Hαline and of selected Fe II and O Ilines are presented.
Key words. Stars: Be – line: profiles
1. Introduction
Observations of B, Be, and shell stars in different spectral re-
gions are important for putting constraints on modeling these
stars. Echelle spectrographs as well as the high sensitivity of
modern detectors in the red part of the spectrum provide a
wealth of the information contained in the whole visible and
near infrared regions obtained simultaneously. The aim of this
paper is a spectroscopic survey of line profiles of Hαand se-
lected non-hydrogenic lines of iron and oxygen in the visual
and near infrared region for selected bright B and Be stars. We
mainly use the echelle observations secured using the HEROS
(Heidelberg Extended Range Optical Spectrograph) spectro-
graph attached to the Ondˇrejov 2m telescope supplemented by
several CCD coud´e spectra.
2. Observations and data reduction
The present data are based on new spectroscopic observations
of 13 Bstars, 28 Be stars, and 8 shell stars. Our sample of stars
contains objects of spectral types B0 – B9.5 and luminosity
classes III, IV and V. Table 1 summarises the basic informa-
tion about the observed objects, their HD and HR no’s, their
name (if available), MK spectral type, luminosity class, and
Julian dates of the observations. Some of these stars have never
been observed before (to the best of our knowledge) in the
near-infrared region. The spectra of these stars were obtained
between January 2001 and November 2003 using the fiber-
fed echelle spectrograph HEROS (for a brief description see
ˇ
Stefl & Rivinius 2000, ˇ
Skoda & ˇ
Slechta 2002a) attached to the
Cassegrain focus of the 2m telescope at Ondˇrejov Observatory.
Send offprint requests to: J. Kub´at,
e-mail: kubat@sunstel.asu.cas.cz
All the basic data reduction processing, including bias subtrac-
tion, flat fielding, and wavelength calibration, have been done
using the HEROS pipeline written by O. Stahl and A. Kaufer
as an extension of basic MIDAS echelle context (see Stahl et
al 1995, also ˇ
Skoda & ˇ
Slechta 2002b). Additional observations
of several stars were secured using a CCD detector of a coud´e
spectrograph of the same telescope (ˇ
Slechta & ˇ
Skoda 2002)
and the data were reduced by the IRAF package.
3. Observed lines
3.1. The hydrogen Hαline
The Hαline in the stars of our sample was found to be either
in absorption or in emission, however,an intermediate case be-
tween emission and absorption was also found. Our set of stars
exhibits basically five different shapes of Hαline. We introduce
corresponding stellar subclasses for our sample, namely
i. Emission is present, but it is completely below the contin-
uum level. We will denote this subclass as AbEm (absorp-
tion with emission).
ii. The absorption part is below the level of continuum while
the emission peak is above the continuum. The ratio of
these two parts often varies at different phases for the same
star. We will denote this subclass as EmAb (emission with
absorption).
iii. The whole emission feature is completely above the con-
tinuum level. They will be denoted by Em (pure emission).
iv. We may also define the shell stars characterised by ex-
tremely sharp Hαabsorption cores as one of the Be star
phases. Since there is no intrinsic difference between Be
and shell stars, we denoted them by Sh. Besides the shape
of the Hαemission line profile, the presence of other sharp
2 S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars
Table 1. List of the B and Be stars in our sample. References to the spectral type are denoted by superscript numbers in paren-
theses, and the values of Teff are from Theodossiou & Danezis (1991).
HD HR Name Sp. Type Teff JD–24 00 000 JD–24 00 000 Shape
22780 1113 B6V(1) 12915 ±393 53217.5656 53217.5434 AbEm
23302 1142 17 Tau B6III(1) 13810 ±383 52619.9573 AbEm
36408B 1847B B7IV(4) 12940 ±1230 52721.8196 AbEm
217675 8762 o And B6III(1) 13810 ±383 51779.0595 AbEm
144 7 10 Cas B9III(1) 10700 ±385 52931.3284 53204.5171 EmAb
6811 335 φAnd B7III(1) 12940 ±1230 52566.8285 EmAb
58050 2817 OT Gem B2V(1) 22400 ±1393 52697.9049 EmAb
58715 2845 βCMi B8Vn(1) 12120 ±623 52620.0981 EmAb
164447 6720 V974 Her B8Vn(1) 12120 ±623 53215.4018 53215.4485 EmAb
171780 6984 B6V(1) 15310 ±750 53070.6629 53182.4968 EmAb
200310 8053 60 Cyg B1V(1) 25570 ±3652 52567.9192 EmAb
205021 8238 βCep B2III(5) 22160 ±1145 52113.0762 EmAb
216200 8690 V360 Lac B3III(2) 18445 ±1426 52527.0736 EmAb
4180 193 o Cas B5III(1) 15310 ±750 52694.8389 Em
5394 264 γCas B0.5IV(1) 30025 ±2160 52682.7532 Em
10516 496 φPer B1.5(V:)e-sh(2) 25570 ±3652 52465.0435 Em
18552 894 B7IVe(2) 12120 ±623 51954.7961 Em
22192 1087 ψPer B3IIIe-sh(2) 15310 ±750 53216.5315 53216.4905 Em
23630 1165 ηTau B7IIIe(2) 12940 ±1230 52648.8068 Em
29866 1500 B7IV(1) 12120 ±623 52526.1050 Em
109387 4787 κDra B5IIIe(2) 15310 ±750 52720.9752 Em
175863 BD+59 1929 B4Ve (3) 17100 ±386 53182.4428 53182.4642 Em
193911 7789 25 Vul B6IVe(2) 14340 ±570 52525.9284 Em
200120 8047 59 Cyg B1Ve(2) 25340 ±2164 51795.9049 Em
203467 8171 6 Cep B2.5Ve(2) 18445 ±1426 52721.0674 Em
206773 BD+572374 B0V:pe(5) 29230 ±208 52484.0447 Em
217891 8773 βPsc B5Ve(2) 15310 ±750 53216.5717 53216.5525 Em
EE Cep B5:neβ(13) 53217.5020 53217.4567 Em
23862 1180 28 Tau B8(V:)e-sh(2) 12120 ±623 51797.0884 Sh
37202 1910 ζTau B1IVe-sh(2) 25570 ±3652 51897.9234 Sh
50658 2568 ψ9Aur B6IV(2) 12300 ±945 52721.9337 Sh
142926 5938 4 Her B7IVe-sh(2) 12300 ±945 52488.8992 Sh
162732 6664 88 Her B7Vn(1) 12915 ±393 53217.4040 53217.4229 Sh
171406 6971 V532 Lyr B5V(1) 17100 ±386 53182.3954 53182.4168 Sh
179343 BD+023815 B9V(1) 10580 ±373 53216.4505 53216.4034 Sh
217050 8731 EW Lac B3IVe-sh(2) 18445 ±1426 53217.3848 53217.3731 Sh
358 15 αAnd B9p(11) 10700 ±385 51779.1187 Ab
886 39 γPeg B2IV(3) 22400 ±1393 51771.0511 Ab
23873 BD+23561 B9.5V(12) 10340 ±465 52651.0012 Ab
24760 1220 ǫPer B0.5V(5) 30000 52648.7495 Ab
34759 1749 ρAur B3V(7) 15310 ±750 52351.9306 Ab
36408 1847A B7III(4) 12940 ±1230 52720.8740 Ab
44743 2294 βCMa B1II/III(5) 26105 ±1779 52720.7954 Ab
87901 3982 αLeo B7Vn(6) 12120 ±623 51925.0219 Ab
120315 5191 ηUMa B3V(7) 18445 ±1426 52618.2262 Ab
138749 5778 θCrB B6Vn(1) 14340 ±570 52693.1422 Ab
155763 6396 ζDra B7III(8) 13810 ±383 52002.1433 Ab
160762 6588 ιHer B3V SB(9) 18445 ±1426 51787.9064 Ab
164852 6738 96 Her B3IV(10) 18445 ±1426 52722.1490 Ab
References:
(1) – Jaschek et al. (1980); (2) – Slettebak (1982); (3) – SIMBAD; (4) – Levato (1975); (5) – Morgan et al. (1955); (6) – Murphy
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars 3
photospheric absorption lines which will be referred to as
“shell lines” were also used for defining this subgroup.
v. The last subclass consists of normal Bstars with Hαab-
sorption lines. They are included in our analysis as a kind
of standard star. We denote them by Ab.
Our five subclasses represent a qualitative estimate of the
Hαline profile in our present observations. Table 1 lists the
stars according to these subclasses.
3.2. Non-hydrogen emission lines
There is a number of non-hydrogen emission lines in the spec-
tra of Be stars. The most striking emission features are pro-
duced by iron, helium, and oxygen. In addition to the hydrogen
lines, these non-hydrogenic lines carry supplementary informa-
tion coming from different regions of the stellar envelope de-
pending on their depth of formation.
3.2.1. Iron lines
Iron lines bring a lot of information from the circumstellar en-
velope depending on their depth of formation. They are often
present in the spectra of Be stars. An interesting fact about Fe II
lines is that they appear in the emission spectrum, however,
in the approximate theoretical spectrum, which was calculated
under the simplified assumption of a LTE static plane-parallel
atmosphere, they are completely missing. This indicates that
the excitation mechanism is connected more probably with the
atomic structure of Fe II and the corresponding NLTE pump-
ing than with some global density changes or even iron over-
abundance. However, such a conclusion is to be verified by
detailed NLTE calculations. We selected several strong lines
mostly from the quartet system for our measurements.
Although the list of available Fe II lines is quite long, only
several of them are useful for further analysis, in particular the
4233 ˚
A line from the multiplet (27), the 4584 ˚
A line from the
multiplet (38), 6148 and 6456 ˚
A lines from the multiplet (74),
and 7516 and 7712 ˚
A lines from the multiplet (73). Note that
the 6148 ˚
A line itself is a blend of two neighbouring Fe II lines.
Due to its vicinity to the Hαline the Fe II 6456 ˚
A line was
present in the Hαspectrograms that were obtained with the
CCD coud´e camera.
The near-infrared line Fe II 7712 ˚
A was severely contami-
nated by telluric lines in the band 7600 – 7700 ˚
A. However, this
line was sometimes strong enough to be measurable in 13 stars
of our sample. In ten of them the line was in emission. Other
Fe II lines, namely the 7516, 6456, and 6148 ˚
A lines are also in
emission. However, another Fe II line, which is not listed in the
multiplet tables of Moore (1972), appeared to be quite strong
in the synthetic spectra and may be possibly misidentified with
the Fe II 7516 ˚
A line. This line has a wavelength of 7513.162 ˚
A
and arises from the transition 5s e 6De
9/25p w 6Po
7/2. For
simplicity we will identify this feature with the wavelength
7516 ˚
A in the figures. In most cases the iron line Fe II 6516 ˚
A
was not detectable due to the huge number of telluric lines.
Table 2. List presented Fe II line profiles. For all stars the Hα
and O I77725˚
A lines are presented as well.
Star
4233
4584
5169
5235
5317
5363
6432
6456
7462
7516
7712
HR 1847B + + +
o And + + +
10 Cas +
φAnd + +
βCMi + + + + +
V974 Her +
o Cas + + + + + + +
γCas + + + + + + +
φPer + + + + + + +
HR 894 + + +
ψPer + + +
HR 1500 + + +
κDra + + + + + + + + +
HD 175863 + +
25 Vul + + +
59 Cyg + +
6 Cep + + + + + + + +
HD 206773 + +
βPsc + +
EE Cep + +
28 Tau + + + + + + +
ζTau + + + + + + +
4 Her + + + + + +
88 Her + +
HD 179343 +
EW Lac + + +
HD 23873 +
ρAur + + +
βCMa +
αLeo +
ηUMa +
θCrB +
ζDra + + + + + +
ιHer + + +
3.2.2. The oxygen infrared triplet O I77725˚
A
The most dominant oxygen line in the visible and near infrared
spectra of Be stars is the near IR triplet line at 7772, 7774,
7775 ˚
A emerging from the transition 3s5So3p5P. Other
transitions between quintet levels which fall into the visual re-
gion are missing in the spectra.
4. Description of the online material
Results of our observations are plotted in the online Appendix.
It contains an atlas of the individual line profiles sorted and
ordered according to the Table 1. For each star, the Hαand
OI77725˚
A lines are plotted. Iron lines are plotted for each
observation where they were available. The list of Fe II lines
presented is listed in the Table 2.
Acknowledgements. This research has made use of the NASA’s
Astrophysics Data System Abstract Service (Kurtz et al. 2000,
Eichhorn et al. 2000, Accomazzi et al. 2000, Grant et al. 2000).
Our work was supported by grants of the Grant Agency of the
4 S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars
Czech Republic 205/02/0445 and 102/02/1000. Astronomical Institute
Ondˇrejov is supported by a project Z10030501.
References
Accomazzi, A., Eichhorn, G., Kurtz, M. J., Grant, C. S., & Murray, S.
S. 2000, A&AS 143, 85
Cowley, A. Cowley, C., Jaschek, M., & Jaschek, C. 1969, AJ, 74, 375.
Eichhorn, G., Kurtz, M. J., Accomazzi, A., Grant, C. S., & Murray, S.
S. 2000, A&AS, 143, 61
Grant, C. S., Accomazzi, A., Eichhorn, G., Kurtz, M. J., & Murray, S.
S. 2000, A&AS 143, 111
Herbig, G. H. 1960, ApJ 131, 632
Jaschek, M., Hubert-Delplace, A. M., Hubert, H. & Jaschek, C. 1980,
A&AS, 42, 103
Johnson, H. L., & Morgan, W. W. 1953, ApJ, 117, 313
Kurtz, M. J., Eichhorn, G., Accomazzi, A. et al. 2000, A&AS, 143, 41
Lesh, J. R. 1968, ApJS, 17, 371
Levato, H. 1975, A&AS, 19, 91
Mendoza, V. E. E. 1956, ApJ, 123, 54
Molnar, M. R. 1972, ApJ, 175, 453
Morgan, W. W., Code, A. C., & Whitford, A. E. 1955, ApJS, 2, 41.
Morgan, W. W. & Keenan, P. C. 1973, ARA&A, 11, 29
Moore, C. E., 1972, A Multiplet Table of Astrophysical Interest,
NSRDS-NBS 40
Murphy, R. E. 1969, AJ, 74, 1082
ˇ
Skoda, P., & ˇ
Slechta, M. 2002a, Publ. Astron. Inst. Czech 90, 1
ˇ
Skoda, P., & ˇ
Slechta, M. 2002b, Publ. Astron. Inst. Czech 90, 40
ˇ
Slechta, M., & ˇ
Skoda, P. 2002, Publ. Astron. Inst. Czech 90, 9
Slettebak, A. 1982, ApJS 50, 55
Stahl, O., Kaufer, A., Wolf, B. et al. 1995, J. Astron. Data 1, 3
ˇ
Stefl, S., & Rivinius, T. 2000, in The Be Phenomenon in Early Type
Stars, IAU Coll. 175, M. A. Smith, H. F. Henrichs, & J. Fabregat
eds., ASP Conf. Ser. Vol. 214, p. 356
Theodossiou, E. & Danezis, E. 1991, Ap&SS, 183, 91
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 1
Online Material
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 2
Appendix A: Atlas of individual line profiles
Note that the panels which contain more than one profile the spectra are arbitrarly shifted by 0.2, 0.4 and 0.6 below or above the
continuum level.
A.1. AbEm subclass
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HR 1113
Hα
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HR 1113
OI 7772
Fig.A.1. Profiles of Hαand O I77725˚
A lines of HR 1113.
0.6
0.8
1
1.2
1.4
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
17 Tau
Hα
0.8
0.85
0.9
0.95
1
1.05
1.1
1.15
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
17 Tau
OI 7772
Fig.A.2. Profiles of Hαand O I77725˚
A lines of 17 Tau.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 3
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HR 1847B
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HR 1847B
FeII 5317
FeII 5235
FeII 5169
OI 7772
Fig.A.3. Profiles of Hα, Fe II 5169, 5235, 5317 ˚
A, and O I77725˚
A lines of HR 1847B.
0
0.2
0.4
0.6
0.8
1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ο And
Hα
0.6
0.8
1
1.2
1.4
1.6
1.8
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ο And
FeII 5317
FeII 5235
FeII 5169
OI 7772
Fig.A.4. Profiles of Hα, Fe II 5169, 5235, 5317 ˚
A, and O I77725˚
A lines of oAnd.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 4
A.2. EmAb subclass
0.6
0.8
1
1.2
1.4
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
10 Cas
Hα
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
10 Cas
FeII 6456
OI 7772
Fig.A.5. Profiles of Hα, Fe II 6456 ˚
A, and O I77725˚
A lines of 10 Cas.
0.8
1
1.2
1.4
1.6
1.8
2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
φ And
Hα
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
φ And
FeII 4233
FeII 4584
OI 7772
Fig.A.6. Profiles of Hα, Fe II 4233, 4584 ˚
A, and O I77725˚
A lines of φAnd.
1
1.5
2
2.5
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
OT Gem
Hα
0.8
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
OT Gem
OI 7772
Fig.A.7. Profiles of Hαand O I77725˚
A lines of OT Gem.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 5
0.6
0.8
1
1.2
1.4
1.6
1.8
2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
β CMi
Hα
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
β CMi
FeII 5317
FeII 5235
FeII 5169
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
β CMi
FeII 6456
FeII 7712
OI 7772
Fig.A.8. Profiles of Hα, Fe II 5169, 5235, 5317, 6456, 7712, and O I77725˚
A lines of βCMi.
0.8
1
1.2
1.4
1.6
1.8
2
2.2
2.4
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
V974 Her
Hα
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
V974 Her
FeII 7712
OI 7772
Fig.A.9. Profiles of Hα, Fe II 77712 ˚
A, and O I77725˚
A lines of V974 Her (HD 164447).
0.8
1
1.2
1.4
1.6
1.8
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HR 6984
Hα
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HR 6984
OI 7772
Fig.A.10. Profiles of Hαand O I77725˚
A lines of HR 6984 (HD 171780).
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 6
0.8
0.85
0.9
0.95
1
1.05
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
60 Cyg
Hα
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
60 Cyg
OI 7772
Fig.A.11. Profiles of Hαand O I77725˚
A lines of 60 Cyg.
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
β Cep
Hα
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
β Cep
OI 7772
Fig.A.12. Profiles of Hαand O I77725˚
A lines of βCep.
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
V360 Lac
Hα
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
V360 Lac
OI 7772
Fig.A.13. Profiles of Hαand O I77725˚
A lines of V 360 Lac.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 7
A.3. Em subclass
1
2
3
4
5
6
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ο Cas
Hα
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ο Cas
FeII 5317
FeII 5235
FeII 5169
FeII 4233
FeII 4584
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ο Cas
FeII 7516
FeII 7712
OI 7772
Fig.A.14. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 7516, 7712 ˚
A, and O I77725˚
A lines of oCas.
0.5
1
1.5
2
2.5
3
3.5
4
4.5
5
−30 −20 −10 0 10 20 30
Relative Intensity
∆λ (Å)
γ Cas
Hα
0
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
γ Cas
FeII 5317
FeII 5235
FeII 5169
FeII 4233
FeII 4584
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
γ Cas
FeII 7516
FeII 7712
OI 7772
Fig.A.15. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 7516, 7712 ˚
A, and O I77725˚
A lines of γCas.
1
1.5
2
2.5
3
3.5
4
4.5
5
5.5
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
φ Per
Hα
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
φ Per
FeII 5317
FeII 5235
FeII 5169
FeII 4233
FeII 4584
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
φ Per
FeII 7516
FeII 7712
OI 7772
Fig.A.16. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 7516, 7712 ˚
A, and O I77725˚
A lines of φPer.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 8
0.5
1
1.5
2
2.5
3
3.5
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HR 894
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HR 894
FeII 5317
FeII 5235
FeII 5169
OI 7772
Fig.A.17. Profiles of Hα, Fe II 5169, 5235, 5317 ˚
A, and O I77725˚
A lines of HR 894.
1
2
3
4
5
6
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ψ Per
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ψ Per
FeII 6432
FeII 6456
OI 7772
FeII 7712
Fig.A.18. Profiles of Hαand Fe II 6432, 6456, 7712 ˚
A lines of ψPer.
0.5
1
1.5
2
2.5
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
η Tau
Hα
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
η Tau
OI 7772
Fig.A.19. Profiles of Hαand O I77725˚
A lines of ηTau.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 9
1
1.5
2
2.5
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HR 1500
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HR 1500
FeII 5317
FeII 5235
FeII 5169
OI 7772
Fig.A.20. Profiles of Hα, Fe II 5169, 5235, 5317 ˚
A, and O I77725˚
A lines of HR 1500.
1
1.5
2
2.5
3
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
κ Dra
Hα
0
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
κ Dra
FeII 4233
FeII 4584
FeII 5363
FeII 5317
FeII 5235
FeII 5169
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
1.3
1.4
−15−10 −5 0 5 10 15
Relative Intensity
∆λ (Å)
κ Dra
FeII 6456
FeII 7516
FeII 7712
OI 7772
Fig.A.21. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 5363, 6456, 7516, 7712 ˚
A, and O I77725˚
A lines of κDra.
0.5
1
1.5
2
2.5
3
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HD 175863
Hα
0.5
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HD 175863
OI 7772
FeII 7712
FeII 6456
Fig.A.22. Profiles of Hα, Fe II 6456, 7712 ˚
A, and O I77725˚
A lines of HD 175863.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 10
0.5
1
1.5
2
2.5
3
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
25 Vul
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
25 Vul
FeII 5317
FeII 5235
FeII 5169
OI 7772
Fig.A.23. Profiles of Hα, Fe II 5169, 5235, 5317 ˚
A, and O I77725˚
A lines of 25 Vul.
0.6
0.8
1
1.2
1.4
1.6
1.8
2
2.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
59 Cyg
Hα
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
59 Cyg
FeII 7516
FeII 7712
OI 7772
Fig.A.24. Profiles of Hα, Fe II 7516, 7712 ˚
A, and O I77725˚
A lines of 59 Cyg.
1
2
3
4
5
6
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
6 Cep
Hα
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
6 Cep
FeII 5317
FeII 5235
FeII 5169
FeII 4233
FeII 4584
0.6
0.8
1
1.2
1.4
1.6
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
6 Cep
FeII 6456
FeII 7516
FeII 7712
OI 7772
Fig.A.25. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 6456, 7516, 7712 ˚
A, and O I77725˚
A lines of 6 Cep.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 11
0.8
0.9
1
1.1
1.2
1.3
1.4
1.5
1.6
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HD 206773
Hα
0.5
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HD 206773
FeII 7516
FeII 7712
OI 7772
Fig.A.26. Profiles of Hα, Fe II 7516, 7712 ˚
A, and O I77725˚
A lines of HD 206773.
1
2
3
4
5
6
7
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
β Psc
Hα
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
β Psc
FeII 7516
FeII 7712
OI 7772
Fig.A.27. Profiles of Hα, Fe II 7516, 7712 ˚
A, and O I77725˚
A lines of βPsc.
1
2
3
4
5
6
7
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
EE Cep
Hα
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−15−10 −5 0 5 10 15
Relative Intensity
∆λ (Å)
EE Cep
FeII 7712
FeII 7516
OI 7772
Fig.A.28. Profiles of Hα, Fe II 7516, 7712 ˚
A, and O I77725˚
A lines of EE Cep.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 12
A.4. Sh subclass
0
1
2
3
4
5
6
7
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
28 Tau
Hα
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
28 Tau
FeII 5169
FeII 5235
FeII 5317
FeII 4233
FeII 4584
0.8
1
1.2
1.4
1.6
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
28 Tau
FeII 7516
FeII 7712
OI 7772
Fig.A.29. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 7516, 7712 ˚
A, and O I77725˚
A lines of 28 Tau.
1
1.5
2
2.5
3
3.5
4
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ζ Tau
Hα
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ζ Tau
FeII 5317
FeII 5235
FeII 5169
FeII 4233
FeII 4584
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ζ Tau
FeII 7516
FeII 7712
OI 7772
Fig.A.30. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 7516, 7712 ˚
A, and O I77725˚
A lines of ζTau.
0.6
0.8
1
1.2
1.4
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ψ9 Aur
Hα
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ψ9 Aur
OI 7772
Fig.A.31. Profiles of Hαand O I77725˚
A lines of ψ9Aur.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 13
0.6
0.8
1
1.2
1.4
1.6
1.8
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
4 Her
Hα
0.2
0.4
0.6
0.8
1
1.2
1.4
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
4 Her
FeII 5317
FeII 5235
FeII 5169
FeII 4584
FeII 4233
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
4 Her
FeII 7712
OI 7772
Fig.A.32. Profiles of Hα, Fe II 4233, 4584, 5169, 5235, 5317, 7712 ˚
A, and O I77725˚
A lines of 4 Her.
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
88 Her
Hα
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
88 Her
FeII 6456
FeII 7712
OI 7772
Fig.A.33. Profiles of Hα, Fe II 6456, 7712 ˚
A, and O I77725˚
A lines of 88 Her.
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
V532 Lyr
Hα
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
V532 Lyr
OI 7772
Fig.A.34. Profiles of Hα, Fe II 6516 ˚
A, and O I77725˚
A lines of HR 6971 (HD 171406, V 532 Lyr).
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 14
0.5
1
1.5
2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HD 179343
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HD 179343
FeII 7712
OI 7772
Fig.A.35. Profiles of Hα, Fe II 7712 ˚
A, and O I77725˚
A lines of HD 179343.
0.5
1
1.5
2
2.5
3
3.5
4
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
EW Lac
Hα
0
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
EW Lac
FeII 7712
FeII 6456
OI 7772
FeII 7516
Fig.A.36. Profiles of Hα, Fe II 6456, 7516, 7712 ˚
A, and O I77725˚
A lines of EW Lac.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 15
A.5. Ab subclass
0.4
0.6
0.8
1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
α And
Hα
0.85
0.9
0.95
1
1.05
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
α And
OI 7772
Fig.A.37. Profiles of Hαand O I77725˚
A lines of αAnd.
0.2
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
γ Peg
Hα
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−15−10 −5 0 5 10 15
Relative Intensity
∆λ (Å)
γ Peg
OI 7772
Fig.A.38. Profiles of Hαand O I77725˚
A lines of γPeg.
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HD 23873
Hα
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HD 23873
FeII 7712
OI 7772
Fig.A.39. Profiles of Hα, Fe II 7712 ˚
A, and O I77725˚
A lines of HD 23873.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 16
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ε Per
Hα
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ε Per
OI 7772
Fig.A.40. Profiles of Hα, Fe II 6516 ˚
A, and O I77725˚
A lines of εPer.
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ρ Aur
Hα
0.2
0.4
0.6
0.8
1
1.2
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ρ Aur
FeII 5169
FeII 6456
FeII 7516
OI 7772
Fig.A.41. Profiles of Hα, Fe II 5169, 6456, 7516, and O I77725˚
A lines of ρAur.
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
HR 1847A
Hα
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
HR 1847A
OI 7772
Fig.A.42. Profiles of Hαand O I77725˚
A lines of HR 1847A.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 17
0.4
0.6
0.8
1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
β CMa
Hα
0.8
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
β CMa
FeII 7462
OI 7772
Fig.A.43. Profiles of Hα, Fe II 7462 ˚
A, and O I77725˚
A lines of βCMa.
0.6
0.7
0.8
0.9
1
1.1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
α Leo
Hα
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
α Leo
FeII 5169
OI 7772
Fig.A.44. Profiles of Hα, Fe II 5169 ˚
A, and O I77725˚
A lines of αLeo.
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
η UMa
Hα
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
η UMa
FeII 5169
OI 7772
Fig.A.45. Profiles of Hα, Fe II 5169 ˚
A, and O I77725˚
A lines of ηUMa.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 18
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
θ CrB
Hα
0.65
0.7
0.75
0.8
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
θ CrB
FeII 5169
OI 7772
Fig.A.46. Profiles of Hα, Fe II 5169 ˚
A, and O I77725˚
A lines of θCrB.
0.3
0.4
0.5
0.6
0.7
0.8
0.9
1
1.1
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ζ Dra
Hα
0
0.2
0.4
0.6
0.8
1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ζ Dra
FeII 4233
FeII 4584
FeII 5235
FeII 5169
FeII 5317
0.6
0.7
0.8
0.9
1
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
ζ Dra
FeII 6456
OI 7772
Fig.A.47. Profiles of Hα, Fe II 4233. 4584, 5169, 5235, 5317, 6456 ˚
A and O I77725˚
A lines of ζDra.
0.2
0.4
0.6
0.8
1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
ι Her
Hα
0.6
0.8
1
1.2
1.4
1.6
1.8
−15 −10 −5 0 5 10 15
Relative Intensity
∆λ (Å)
ι Her
FeII 5317
FeII 5235
FeII 5169
OI 7772
Fig.A.48. Profiles of Hα, Fe II 5169, 5235, 5317 ˚
A, and O I77725˚
A lines of ιHer.
S. M. Saad et al.: Observations of Hα, iron, and oxygen lines in B, Be, and shell stars,Online Material p 19
0.4
0.6
0.8
1
1.2
−40 −20 0 20 40
Relative Intensity
∆λ (Å)
96 Her
Hα
0.85
0.9
0.95
1
1.05
1.1
−20 −10 0 10 20
Relative Intensity
∆λ (Å)
96 Her
OI 7772
Fig.A.49. Profiles of Hαand O I77725˚
A lines of 96 Her.
... Finally, 10 Cas (BS 7) is the lowest temperature Be star in our sample (spectral type B9). It has not been closely studied, and only a few spectroscopic observations have been reported in the literature (e.g., [62][63][64]). The Hα profile is double-peaked (except in the spectrum presented in [63] where it is single-peaked, which might be due to low resolution) and occupies a central part of a broad photospheric absorption line (see top left panel of Figure 17). ...
... It has not been closely studied, and only a few spectroscopic observations have been reported in the literature (e.g., [62][63][64]). The Hα profile is double-peaked (except in the spectrum presented in [63] where it is single-peaked, which might be due to low resolution) and occupies a central part of a broad photospheric absorption line (see top left panel of Figure 17). To the best of our knowledge, no significant variations in the Hα line (which, along with Hβ, is the only emission feature in the object's optical spectrum) have been documented. ...
... The collected spectra allowed us to confirm earlier findings for the objects with already known periods (see Table 1), reveal periodicities in others, and obtain more insights into the V/R behavior in general. It was expected from the previous studies that: (1) it takes time for V/R variations to become regular and phase-locked (e.g., [24] for π Aqr); (2) double-peaked emission-line profiles of the Balmer lines (especially those of the Hα line) may turn into more complicated structures (e.g., triple-peaked, see [63] for ν Gem, [65] for π Aqr); (3) the V/R ratio may change significantly and vary randomly (e.g., [61] for EW Lac). ...
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Citation: Miroshnichenko, A.S.; Chari, R.; Danford, S.; Prendergast, P.; Aarnio, A.N.; Andronov, I.L.; Chinarova, L.L.; Lytle, A.; Amantayeva, A.; Gabitova, I.A.; et al. Abstract: There is growing evidence that many Be stars are parts of binary systems. As the B-type primaries are very fast rotators and their spectral lines may be distorted by the circumstellar material, it is not easy to measure their radial velocity directly from the spectral lines. It has been shown that some Be binaries exhibit peak intensity variations consisting of double-peaked Hα lines that are phase-locked with orbital periods. We searched for such variations in the spectra of 12 Be stars, including several known and suspected binaries. Our results include confirmation of the orbital periods in ν Geminorum, Capricorni, κ Draconis, 60 Cygni, and V2119 Cygni, its refinement in o Puppis, as well as suggesting hints for binarity in o Aquarii, BK Camelopardalis, and 10 Cassiopeae. Monitoring of the Hα line profile variations in β Canis Minoris for over the last 10 years gives further support to the existence of a 182.5-day period found earlier in a smaller set of data. A similar but still preliminary period (179.6 days) was found in the Hα line profile variations in ψ Persei. It is shown for the first time that ν Geminorum exhibits phase-locked variations in the Hα emission peak intensity ratio and, therefore, is a part of the inner binary in this triple system. Our results show that the mentioned phase-locked peak intensity variations are observed in more Be binary systems than previously known and can be used to search for binarity of Be stars when application of other methods is inconclusive.
... The spectrum covers the wavelength range 3450 A° - 8620A° the Balmer lines up to H15 as well as some infrared lines are seen. The resolving power is R = 20000 which analogue to FWHM = 0.25 A°.Table 1 represents the list of observed objects and their published parameters , for details we refer to [7] and reference there in. ...
... It has been assigned to this group by [22] who demonstrated its variability in radial velocity with a single period of 0.1517 d and amplitude of 3.5 km/s. Hα is in sharp absorption [7]. Our spectrum for γ Peg cover only observations from 5850 A° to 8350 A° and we hope in future to collect observation for this star in a wider visible wavelengths to get more accurate results. ...
... Both Hα and OI 7772 A° -5 A° lines show absorption. FeII 6456, 7516, and 7712 A° lines are not visible, while both 6516 and 5169 A° lines are very weak [7]. θ CrB (HD 138794, HR 5778, HIP 76127). ...
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We present model atmosphere analysis for a sample of B-type stars in optical region to obtain their fundamental parameters e.g. effective temperature, surface gravities, and rotational velocities. Approximate masses for the sample of stars under study are obtained by comparing the resulted effective temperatures and surface gravities with the evolutionary tracks. Comparison between these masses and the empirical effective temperatures-mass relation revealed good agreement.
... Besides our FEROS data, several authors observed the Hα line profiles of β Psc with different instrumentation (Slettebak & Reynolds 1978;Andrillat & Fehrenbach 1982;Hanuschik et al. 1988Hanuschik et al. , 1996Banerjee et al. 2000;Saad et al. 2006;Silaj et al. 2010) and recently, many amateur astronomers contributed to the BeSS data base. The whole set of observations is not uniformly sampled in time. ...
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A study on the photosphere and disc of the Be star β Psc is presented. We recover almost 40 yr of high-resolution spectroscopic observations and additional data gathered from the BeSS data base. We evaluate the photospheric parameters from the spectral energy distribution (SED) and fittings of state-of-the-art non-LTE model atmospheres to observed helium, carbon, silicon, and magnesium line profiles. Our models include the stellar geometric deformation as well as the co-latitude dependence of temperature and gravity, aiming to derive the effects of rotation on the stellar parameters. We estimate the circumstellar disc parameters from the fitting of models assuming different disc properties, namely its radius and gas density profile. The disc inclination angle i is constrained from the fittings of He i 4471 Å, Mg ii 4481 Å, C ii 4267 Å, and Si ii 4128, 4132 Å lines with gravity darkened models. Our findings, based on model fittings, suggest that during the last 40 yr, the disc radius changed within the interval 5.5 ≤ Rd ≤ 7.8 $R/R_{*}\,$, the disc base gas density within 5 × 10−13 ≤ ρ ≤ 1 × 10−12 g cm−3, while the radial power-law density index m assumed values between 2.0 and 2.3. These results are in agreement with recent works dealing with spectroscopic and interferometric measurements of this object.
... Besides our FEROS data, several authors observed the Hα line profiles of β Psc with different instrumentation (Slettebak & Reynolds 1978;Andrillat & Fehrenbach 1982;Hanuschik et al. 1988Hanuschik et al. , 1996Banerjee et al. 2000;Saad et al. 2006;Silaj et al. 2010) and recently, many amateur astronomers contributing to the BeSS database. The whole set of observations are not uniformly sampled in time. ...
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A study on the photosphere and disc of the Be star $\beta$ Psc is presented. We recover almost 40 years of high-resolution spectroscopic observations and additional data gathered from the BeSS database. We evaluate the photospheric parameters from the SED and fittings of state-of-the-art non-LTE model atmospheres to observed helium, carbon, silicon and magnesium line profiles. Our models include the stellar geometric deformation as well as the co-latitude dependence of temperature and gravity, aiming to derive the effects of rotation on the stellar parameters. We estimate the circumstellar disc parameters from the fitting of models assuming different disc properties, namely its radius and gas density profile. The disc inclination angle $i$ is constrained from the fittings of He I 4471 \r{A}, Mg II 4481 \r{A}, C II 4267 \r{A}, and Si II 4128, 4132 \r{A} lines with gravity darkened models. Our findings, based on model fittings, suggest that during the last 40 years the disc radius changed within the interval $5.5 \le R_d \le 7.8$ $R_*$, the disc base gas density within $5 \times 10^{-13} \le \rho \le 1 \times 10^{-12}$ $g.cm^{-3}$, while the radial power-law density index $m$ assumed values between 2.0 and 2.3. These results are in agreement with recent works dealing with spectroscopic and interferometric measurements of this object.
... They were therefore removed from the study. The remaining eight stars are all well known classical Be (shell) stars, most of which have been observed and studied by various other groups of authors (see, e.g., Jaschek et al. 1980; Slettebak 1982 and, more recently, Rivinius et al. 2006; Saad et al. 2006). As detailed in Paper I, all of the observations presented in our catalog were obtained between 2005 and 2008 with the fiberfedéchellefed´fedéchelle spectrograph attached to the 42 inch John S. Hall telescope at the Lowell Observatory, located near Flagstaff, AZ. ...
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A new set of theoretical Hα emission line profiles of Be stars has been computed using the code BERAY, which solves the transfer equation along a series of rays passing through the star+disk system, representing an improved treatment over earlier work done by the authors. The new profiles were compared with the previous work, and general trends (such as line profile shapes and correlations between line equivalent widths as a function of initial density ρ0 and power law index n) were recovered. Additionally, BERAY was employed to model the spectra of eight well-known Be shell stars. Some degeneracy was found in the choice of model parameters, highlighting the need to employ alternate observables to constrain the models. However, the inclination angle of the model seemed relatively insensitive to the choices of other parameters, and we show that, with our models, only a very small range of inclination angles can adequately reproduce the observations. Five of our eight targets were found to have inclination angles of 70° or higher, and two more were found to have inclination angles of 67° and 65°. The observation of one target—4 Aquilae—could only be reproduced by models created at an inclination angle of approximately 45°.
... The spectra of the stars under investigation were secured mostly using the echelle spectrograph HEROS attached to the Cassegrain focus of the 2-m telescope at the Ondřejov observatory. Additional observations of several stars were obtained using a CCD camera attached to the coudé spectrograph of the same telescope, Table 1 in Saad et al. (2006) lists the studied stars. ...
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We present the equivalent width measurements of the hydrogen H α line, the oxygen near-IR triplet OI 7772–5 and of a number of FeII lines in several B, Be, and shell stars in optical and near-infrared regions. A study of the correlations between all these measured quantities has been made. The correlations of strength of lines with collected data of the near-IR color excess, the rotational velocity and the intrinsic polarization are also obtained and presented.
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The eclipsing binary α CrB, is a well-known double-lined spectroscopic binary. The system is considered unique among main-sequence systems with respect to its small mass ratio and large magnitude difference between the components. Our aim in the present paper is to compute the orbital parameters and to model the atmospheric parameters of the system. Synthetic spectral analysis of both the individual and disentangled spectra has been performed and yielded effective temperatures T eff = 10000±250 K, surface gravities logg = 4±0.25 and projected rotational velocities \(\emph{v}\) sini = 110±5 km/sec for the primary component, and T eff = 6000±250 K and logg = 4.5±0.25 for the secondary component. Evolutionary state of the system is investigated using stellar models.
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Context. Be stars are fast-rotating early-type emission line stars. It is generally assumed that observed emission is generated in a rotating disk-like envelope, as supported by the observed correlation between the stellar projected rotational velocity vsini and the width of the emission lines. Then, high-resolution spectroscopic observations of Balmer lines profiles play an important role in putting constraints on Be stars modeling. Aims: We present Balmer lines spectroscopy for a sample of 48 Be stars. For most of them, Hα and Hβ have been observed more than two times, in a total period spanning almost two years between 2008 and 2009. Methods: Spectral synthesis of the Hα profile was performed following two steps: photospheric contribution was computed by using Kurucz's code ATLAS9 and SYNTHE, and disk emission was derived by the approach of Hummel & Vrancken (2000, A&A, 302, 751). Results: For 26 out of 48 stars, a modeling of the total Hα emission, i.e. photospheric absorption plus disk net emission, has been attempted. By this modeling we derived an estimation of the disk radius, as well as the inclination angle between the rotational axis with line of sight and the base density at the stellar equator. For the stars observed more than once, we also discuss the variability of Hα and Hβ for what concerns both the equivalent width and the spectral profile. We found 16 stars with variable equivalent width and 7 stars with clear signs of profile variations. Conclusions: For all the stars in our sample, we derive all the fundamental astrophysical quantities, such as, effective temperature, gravity, and projected rotational velocity. We found 13 stars whose equivalent width is variable with a confidence level greater than 80% and 7 object for which spectral profiles show change with time. According to the commonly used classification scheme, we classified 16 stars as belonging to class 1, 13 to class 2, 11 are shell stars, 6 objects do not show net emission, and 2 stars display transitions from class 1 and 2. For the class 1 stars, we confirm the correlation between vsini and peak separation. Concerning the geometry of the disk, we derived the base density at the stellar equator, the radius, and the inclination angle between rotational axis and line of sight. The maximum concentration of stars occurs for disk dimensions ranging in the interval of 6 to 8 stellar radii and for inclination angles going from 23° to 35°. The observed spectra and Table B.1 are available in electronic form at the CDS via anonymous ftp to cdsarc.u-strasbg.fr (130.79.128.5) or via http://cdsarc.u-strasbg.fr/viz-bin/qcat?J/A+A/550/A79
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Spectrophotometrically measured continuum energy distribution of gamma Cassiopeiae are presented during six nights in the wavelength range of ⪅⪅ 3200-8000 Å. The observations are compared with the theoretical models and are used to derive the values of effective temperature, gravity and to explore the behaviour of the continuum. It is found that gamma Cassiopeiae exhibited moderate to strong near-ultraviolet and near-infrared excess radiation over the underlying photospheric emission, with variable intensity on a time-scale of months to years. The amount of extra emission has been measured in magnitude units. The discovery of two steps in Balmer jumps during one night is being reported for the first time in this star. The second step of Balmer jump is found strongly in emission and exhibited short time-scale variations. The measures of Balmer jumps and ⪅_1(Å) parameters are also made for this star.
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Context. The first magnetic fields in O- and B-type stars that do not belong to the Bp-star class, have been discovered. The cyclic UV wind-line variability, which has been observed in a significant fraction of early-type stars, is likely to be related to such magnetic fields. Aims. We attempt to improve our understanding of massive-star magnetic fields, and observe twenty-five carefully-selected, OB-type stars. Methods. Of these stars we obtain 136 magnetic field strength measurements. We present the UV wind-line variability of all selected targets and summarise spectropolarimetric observations acquired using the MUSICOS spectropolarimeter, mounted at the TBL, Pic du Midi, between December 1998 and November 2004. From the average Stokes I and V line profiles, derived using the LSD method, we measure the magnetic field strengths, radial velocities, and first moment of the line profiles. Results. No significant magnetic field is detected in any OB-type star that we observed. Typical 1{\sigma} errors are between 15 and 200 G. A possible magnetic-field detection for the O9V star 10 Lac remains uncertain, because the field measurements depend critically on the fringe- effect correction in the Stokes V spectra. We find excess emission in UV-wind lines, centred about the rest wavelength, to be a new indirect indicator of the presence of a magnetic field in early B-type stars. The most promising candidates to host magnetic fields are the B-type stars {\delta} Cet and 6 Cep, and a number of O stars. Conclusions. Although some O and B stars have strong dipolar field, which cause periodic variability in the UV wind-lines, such strong fields are not widespread. If the variability observed in the UV wind-lines of OB stars is generally caused by surface magnetic fields, these fields are either weak (<~few hundred G) or localised.
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Systematic Be star observations with the HEROS spectrograph have been carried out in several long observing runs and seasons, mainly at the ESO La Silla Observatory. The HEROS data represents one of the most extended spectroscopic data sets for the Be star research. More complete and efficient diagnostics and a higher frequency resolution in analyses of periodic spectral variations were achieved, thanks to a combination of relatively high spectral resolution, a large sample of monitored spectral lines of different formation properties, long observing runs, and a relatively high frequency of observations of main targets. Important results concerning different parts of the extended atmospheres of Be stars and having strong impact on our understanding of these objects have been achieved.