Coordinated XTE/EUVE Observations of Algol NASA P.O. No. …small by Algol standards, with an...
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Coordinated XTE/EUVE
Observations of Algol
NASA P.O. No. S-73068-Z
Final Report
Submitted To:
National Aeronautics and Space Administration
Goddard Space Flight CenterGreenbelt MD 20771
Principal Investigator:
Robert A. Stern
Dept Hl-12 Bldg 252
Solar and Astrophysics Laboratory
Lockheed Martin ATC
3251 Hanover St.
Palo Alto, CA 94304
(415) 424-a272
October 10, 1997
https://ntrs.nasa.gov/search.jsp?R=19980004494 2020-03-11T22:34:16+00:00Z
1. Summary
We performed a coordinated RXTE observation of the prototypical eclipsing binary Algol
in conjunction with EUVE and ASCA observations. Observing the X-ray spectrum of
Algol with ASCA, EUVE, and RXTE provides critical, near-simultaneous constraints on
the distribution of the hottest temperature plasma in the Algol system: this is required
to unambiguously determine the coronal Fe abundance. After some initial shuffling of
observatory schedules with the help of mission planners, the coordinated multiwavelength
observation was successfully performed in February, 1996. Analysis of the data, including
development of new, IDL-based global model fitting routines, was accomplished from
mid-1996 to mid-1997. The results indicate that the initial estimates of [Fe/H] ,-_ 0.3
dex (Stern et al. 1995) are confirmed, and the Algol high temperature plasma thus has
an Fe deficiency relative to the (Anders and Grevesse 1989) solar abundance.
2. Technical Progress
The results of this investigation will be published (in CD ROM format) in the proceedings
of the 10th Workshop on Cool Stars, Stellar Systems, and the Sun, Cambridge, 1997,
ASP Conference Series, eds. J.A. Bookbinder & R.A. Donahue (San Francisco: ASP).
A hardcopy version of this paper is appended to this report.
Multiwavelength EUVE/ASCA/RXTE Observations of
Algol and the [Fe/H] Abundance
Robert A. Stern 1, James R. Lemen t Sandy Antunes 2 Stephen A.Drake 3, Fumiaki Nagase 4 Jfirgen H.M.M. Schmitt s KulinderpalSingh 6, Nicolas E. White 7
Abstract.
EUVE, ASCA, and XTE observed the eclipsing binary Algol (BetaPer) from 1-7 Feb 96. The coordinated observation covered _ 2 binaryorbits of the system, with a net exposure of _ 160 ksec for EUVE, 40 ksec
for ASCA (in 4 pointings}, and 9G ksec for XTE (in 45 pointings). Wediscuss results of modeling the combined EUVE, ASCA, and XTE datausing continuous differential emission measure distributions, and provide
constraints on the Fe abundance in the Algol system.
1. Introduction
The prototype eclipsing binary Algol (/3 Per; P = 2.87 d.), studied intensivelyin nearly all wavelength regions from IR to X-rays, is now beginning to revealmore of its multifaceted nature through both ASCA (Antunes, Nagase, andWhite 1994), and EUVE spectrometer observations (Stern et al. 1995). A keyresult in both of these investigations is that the highly ionized Fe X-ray line
complexes or individual EUV lines are considerably weaker than expected (rel-ative to the continuum or other spectral features) from models using the solarabundances of, e.g. Anders and Grevesse (1989). However, because these ob-servations were performed many months apart, and because of Algol's inherentvariability, a combined analysis of the earlier data is not possible. To remedythis, a coordinated EUVE/ASCA/XTE observation was undertaken to settlethe issue of the Fe abundance in Algol's corona and place limits on the form of
the differential emission measure (DEM) from 106-10 s K, using the presence ofthe strong Fe L complexes and the line-to-continuum ratios of the Fe lines.
I Solar and Astrophysics Lab/Lockheed Martin
2Hughes/STX
3NASA/USRA
4ISAS
5MPE/Garching
6Tara Inst. of Fund. Res.
7NASA/GSFC
2. Observations
EUVE observed Algol for more than 2 binary orbits, with a net exposure time of
140 ksec. ASCA co-observed for a total of_ 40 ksec in four separate pointings,and XTE in 40 pointings for _ 90 ksec. The ASCA data were taken largelyduring quiescent periods, which will be helpful in the combined emission measureand Fe abundance analysis. The XTE data sampled a much larger portion of the
EUVE observation, with concentrated periods of observation designed to overlapwith the ASCA observations. The times of the coordinated EUVE/ASCA/XTEobservations are indicated in Figure 1. Because of the late launch of XTE, theEUVE and ASCA observations were delayed by about 1 week: the high levelof coordination and cooperation among the various observatories and schedulersmade this last minute shift possible.
3. Results
3.1. EUVE Lightcurve
A lightcurve from the EUVE Deep Survey/Lexan filter (A -,_ 70-170/_) is shownin Figure 2. Note the nearly continuous variability of the Algol system in this
wave band, which is similar to the coverage of the EUVE Short Wavelength(SW) spectrometer. The flare occurring at about midday on Feb 3 is relativelysmall by Algol standards, with an exponential decay time £ 4 hr. Folding theDS/Lexan data with the orbital period of Algol, 2.867 d, results in the lightcurveshown in Figure 3. Although parts of the Algol lightcurve are reproducible fromorbit to orbit, successive orbits of the Algol system reveal numerous changes dueeither to small flares or evolution of activity patterns. For example, what appearsto be a secondary eclipse during the first orbit (_b _ 0.5) is masked by what isprobably a decaying flare during the second orbit. This lack of reproducibility
on an orbit-to-orbit basis suggests caution in attempting a detailed model ofEUV eclipses.
3.2. RXTE lightcurve
The RXTE observation was designed to provide _ one (spacecraft) orbit expo-sures, sampled throughout the EUVE observation. The RXTE PCA (Propor-tional Counter Array) data are strongly affected by instrumental background,which is highly variable during a given observation. Hence a correct backgroundcorrection algorithm is crucial. Using the software developed by Keith Jahodaand provided by the RXTE GOF, we have obtained a background-corrected
PCA lightcurve for the Algol observation. This is shown in Figure 4. Note thatthe RXTE and EUVE lightcurves are in rough correspondence, but the peak onthe larger flare is missed by RXTE, and there are still likely some systematiceffects present in the background subtraction.
3.3. EUVE/ASCA/RXTE Spectra and Continuous EM Model Fit
By filtering the EUVE spectrometer data, removing periods of high count rate (_
i c/s), we obtain what may be termed a "quiescent" spectrum in the EUVE SW
EUVE Start
04:00
Coordinoted EUVE/ASCA/XTE Times
08:00 12:00 16:00 20:00 00:[30
UT from 01-Feb-96 00:00:00
ICO:O0 04:00 08:00 12:00 16:00 20:00 00:00
UT from 02-Feb-96 00:00:00
00:00 04:00 08:00 12:00 16:00 20:00 00:00
UT from 05-F'eb-96 00:00:00
00:00 04:00 08:00 12:00 16:00 20:00 00:00
UT from 04-Feb-96 00:00:00
I0(3:00 04:00 08:00 12:00 16:00 20:00 00:0(3
UT from 05-Feb-96 00:00:00
00:00 04:00 08:00 12:00 16:00 20:00 00:(30
UT from 06-F'eb-96 00:00:00
I00:00 04:00 08;00 12:00 16:00 20:00 00:(30
UT from 07-Feb-96 00:00:00
Figure 1. Times of coordinated EUVE, ASCA, and XTE observa-tions. The EUVE observation start and end times are indicated by
vertical dashed lines. The ASCA times are indicated by the four line
shaded regions with the wider spacing, and the XTE observation times
by the more numerous line shaded regions with the smaller spacing.The indicated observation periods include some times of SAA passes,
earth occultations, etc.
and MW bands. Corresponding to this, we have selected the final ASCA obser-
vation, and the overlapping RXTE observations to match this "quiescent" data.
We have developed a multiwavelength version (MULTI_FIT) of the EUVE_FIT
software used to fit a spectrum to an emission measure (EM) distribution de-
scribed by a sum of Chebyshev polynomials (see Stern et aL 1995). The ASCA
and RXTE response matrices and effective areas were all computed using the
data analysis software provided by their respective GOFs. The output FITSfiles were then read into IDL and converted into data structures for use by
the MULTI_FIT software. The MULTI__FIT software was adapted to use the
models produced by the SPEX software of Mewe, Kaastra and Liedhal (1995),
EUVE DS/Lexon Light Curve + ASCA Coord Obs (Shoded)
Figure 2. EUVE Deep Survey/Lexan lightcurve (50-170 h). Thetimes of the coordinated ASCA observations are indicated by the line-
shaded regions.
with lines from each element separately calculated to allow for varying elementalabundances. In addition, the normalizations of the 3 instruments were allowed
to vary independently to allow for intercalibration effects, but never were > 15%from their nominal values. A fixed absorption of N_/_ 4 × 102° was applied tothe ASCA and RXTE data to account for known calibration problems with theASCA SIS.
We experimented with Chebyshev polynomials with nterms -- 6 to 25, andallowing the elements Fe, Mg, S, and Si to vary. In general, the fits, though notformally accepted, provided good representations of the spectra. A sample ofthe best fit results is given in Table 1. As can be seen, changing the numberof terms above ,,, 10-13 did not have a significant affect on the fit, and the
range of [Fe/H] values (relative to Anders and Grevesse 1989) was ,,_ 0.26-0.35.Attempting to place a formal confidence limit on this range is difficult, becauseof the dominance of systematic effects in the instrument calibrations and atomiccodes.
For the purposes of illustration, we show the fit results for nterms -- 11.The spectral fit in the EUVE SW and MW bands, the ASCA SIS and the RXTEPCA is shown in Figures 5-8 and the resulting EM distribution in Figure 9.
O3
O3
Z
O(D
2.0
1.5
1.0
0.5
Folded DS/Lexan LightcurveT _ T _ T _ i
0 ¢ = 0.00-0.99 !
A _ = 1.00-1.99 ?[] _ = 2.00-2.99
+÷ + ,I*+ ÷
+
44 4 +
, *I,+
44444
0.2 0.4 0.6 0.8 1.0
Orbitol Phase
Figure 3. Phased lightcurve for DS/Lexan data. Different plottingsymbols, indicated in the legend, refer to successive orbits.
4. Summary
The coordinated EUVE, ASCA, and XTE observations of Algol obtained inFebruary 1996 offer a unique opportunity to determine the EM distribution and
element abundances of the Algol system. Coordinated multiwavelength dataindicate consistency with earlier ASCA and EUVE results, i.e., an [Fe/H]30%. The simultaneous fitting of these results leaves no doubt that, unless theatomic physics data is wrong to the same degree in both the EUV and X-rayregions for the Fe L lines, the derived underabundances are real. The question ofthe photospheric Fe abundance of Algol is, however, still an unresolved problem.
Acknowledgments. This work was supported by NASA Contracts NAS5-
96052 (EUVE), PO# S-57785-Z (ASCA), PO# S-73068-Z (XTE) and the Lock-heed Martin Independent Research Program.
5
09
}--Z
00
6O
40
2O
o
Ol -Feb
I IRXTE PCA Light Curve
tt
I'
I I
t tltt i
I , I _ I , I , I , I
02-Feb 03-Feb 04-Feb 05-Feb 06-Feb 07-FebStort Time (01-Feb-95 00:00:00)
Figure 4. RXTE PCA Lightcurve for Algol observation.
References
Anders, E., and Grevesse, N., 1989, Geochim. Cosmochim. Acta, 53, 197.
Antunes, A., Nagase, F., and White, N.E., 1994, ApJ, 436, L83.
Mewe, R., Kaastra, J., and Liedhal, D., 1995, SPEX code.
Stern, R.A., Lemen, J.R., Schmitt, J.H.M.M., and Pye, J.P., 1995, ApJ, 444,L45.
6
Table 1. Chebyshev Polynomial Fit Results
Nterms X_ NFREE Fe Mg S Si O6 1.39 741 0.26 0.48 0.08 0.29 N/A
10 1.34 737 0.27 0.44 0.08 0.28 N/A15 1.35 732 0.26 0.42 0.09 0.28 N/A20 1.36 727 0.27 0.44 0.08 0.28 N/A25 1.37 722 0.27 0.44 0.08 0.28 N/A
11 1.52 737 0.26 0.73 N/A 0.41 N/A
11 1.49 737 0.35 0.90 0.20 N/A N/A11 1.39 737 0.31 N/A 0.18 0.40 N/A
11 1.48 737 0.31 1.1 N/A N/A 0.
$W
(fl
E
0(D
3O0
250
2O0
150
1O0
5O
0
i: :- _i
-:_...--',-.--_.._-_-:: ... !_. 1!:! . ,.:: , : , . . . : :.
(Drr" 80 1O0 120 140
Wovelength(/_,)
Figure 5. EUVE SW Spectral fits and residuals.
80-
60
0 i_ : _ :i _'ii _i_:h,i!_
_'_, : ' ! ' i
-20b.._,-4 :_., :_,;r.,_.::.',.._,%_'._
_ :""::"'":';:.I'"" '_!i_;:_"
1.50250 300
2.00 Wave_e ng_.h(,,&.")
55O
Figure 6.
_D
0
EUVE MW Spectral fits and residuals.
1000
BOO
600
400
ASCA
,/'200 . ,,,r_ . ___-_-_.
cE 0 wavelength
Figure 7.ASCA SIS Spectral fits and residualS.
8
8OO
6OO
03
C400
00
2OO
A
bo 0
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Wovelength(_,)
5
Figure 8. RXTE PCA Spectral fits and residuals.
Ou3
tad
3000
2000
1000
NTERMS = 11 NFREE =I I I
[, , , , I , , , , I , , , |, I i , ,
5.5 6.0 6.5 7.0
Log T
755
Figure 9. DEM for Nterms=ll Chebyshev Polynomial fit.
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4, TITLE AND SUBTITLE 5. FUNDING NUMBERS
Coordinated XTE/EUVE Observations of ALGOL
6. AUTHOR(S)
Robert A. Stern
7. PERFORMING ORGANIZATION NAME(S) AND ADDRESS (ES)
Lockheed Martin Corporation
3251 Hanover Street
Palo Alto, CA 94304-1191
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National Aeronautics and Space Administration
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S-73068-Z
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13. ABSTRACT (Maximum 200 words)
EUVE, ASCA, and XTE observed the eclipsing binary Algol (Beta Per) from 1-7 Feb. 96. The
coordinated observation covered - 2 binary orbits of the system, with a net exposure of - 160 ksec for
EUVE, 40 ksec for ASCA (in 4 pointing), and 90 ksec for XTE (in 45 pointings). We discuss results of
modeling the combined EUVE, ASCA, and XTE data using continuous differential emission measure
distributions, and provide constraints on the Fe abundance in the Algol system.
14. SUBJECT TERMS
EUVE, ASCA, XTE, Algol, Fe/H Abundance
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