EUVE spectroscopy of beta Canis majoris (B1 II-III) from 500 angstrom to 700 angstrom

被引:49
作者
Cassinelli, JP
Cohen, DH
MacFarlane, JJ
Drew, JE
LynasGray, AE
Hubeny, I
Vallerga, JV
Welsh, BY
Hoare, MG
机构
[1] UNIV WISCONSIN, FUS TECHNOL INST, MADISON, WI 53706 USA
[2] UNIV OXFORD, DEPT ASTROPHYS, OXFORD OX1 3RH, ENGLAND
[3] NASA, GODDARD SPACE FLIGHT CTR, GREENBELT, MD 20771 USA
[4] EUREKA SCI, OAKLAND, CA 94602 USA
[5] UNIV CALIF BERKELEY, SPACE SCI LAB, BERKELEY, CA 94720 USA
[6] MAX PLANCK INST ASTRON, D-69117 HEIDELBERG, GERMANY
关键词
ISM; abundances; line; identification; stars; early-type; individual (beta Canis Majoris); oscillations; ultraviolet;
D O I
10.1086/177023
中图分类号
P1 [天文学];
学科分类号
0704 ;
摘要
Observations of the bright variable star beta CMa (B1 II-III) made with the Extreme Ultraviolet Explorer (EUVE) are presented, We report on the continuous energy distribution, photospheric line identification, and the variability of the star, as well as the physical implications for the structure of the local interstellar medium. The star is one of the strongest EUV sources in the long-wavelength spectrometer of EUVE, and one of only two early-type stars whose photospheric continuum was detected by the EUVE spectrometers. This paper is primarily concerned with the portion of the spectrum that lies between the neutral helium ionization edge at 504 Angstrom and an effective cutoff by interstellar absorption near 700 Angstrom. As in our EUV analysis of the B2 II star epsilon CMa, we found that line-blanketed model atmospheres are not capable of predicting an energy distribution which matches observations in all wavelength regions. Consequently, we derived two set of basic parameters for the star (T-eff = 24,800 K, log g = 3.7; and T-eff = 23,250 K, log g = 3.5), depending whether we accept the measured angular diameter, or require an exact agreement between models and the observed visual flux. For the higher T-eff model, the predicted EUV flux is in agreement with observations, while for the lower T-eff the star's EUV continuum is about 5 times brighter than the predictions. In either case, the star does not show the order of magnitude EUV excess that was seen in epsilon CMa. Neither model fits the data near 2200 Angstrom, and additional photospheric opacity is proposed. The EUVE data also provide information concerning the low-density interstellar medium in the direction of beta CMa. We derive a neutral hydrogen column density of similar to 2 x 10(18) cm(-2) and estimate a fewer limit for the neutral helium column density of 1.4 x 10(18) cm(-2). This indicates that along this sight line much of the hydrogen is ionized while the helium is neutral, The EUVE spectrum shows many strong photospheric absorption features, similar to that of epsilon CMa. Evidence for a stellar wind is seen in the O v 630 Angstrom absorption feature. There is special interest in beta CMa because it is among the brightest of the beta Cephei class of variables, The pulsations in this class of star manifest themselves primarily as periodic effective temperature changes. We find that the semiamplitude of the change is 108(-32)(+31) K for the primary period. This result is consistent with that derived from an analysis of the UV continuum by Beeckmans & Burger (1977), but our 68% confidence limits are significantly smaller than their 1 sigma error bars, The general agreement implies that the pulsations do propagate between the layers where the optical and UV continua are formed and the layers where the EUV continuum forms, which is about six density scale heights higher in static models. The possibility that some pulsational energy deposition could occur within the outer photosphere is discussed. Our observations, taken over two time intervals separated by 70 days, resulted in the detection of the beat phenomenon owing to the three oscillation periods of beta CMa.
引用
收藏
页码:949 / 963
页数:15
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