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首页> 外文期刊>Astronomy and astrophysics >Observational calibration of the projection factor of Cepheids - II. Application to nine Cepheids with HST/FGS parallax measurements
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Observational calibration of the projection factor of Cepheids - II. Application to nine Cepheids with HST/FGS parallax measurements

机译:造父变星投影因子的观测标定-II。 HST / FGS视差测量应用于九个造父变星

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Context. The distance to pulsating stars is classically estimated using the parallax-of-pulsation (PoP) method, which combines spectroscopic radial velocity (RV) measurements and angular diameter (AD) estimates to derive the distance of the star. A particularly important application of this method is the determination of Cepheid distances in view of the calibration of their distance scale. However, the conversion of radial to pulsational velocities in the PoP method relies on a poorly calibrated parameter, the projection factor ( p -factor). Aims. We aim to measure empirically the value of the p -factors of a homogeneous sample of nine bright Galactic Cepheids for which trigonometric parallaxes were measured with the Hubble Space Telescope (HST) Fine Guidance Sensor. Methods. We use the SPIPS algorithm, a robust implementation of the PoP method that combines photometry, interferometry, and radial velocity measurements in a global modeling of the pulsation of the star. We obtained new interferometric angular diameter measurements using the PIONIER instrument at the Very Large Telescope Interferometer (VLTI), completed by data from the literature. Using the known distance as an input, we derive the value of the p -factor of the nine stars of our sample and study its dependence with the pulsation period. Results. We find the following p -factors: p = 1.20 ± 0.12 for RT Aur, p = 1.48 ± 0.18 for T Vul, p = 1.14 ± 0.10 for FF Aql, p = 1.31 ± 0.19 for Y Sgr, p = 1.39 ± 0.09 for X Sgr, p = 1.35 ± 0.13 for W Sgr, p = 1.36 ± 0.08 for β Dor, p = 1.41 ± 0.10 for ζ Gem, and p = 1.23 ± 0.12 for ? Car. Conclusions. The values of the p -factors that we obtain are consistently close to p = 1.324 ± 0.024 . We observe some dispersion around this average value, but the observed distribution is statistically consistent with a constant value of the p -factor as a function of the pulsation period ( χ ~(2) = 0.669 ). The error budget of our determination of the p -factor values is presently dominated by the uncertainty on the parallax, a limitation that will soon be waived by Gaia .
机译:上下文。传统上,使用脉动视差(PoP)方法估计到脉动星的距离,该方法结合了光谱径向速度(RV)测量值和角直径(AD)估计值来得出恒星的距离。该方法的一个特别重要的应用是,根据造父变星的距离刻度的校准来确定造父变星的距离。但是,在PoP方法中径向速度到脉动速度的转换依赖于校准系数较差的投影系数(p-factor)。目的我们的目的是凭经验测量9个亮银河造父星的均质样本的p因子值,并使用哈勃太空望远镜(HST)精细制导传感器测量了其三角视差。方法。我们使用SPIPS算法,这是PoP方法的可靠实现,该方法将光度法,干涉法和径向速度测量结合在恒星脉动的全局建模中。我们使用超大型望远镜干涉仪(VLTI)上的PIONIER仪器获得了新的干涉角直径测量结果,并通过文献数据完成了测量。使用已知距离作为输入,我们得出样本中九颗星的p因子值,并研究其与脉动周期的相关性。结果。我们发现以下p因子:对于RT Aur,p = 1.20±0.12,对于T Vul,p = 1.48±0.18,对于FF Aql,p = 1.14±0.10,对于Y Sgr,p = 1.31±0.19,对于p V = 1.39±0.09 X Sgr,对于W Sgr,p = 1.35±0.13,对于βDor,p = 1.36±0.08,对于ζGem,p = 1.41±0.10,对于βδ,p = 1.23±0.12。汽车。结论。我们获得的p因子的值始终接近p = 1.324±0.024。我们在这个平均值附近观察到一些离散,但是观察到的分布在统计上与作为脉动周期的函数的p因子的恒定值一致(χ〜(2)= 0.669)。目前,我们确定p因子值的误差预算主要由视差的不确定性决定,Gaia很快将放弃这一限制。

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