{"title":"SZ Lyn:基于旧的和最近的光度观测的新的脉动和轨道元素","authors":"K. Gazeas, P. Niarchos, K. Boutsia","doi":"10.1553/CIA145S47","DOIUrl":null,"url":null,"abstract":"SZ Lyncis (=HD 67390) is a high amplitude δ Scuti star, discovered by Hoffmeister in 1949. Van Genderen (1967) noticed that the residuals in the O-C diagrams followed a sinusoidal variation with a period of Porb = 3.091 years. Several years later, Barnes & Moffett (1975) improved this period to Porb = 3.138 years and suggested that the sinusoidal variations in the O-C diagrams, observed by van Genderen (1967), originate from the light travel time effect, since SZ Lyn is a member of a binary system. This hypothesis was confirmed by Bardin & Imbert (1984) with measurements of radial velocities. Soliman et al. (1986) found the pulsation period to be 0.120534896 days and the orbital period 1173.5 days. From BVRI observations during the period January 1975 March 1979, Moffett et al. (1988) estimated the pulsational period as 0.12052115 days, which is shorter than earlier determinations. The latest research was made by Paparo et al. (1988), who determined the pulsational and orbital elements of the system even better, using all available data from 1961 until 1988. In this paper we present the results of new CCD time-series photometry carried out at the University of Athens Observatory. Our new BVRI CCD photometric observations and those obtained by Derekas et al. (2003) and Hipparcos (ESA 1997) extended the time base of the data from 27 to 42 years (or from 8 to 14 revolutions of the system). The 165 times of maxima observed between 1961 and 2003 were used to calculate the pulsational and orbital elements of the binary system. A new ephemeris was calculated with the new times of maxima, derived from our light curves: tmax(HJD) = 2452776.289(10) + 0d.1205349(41)×E; From a least squares fit to all available O-C values we were able to calculate more precise values of the following parameters: the linear change in the star’s pulsational period (β=2.90±0.22 × 10−12 days/cycle), the orbital period (Porb=1179.3±2 days), the semimajor axis (a sin i=0.998±0.04 AU), the eccentricity (e=0.205±0.010), the longitude and time of the periastron passage (ω=87.6±1.1 degrees and T (HJD)=2445699.8436±0.022) and the mass function f(M)=0.095±0.008.","PeriodicalId":151133,"journal":{"name":"Third Coast","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2004-06-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"SZ Lyn: New pulsational and orbital elements based on old and recent photometric observations\",\"authors\":\"K. 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(1988) estimated the pulsational period as 0.12052115 days, which is shorter than earlier determinations. The latest research was made by Paparo et al. (1988), who determined the pulsational and orbital elements of the system even better, using all available data from 1961 until 1988. In this paper we present the results of new CCD time-series photometry carried out at the University of Athens Observatory. Our new BVRI CCD photometric observations and those obtained by Derekas et al. (2003) and Hipparcos (ESA 1997) extended the time base of the data from 27 to 42 years (or from 8 to 14 revolutions of the system). The 165 times of maxima observed between 1961 and 2003 were used to calculate the pulsational and orbital elements of the binary system. 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引用次数: 0
摘要
SZ Lyncis (=HD 67390)是一颗高振幅δ Scuti星,由Hoffmeister于1949年发现。Van Genderen(1967)注意到O-C图的残差遵循一个周期为Porb = 3.091年的正弦变化。几年后,Barnes & Moffett(1975)将这个周期改进为Porb = 3.138年,并提出van Genderen(1967)观察到的O-C图中的正弦变化源于光传播时间效应,因为SZ Lyn是双星系统的成员。这个假设被Bardin和Imbert(1984)用径向速度的测量证实了。Soliman et al.(1986)发现其脉动周期为0.120534896天,轨道周期为1173.5天。Moffett et al.(1988)根据1975年1月至1979年3月期间的BVRI观测,估计脉动周期为0.12052115天,比以前的测定短。最新的研究是由Paparo等人(1988)进行的,他们利用1961年至1988年的所有可用数据,更好地确定了该系统的脉动和轨道元素。本文介绍了在雅典大学天文台进行的新型CCD时间序列光度测量的结果。我们新的BVRI CCD光度观测和Derekas et al.(2003)和Hipparcos (ESA 1997)获得的数据将数据的时间基础从27年延长到42年(或从系统的8到14转)。1961年至2003年间观测到的165次极大值被用来计算双星系统的脉动和轨道元素。根据我们的光曲线,计算了新的星历表:tmax(HJD) = 2452776.289(10) + 0d.1205349(41)×E;通过对所有可用的O-C值进行最小二乘拟合,我们能够计算出以下参数的更精确值:恒星的脉动周期(β=2.90±0.22 × 10−12天/周期)、轨道周期(Porb=1179.3±2天)、半长轴(a sin i=0.998±0.04 AU)、偏心率(e=0.205±0.010)、经过近星点的经度和时间(ω=87.6±1.1度,T (hdd)=2445699.8436±0.022)和质量函数f(M)=0.095±0.008。
SZ Lyn: New pulsational and orbital elements based on old and recent photometric observations
SZ Lyncis (=HD 67390) is a high amplitude δ Scuti star, discovered by Hoffmeister in 1949. Van Genderen (1967) noticed that the residuals in the O-C diagrams followed a sinusoidal variation with a period of Porb = 3.091 years. Several years later, Barnes & Moffett (1975) improved this period to Porb = 3.138 years and suggested that the sinusoidal variations in the O-C diagrams, observed by van Genderen (1967), originate from the light travel time effect, since SZ Lyn is a member of a binary system. This hypothesis was confirmed by Bardin & Imbert (1984) with measurements of radial velocities. Soliman et al. (1986) found the pulsation period to be 0.120534896 days and the orbital period 1173.5 days. From BVRI observations during the period January 1975 March 1979, Moffett et al. (1988) estimated the pulsational period as 0.12052115 days, which is shorter than earlier determinations. The latest research was made by Paparo et al. (1988), who determined the pulsational and orbital elements of the system even better, using all available data from 1961 until 1988. In this paper we present the results of new CCD time-series photometry carried out at the University of Athens Observatory. Our new BVRI CCD photometric observations and those obtained by Derekas et al. (2003) and Hipparcos (ESA 1997) extended the time base of the data from 27 to 42 years (or from 8 to 14 revolutions of the system). The 165 times of maxima observed between 1961 and 2003 were used to calculate the pulsational and orbital elements of the binary system. A new ephemeris was calculated with the new times of maxima, derived from our light curves: tmax(HJD) = 2452776.289(10) + 0d.1205349(41)×E; From a least squares fit to all available O-C values we were able to calculate more precise values of the following parameters: the linear change in the star’s pulsational period (β=2.90±0.22 × 10−12 days/cycle), the orbital period (Porb=1179.3±2 days), the semimajor axis (a sin i=0.998±0.04 AU), the eccentricity (e=0.205±0.010), the longitude and time of the periastron passage (ω=87.6±1.1 degrees and T (HJD)=2445699.8436±0.022) and the mass function f(M)=0.095±0.008.