宽双星WDS 12483-6708恒星脉动的光度探测

Third Coast Pub Date : 2008-04-01 DOI:10.1553/CIA_153S17
D. Sinachopoulos, P. Gavras
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It is the HIC 62482 target of Hipparcos with V=7.58, (B−V) = 0.19 and parallax 10mas. The secondary star is HIC 62488 with magnitude V=8.74, (B − V) = 0.47 and has practically the same parallax of the primary. The proper motions of the two components are the same (common proper motion stars). These two facts show that this double star is not an optical pair. Hipparcos catalogue (ESA 1997) flags both components for ’duplicity-induced’ variability. Figure 1: A characteristic CCD exposure of WDS 12483-6708 in Stroemgren y filter 18 Photometric detection of pulsations in the wide binary WDS 12483-6708 Figure 2: Variability of the magnitude difference of the components of WDS 12483 − 6708, together with the fit of the two detected frequencies. We observed this double star in May 16, 2004, in the frame of astrometric observations of wide Hipparcos visual double stars (Sinachopoulos et al. 2007), using the STE4 CCD camera of SAAO observatory attached to the Cassegrain focus of the 1m telescope, using the Stroemgren y filter. To improve the instrumental accuracy of our measurements, especially the astrometric ones, we obtained sixteen CCD exposures of each double star similar to the image shown in Figure 1. Our -quasion-line data reduction resulted in an unexpectedly high value of the standard deviation of measured mean magnitude difference of the double star components. Since these two stars are in or close to the instability strip of the MS, we decided to spend five hours monitoring them photometrically. To our regret, there is no other star close WDS 12483-6708 bright enough which could be used as a comparison star, so we could only measure the variability of the magnitude difference of the two components. We took a series of ten-second exposures, which together with the CCD readout time resulted in 95 magnitude differences per hour. Our measurements are shown in Figure 2. Frequency analysis The light curve shows significant variability during the observational window. The largest amplitude we see in our measurements is about 0.02 mag. Consequently, Fourier analysis was performed using Period04 (Lenz & Breger 2005). Two frequencies were detected and listed in Table 1 together with their semi-amplitudes and phases. Uncertainties are calculated by least-square fitting. Frequencies and phases D. Sinachopoulos and P. Gavras 19 Table 1: Observed frequencies for WDS 12483-6708 y-Data Id. Frequency Semi-ampl. Phase [c/d] [mag] [cycles] f1 50.6 ±0.3 0.0032 ±0.0003 0.52 ±0.01 f2 60.1 ±0.3 0.0027 ±0.0003 0.54 ±0.02 are fitted uncorrelated. The difference of 9.5 c/d between the two detected frequencies is significantly larger than the proposed frequency resolution of 1.5/dT limit by Loumos &Deeming (1978), which in this case is 7.2 c/d. Residuals to the observations are 0.004 magnitudes. Discussion and Conclusion Despite the relatively low level of the photometric residuals, the two frequencies fitted to the data and shown in Figure 2 give rise to the need for additional observations. These should include observations of external comparison and check stars to uncover the variable component of the wide, without excluding the scenario of finding both of them pulsating. In any case, we were not able to locate any variable star previously known at these coordinates in the sky. This object is not listed in the Delta Scuti catalogue by Rodriguez et al. (2000). So, this paper reports the detection of at least one additional pulsating star in a wide double star system. Acknowledgments. We would like to thank SAAO for generous telescope time allocation.","PeriodicalId":151133,"journal":{"name":"Third Coast","volume":null,"pages":null},"PeriodicalIF":0.0000,"publicationDate":"2008-04-01","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":"{\"title\":\"Photometric detection of pulsations in the stars of the wide binary WDS 12483-6708\",\"authors\":\"D. Sinachopoulos, P. Gavras\",\"doi\":\"10.1553/CIA_153S17\",\"DOIUrl\":null,\"url\":null,\"abstract\":\"We detected stellar pulsations in at least one of the components of the wide double star WDS 12483-6708. The largest observed photometric amplitude, in Stroemgren filter y, is around 0.02 magnitudes with period about 0.02 days. The detection was based on five hours of differential CCD photometry of the two double star components. Individual Objects: WDS 12483-6708, HIC 62482, HIC 62488 Introduction and Observations WDS 12483-6708 is a wide double star detected in 1835. Since then, the relative positions of its components have been observed 16 times. The last observation listed in the Washington Double Star Catalogue (WDS) (Mason & Hartkopf 2006) is from the year 2000, when the angular separation of the components measured was 13.5 arcseconds. The primary of the system is a A3III/IV type star. It is the HIC 62482 target of Hipparcos with V=7.58, (B−V) = 0.19 and parallax 10mas. The secondary star is HIC 62488 with magnitude V=8.74, (B − V) = 0.47 and has practically the same parallax of the primary. The proper motions of the two components are the same (common proper motion stars). These two facts show that this double star is not an optical pair. Hipparcos catalogue (ESA 1997) flags both components for ’duplicity-induced’ variability. Figure 1: A characteristic CCD exposure of WDS 12483-6708 in Stroemgren y filter 18 Photometric detection of pulsations in the wide binary WDS 12483-6708 Figure 2: Variability of the magnitude difference of the components of WDS 12483 − 6708, together with the fit of the two detected frequencies. We observed this double star in May 16, 2004, in the frame of astrometric observations of wide Hipparcos visual double stars (Sinachopoulos et al. 2007), using the STE4 CCD camera of SAAO observatory attached to the Cassegrain focus of the 1m telescope, using the Stroemgren y filter. To improve the instrumental accuracy of our measurements, especially the astrometric ones, we obtained sixteen CCD exposures of each double star similar to the image shown in Figure 1. Our -quasion-line data reduction resulted in an unexpectedly high value of the standard deviation of measured mean magnitude difference of the double star components. Since these two stars are in or close to the instability strip of the MS, we decided to spend five hours monitoring them photometrically. To our regret, there is no other star close WDS 12483-6708 bright enough which could be used as a comparison star, so we could only measure the variability of the magnitude difference of the two components. We took a series of ten-second exposures, which together with the CCD readout time resulted in 95 magnitude differences per hour. Our measurements are shown in Figure 2. Frequency analysis The light curve shows significant variability during the observational window. The largest amplitude we see in our measurements is about 0.02 mag. Consequently, Fourier analysis was performed using Period04 (Lenz & Breger 2005). Two frequencies were detected and listed in Table 1 together with their semi-amplitudes and phases. Uncertainties are calculated by least-square fitting. Frequencies and phases D. Sinachopoulos and P. Gavras 19 Table 1: Observed frequencies for WDS 12483-6708 y-Data Id. Frequency Semi-ampl. Phase [c/d] [mag] [cycles] f1 50.6 ±0.3 0.0032 ±0.0003 0.52 ±0.01 f2 60.1 ±0.3 0.0027 ±0.0003 0.54 ±0.02 are fitted uncorrelated. The difference of 9.5 c/d between the two detected frequencies is significantly larger than the proposed frequency resolution of 1.5/dT limit by Loumos &Deeming (1978), which in this case is 7.2 c/d. Residuals to the observations are 0.004 magnitudes. Discussion and Conclusion Despite the relatively low level of the photometric residuals, the two frequencies fitted to the data and shown in Figure 2 give rise to the need for additional observations. These should include observations of external comparison and check stars to uncover the variable component of the wide, without excluding the scenario of finding both of them pulsating. In any case, we were not able to locate any variable star previously known at these coordinates in the sky. This object is not listed in the Delta Scuti catalogue by Rodriguez et al. (2000). So, this paper reports the detection of at least one additional pulsating star in a wide double star system. Acknowledgments. 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引用次数: 0

摘要

我们在宽双星WDS 12483-6708的至少一个组成部分中发现了恒星脉动。在斯特伦格伦滤光器y中观测到的最大光度振幅约为0.02等,周期约为0.02天。该探测是基于对两个双星组成部分的5小时差分CCD光度测量。WDS 12483-6708是1835年发现的一颗宽双星。从那时起,其组成部分的相对位置已经被观察了16次。在华盛顿双星目录(WDS) (Mason & Hartkopf 2006)中列出的最后一次观测是在2000年,当时测量到的组成部分的角距为13.5角秒。该系统的主星是一颗A3III/IV型恒星。它是Hipparcos的HIC 62482靶标,V=7.58, (B−V) = 0.19,视差为10mas。副恒星为HIC 62488,星等V=8.74, (B−V) = 0.47,视差与主星基本相同。两个分量的固有运动是相同的(共同固有运动星)。这两个事实表明,这颗双星不是一对光学双星。喜巴可思目录(ESA 1997)将这两种成分标记为“重复诱发的”可变性。图1:宽双星WDS 12483-6708中脉冲的光度检测图2:WDS 12483-6708各分量的幅度差变异性,以及两个检测频率的拟合。2004年5月16日,我们在天文测量观测广角希巴谷双星(Sinachopoulos et al. 2007)的框架下观测到了这颗双星,使用的是SAAO天文台的STE4 CCD相机,连接到1m望远镜的Cassegrain焦上,使用了Stroemgren滤光片。为了提高仪器测量的精度,特别是天文测量的精度,我们对每颗双星进行了16次CCD曝光,如图1所示。我们的准在线数据缩减导致测量的双星分量的平均星等差的标准偏差出乎意料地高。由于这两颗恒星处于或接近质谱的不稳定带,我们决定花5个小时对它们进行光度监测。遗憾的是,在WDS 12483-6708附近没有其他足够亮的恒星可以作为比较星,所以我们只能测量这两个分量的星等差的可变性。我们拍摄了一系列10秒的曝光,加上CCD读出时间,每小时产生95个量级的差异。我们的测量结果如图2所示。在观测窗口内,光曲线表现出显著的变异性。我们在测量中看到的最大振幅约为0.02 mag。因此,使用Period04进行傅立叶分析(Lenz & Breger 2005)。检测到的两个频率及其半幅和相位列在表1中。不确定性由最小二乘拟合计算。频率和相位D. Sinachopoulos和P. Gavras 19表1:WDS 12483-6708观测频率Semi-ampl频率。相位[c/d] [mag] [cycles] f1为50.6±0.3 0.0032±0.0003 0.52±0.01 f2为60.1±0.3 0.0027±0.0003 0.54±0.02,拟合不相关。两个检测频率之间9.5 c/d的差异明显大于Loumos &Deeming(1978)提出的1.5/dT的频率分辨率限制,在这种情况下为7.2 c/d。观测值的残差为0.004个量级。尽管光度残差的水平相对较低,但这两个频率与数据相拟合,如图2所示,因此需要进行额外的观测。这应该包括对外部比较和检查恒星的观察,以发现宽的可变成分,而不排除发现它们都在脉动的情况。无论如何,我们无法在天空的这些坐标上找到任何已知的变星。这个天体没有被Rodriguez等人(2000)列入Delta Scuti星表。因此,本文报道了在一个宽双星系统中至少发现了一颗额外的脉动恒星。致谢我们要感谢SAAO慷慨的望远镜时间分配。
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Photometric detection of pulsations in the stars of the wide binary WDS 12483-6708
We detected stellar pulsations in at least one of the components of the wide double star WDS 12483-6708. The largest observed photometric amplitude, in Stroemgren filter y, is around 0.02 magnitudes with period about 0.02 days. The detection was based on five hours of differential CCD photometry of the two double star components. Individual Objects: WDS 12483-6708, HIC 62482, HIC 62488 Introduction and Observations WDS 12483-6708 is a wide double star detected in 1835. Since then, the relative positions of its components have been observed 16 times. The last observation listed in the Washington Double Star Catalogue (WDS) (Mason & Hartkopf 2006) is from the year 2000, when the angular separation of the components measured was 13.5 arcseconds. The primary of the system is a A3III/IV type star. It is the HIC 62482 target of Hipparcos with V=7.58, (B−V) = 0.19 and parallax 10mas. The secondary star is HIC 62488 with magnitude V=8.74, (B − V) = 0.47 and has practically the same parallax of the primary. The proper motions of the two components are the same (common proper motion stars). These two facts show that this double star is not an optical pair. Hipparcos catalogue (ESA 1997) flags both components for ’duplicity-induced’ variability. Figure 1: A characteristic CCD exposure of WDS 12483-6708 in Stroemgren y filter 18 Photometric detection of pulsations in the wide binary WDS 12483-6708 Figure 2: Variability of the magnitude difference of the components of WDS 12483 − 6708, together with the fit of the two detected frequencies. We observed this double star in May 16, 2004, in the frame of astrometric observations of wide Hipparcos visual double stars (Sinachopoulos et al. 2007), using the STE4 CCD camera of SAAO observatory attached to the Cassegrain focus of the 1m telescope, using the Stroemgren y filter. To improve the instrumental accuracy of our measurements, especially the astrometric ones, we obtained sixteen CCD exposures of each double star similar to the image shown in Figure 1. Our -quasion-line data reduction resulted in an unexpectedly high value of the standard deviation of measured mean magnitude difference of the double star components. Since these two stars are in or close to the instability strip of the MS, we decided to spend five hours monitoring them photometrically. To our regret, there is no other star close WDS 12483-6708 bright enough which could be used as a comparison star, so we could only measure the variability of the magnitude difference of the two components. We took a series of ten-second exposures, which together with the CCD readout time resulted in 95 magnitude differences per hour. Our measurements are shown in Figure 2. Frequency analysis The light curve shows significant variability during the observational window. The largest amplitude we see in our measurements is about 0.02 mag. Consequently, Fourier analysis was performed using Period04 (Lenz & Breger 2005). Two frequencies were detected and listed in Table 1 together with their semi-amplitudes and phases. Uncertainties are calculated by least-square fitting. Frequencies and phases D. Sinachopoulos and P. Gavras 19 Table 1: Observed frequencies for WDS 12483-6708 y-Data Id. Frequency Semi-ampl. Phase [c/d] [mag] [cycles] f1 50.6 ±0.3 0.0032 ±0.0003 0.52 ±0.01 f2 60.1 ±0.3 0.0027 ±0.0003 0.54 ±0.02 are fitted uncorrelated. The difference of 9.5 c/d between the two detected frequencies is significantly larger than the proposed frequency resolution of 1.5/dT limit by Loumos &Deeming (1978), which in this case is 7.2 c/d. Residuals to the observations are 0.004 magnitudes. Discussion and Conclusion Despite the relatively low level of the photometric residuals, the two frequencies fitted to the data and shown in Figure 2 give rise to the need for additional observations. These should include observations of external comparison and check stars to uncover the variable component of the wide, without excluding the scenario of finding both of them pulsating. In any case, we were not able to locate any variable star previously known at these coordinates in the sky. This object is not listed in the Delta Scuti catalogue by Rodriguez et al. (2000). So, this paper reports the detection of at least one additional pulsating star in a wide double star system. Acknowledgments. We would like to thank SAAO for generous telescope time allocation.
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