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Bingqiu Chen & Biwei Jiang Beijing Normal University

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1 Bingqiu Chen & Biwei Jiang Beijing Normal University
Frequency analysis of RR Lyrae stars in the LMC Bingqiu Chen & Biwei Jiang Beijing Normal University 2010.4 Department of Astronomy Beijing Normal University

2 The data & the method of analysis Variable classification Conclusion
Overview Introduction The data & the method of analysis Variable classification Conclusion Discussion

3 RR Lyrae Star RR Lyrae stars: Types : Period : 0.1 to 1 day
Amplitude in V : up to 1.5 magnitudes Spectral type : A5 to F5 Absolute visual magnitude : about +0.5 Mass : about half a solar mass Low metal abundance Z : ~ 0.01 Evolutionary stage: Away from the main sequence & burning Helium in their core. Useful tracer of galactic evolution. Obey a period-luminosity-color relation & used as distance indicators.( Like the Cepheids) Types : RRab stars, RRc stars , RRd stars, RRe stars

4 The Blazhko effect A long-term modulation of the amplitude, shape, and phase of the light and radial velocity curve. Blazhko effect period : 11 to 533 days Occurs in 1/3 RRab stars, & a few RRc stars . (The incidence is lower in LMC). A century of study: Nonradial modes triggered by resonance effects Magnetic field e.g. : Dziembowski and Mizerski (2004).

5 Data 24906 light curves from the OGLE-III Exclude 671 stars
(Soszynski et al. 2009) Exclude I <18m & Observed dots’ number <1000 671 stars

6 Method Frequency analysis based on a PDM method : f0
In the [1 5] 1/d band Fit the light curve with five harmonics of f0: Frequency analysis with the residual: f1 In the [ ] 1/d band Fit the residual with f1 …f2…f3…f4 Visual inspection of lightcurves to check

7 RR-S Singly-periodic RR Lyrae : 495 stars 73.7%
RR0: (fundamental mode): 369~74.5% RR1: (1st overtone mode) : 124~25.1% RR2: (2nd overtone mode) : 2~0.4% ID P f Θ s amp mag A 762 0.0000 0.567 18.850 0.183 5976 0.786 18.720 0.253 5990 0.746 18.894 0.231 6004 0.505 18.740 0.175 6114 0.639 18.811 0.203 6125 0.410 18.469 0.155 6147 0.677 18.813 0.215 6180 0.778 18.818 6300 0.503 18.580 0.161

8 PDM & fitting

9 Period distribution

10 Period–amplitude diagram

11 RR-01 Double modes RR Lyrae : 12 ~1.8%
There main pulsation modes are all 1st overtone (RR1-01) ID p1 f1 Θ1 s1 a1 m c1 p0 f0 Θ0 s0 a0 c0 5901 0.0000 0.194 18.828 0.100 0.157 0.076 9165 0.223 18.779 0.105 0.156 0.072 12828 0.265 18.906 0.131 0.183 0.086 13033 18.797 0.136 0.164 0.081 13231 0.236 18.671 0.111 0.125 0.055 15012 0.257 18.870 0.118 0.240 0.112 16035 0.241 18.705 0.0012 0.121 0.056 16953 0.255 18.488 0.128 0.093 0.045 17575 0.238 18.784 0.114 0.173 0.078 18546 0.261 18.891 0.219 0.103 17311 0.187 18.624 0.221 0.091 17317 0.158 18.680 0.066 0.146 0.071

12 Phased lightcurves

13 A1 to A0 ratios Wide range A0,only 1 exceeds A1

14 Petersen diagram

15 RR-BL1 RR Lyrae with 1 close frequency component:
Number : 84 stars 12.5% RR1-BL1: 18 ~ 21.4% RR0-BL1: 66 ~ 78.6% id p0 f0 Θ0 s0 a0 mag c0 p1 f1 Θ1 s1 a1 c1 6033 0.5035 0.0000 0.106 18.059 0.044 0.8118 0.0011 0.042 0.018 6872 0.1517 0.721 18.611 0.244 0.7749 0.111 0.053 7970 0.2523 0.254 18.597 0.126 0.8735 0.0202 0.049 0.021 8072 0.3274 0.320 18.950 0.122 0.8861 0.0386 0.025 8800 0.2663 0.152 17.720 0.056 0.8604 0.0147 0.024 0.011 8809 0.2794 0.556 18.738 0.193 0.8609 0.083 0.038 9161 0.3023 0.375 18.623 0.147 0.8272 0.0029 0.084 0.036 9189 0.1961 0.404 18.673 0.153 0.8623 0.0112 0.066 0.023 9239 0.4478 0.245 18.564 0.123 0.7318 0.128 0.052 9254 0.1059 0.581 18.598 0.196 0.8975 0.0742 0.013 9340 0.3000 0.260 18.709 0.8599 0.0123 0.065

16 Phased lightcurves

17 RR-BL1 Frequency difference: RR0: f1>f0  48 stars 72.7%

18 RR-BL2 RR Lyrae with 2 close symmetric frequency components: 28 4.2%
id p0 f0 a0 f1 a1 f2 a2 f1-f0 f2-f0 5348 0.258 0.036 0.035 8575 0.119 0.098 0.060 9295 0.508 0.106 0.090 10212 0.186 0.071 0.063 11476 0.102 0.094 11701 0.311 0.179 0.129 11708 0.269 0.087 0.080 12991 0.267 0.027 0.028 13088 0.405 0.073 0.045 13183 0.079 13235 0.566 0.084 0.053

19 Phased lightcurves

20 Relation of Δf & f0

21 RR-BL3+ RR Lyrae with several close components : 29 4.2%
id p0 a0 a1 a2 a3 f1-f0 f2-f0 f3-f0 7634 0.1540 0.1216 0.1065 0.0983 10248 0.4282 0.1563 0.1049 0.1053 11434 0.3987 0.1441 0.1525 0.1118 12620 0.2287 0.1071 0.0887 0.0780 12972 0.2400 0.1152 0.0934 0.1056 12994 0.5543 0.1632 0.1181 0.1091 13023 0.5032 0.1112 0.0739 0.0798 13039 0.1514 0.1000 0.0928 0.1025 13078 0.5608 0.1553 0.1208 0.0814 13095 0.1982 0.0901 0.0548 0.0493

22 RR-BL3+

23 Relation of Δf & f0

24 RR-D & RR-unknown id p0 f0 Θ0 a0 m0 p1 f1 Θ1 s1 a1 7071 0.3352 0.474 19.043 0.7996 0.0004 0.147 16756 0.4502 0.432 18.506 0.6978 0.0000 0.276 16779 0.1346 0.654 18.695 0.8967 0.0826 0.061 17512 0.2898 0.287 18.447 0.8827 0.0462 0.050 13184 0.4371 0.254 18.617 0.6163 0.137 17331 0.3886 0.257 18.669 0.7573 0.098 6 RR-D & 17 unknown type double period RR Lyrae stars id p0 f0 Θ0 a0 mag p1 f1 Θ1 s1 a1 13070 0.2849 0.371 18.598 0.8473 0.0035 0.079 13230 0.2014 0.421 18.813 0.8116 0.0003 0.070 13254 0.0933 0.269 17.491 0.8807 0.0315 0.019 15056 0.3674 0.278 18.855 0.7799 0.0000 0.097 16035 0.5724 0.241 18.705 0.8355 0.0012 0.121 16818 0.0924 0.634 18.522 0.8951 0.0539 0.046 16953 0.2587 0.255 18.488 0.6515 0.093 17317 0.6458 0.146 18.680 0.4689 0.158

25 Main pulsation modes are all 1st overtone
Conclusion Type Number Percent Notes RR-S RR0-S 369 55.0% fundamental mode RR1-S 124 18.5% 1st overtone mode RR2-S 2 0.3% 2nd overtone mode RR-01 12 1.8% Main pulsation modes are all 1st overtone RR-BL1 RR0-BL1 66 9.8% RR1-BL1 18 2.7% RR-BL2 RR0-BL2 RR1-BL2 16 2.4% RR-BL3+ RR0-BL3+ 14 2.1% RR1-BL3+ 15 2.2% RR-D 6 0.9% P1=1,2 c/d RR-unknown 17 2.5%

26 Discussion Blazhko effect occurs more frequently in RR0 than RR1.
The Blazhko period is short in RR1, while sometimes long in RR0 than in RR1. With the number of oscillating components, the numbers of the RR0-BLn and RR1-BLn stars have a trend to be the same, so the Blazhko effect depends on the mode of pulsation and the number of oscillating components. For the RR-BL1,RR-BL2, & RR-BL3+, it seems the Blazhko can lead the period to split for any number (1-4) of components, so nonradial mode of oscillation seems better explain for Blazhko effect.

27 Thank You!

28


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