2004AJ....128..858S


Query : 2004AJ....128..858S

2004AJ....128..858S - Astron. J., 128, 858-868 (2004/August-0)

The metallicity dependence of the Fourier components of RR Lyrae light curves is the Oosterhoff-Arp-Preston period ratio effect in disguise.

SANDAGE A.

Abstract (from CDS):

The correlation of particular Fourier components of the light curves of RR Lyrae variables with metallicity, discovered by Simon and later by Kovacs and his coworkers, is shown to have the same explanation as the period ratios (period shifts in logP) between RRab Lyrae variables that have the same colors, amplitudes, and light-curve shapes but different metallicities. A purpose of this paper is to demonstrate that the model that predicts the period-metallicity relations in the mediating parameters of colors, amplitudes, and light-curve shapes also explains the Simon-Kovacs et al. correlation between period, φ31, and metallicity. The proof is made by demonstrating that the combination of the first- and third-phase terms in a Fourier decomposition of RRab light curves, called φ31by Simon & Lee, varies monotonically across the RR Lyrae instability strip in the same way that amplitude, color, and rise time vary with period within the strip. The premise of the model is that if horizontal branches at the RR Lyrae strip are stacked in luminosity according to the metallicity, then there necessarily must be a logperiod shift between RR Lyrae stars with different metallicities at the same φ31 values. However, there are exceptions to the model. The two metal-rich globular clusters NGC 6388 and NGC 6441, with anomalously long periods of their RR Lyrae stars for their amplitudes, violate the period-metallicity correlations both in amplitudes and in φ31values (for NGC 6441 where φ31 data exist). The cause must be related to the anomalously bright horizontal branches in these two clusters for their metallicities. The effect of luminosity evolution away from the zero-age horizontal branch, putatively causing noise in the metallicity equation, is discussed. It is clearly seen in the amplitude-period correlations but apparently does not exist in the φ31-period correlation in the data for the globular cluster M3 analyzed by Jurcsik and coworkers and by Cacciari and Fusi Pecci, for reasons not presently understood. Clarification can be expected from study of precision photometric data of evolved RR Lyrae stars in globular clusters of different metallicity when their Fourier components are known.

Abstract Copyright: ∼

Journal keyword(s): Galaxy: Globular Clusters: General - Stars: Evolution - Stars: Horizontal-Branch - Stars: Variables: Other

Simbad objects: 53

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Number of rows : 53
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* RY Psc RR* 00 11 41.1029039544 -01 44 55.329956556   11.94 11.49     kA8hF6 91 0
2 V* SW And RR* 00 23 43.0896315888 +29 24 03.626531352 9.53 9.34 9.15     A7IIImF0 270 0
3 V* RR Cet RR* 01 32 08.1731409309 +01 20 30.230098757 9.46 9.33 9.15     A9V 237 0
4 V* SS For RR* 02 07 51.9781810872 -26 51 57.716828856   10.45 10.20     kF5hF8 119 0
5 V* RZ Cet RR* 02 28 32.4383325288 -08 21 30.111811236   11.74 11.53     kF0.5hF2.3 109 0
6 V* X Ari RR* 03 08 30.8846437148 +10 26 45.218712967 9.45 9.25 8.97     F0.5 305 0
7 V* RX Eri RR* 04 49 44.2915145832 -15 44 28.242958128 9.64 9.43 9.22     kA8.5hF6.5 196 0
8 V* RY Col RR* 05 15 07.7818581648 -41 37 41.674798776   10.59 10.45     A7 98 0
9 V* IU Car RR* 06 53 07.4637983016 -59 35 44.251372248   12.35 12.10     kA7hF4 69 0
10 V* HH Pup RR* 07 20 35.5562195569 -46 42 30.091727783   11.52 11.31 11.49   A3II/III 94 0
11 V* BB Pup RR* 08 24 22.6433041464 -19 32 31.408283544           kA5:hF2 92 0
12 V* RR Leo RR* 10 07 43.4605279536 +23 59 30.318828648 10.14 10.01 9.94     kA1.5hA9.5 198 0
13 V* WY Ant RR* 10 16 04.9461830443 -29 43 42.417855880   11.03 10.78     kA2hA6 141 0
14 V* TV Leo RR* 11 11 21.9330503352 -05 53 31.446935268     12.35     kB9.5hF0.5 90 0
15 V* W Crt RR* 11 26 29.6452105074 -17 54 51.700992767   12.07 11.70     kF0.5hF6 130 0
16 V* SU Dra RR* 11 37 56.6071282968 +67 19 47.060102316 9.52 9.37 9.27     kA2.5hA9.5 264 0
17 V* ST Leo RR* 11 38 32.6789993717 +10 33 41.735158309   11.85 11.50     kA8hF6 141 0
18 V* X Crt RR* 11 48 56.2214628480 -10 26 28.519205856   9.99 11.62     kA7hF6 92 0
19 V* SV Hya RR* 12 30 30.5031966024 -26 02 51.113236488   10.82 10.54     kA2hF5 113 0
20 V* AV Vir RR* 13 20 11.5637828400 +09 11 16.370850120   12.14 11.88     kA5.5hF1.5 95 0
21 M 3 GlC 13 42 11.62 +28 22 38.2     6.39     ~ 2593 0
22 V* RV Oct RR* 13 46 31.7442284943 -84 24 06.384454864   11.39 10.94     ~ 105 0
23 V* V499 Cen RR* 13 55 14.7680994672 -43 14 24.800295408   11.43 11.15     kA7hF6/7 90 0
24 V* UY Boo RR* 13 58 46.3367502960 +12 57 06.457864896   11.18 10.81     kA0hA8 137 0
25 V* TY Aps RR* 14 48 50.0092910856 -71 19 41.895022044   12.03 11.65     kA5hF0 74 0
26 V* VY Ser RR* 15 31 01.9269312402 +01 41 01.762136979 10.07 9.97 9.73     A5/7Ib/II 195 0
27 V* VY Lib RR* 15 51 16.9893819264 -15 45 03.344507676   11.95 12.10     kA9.5hF6 74 0
28 V* AN Ser RR* 15 53 31.0531421656 +12 57 40.112740009   11.32 10.93     kA7hA8.5 143 0
29 V* AT Ser RR* 15 55 40.3715381538 +07 59 19.597394432   11.68 11.24     kA4hF7 103 0
30 V* AV Ser RR* 16 03 41.8338584088 +00 35 56.864330880   12.01 11.54     kA6hF2 87 0
31 V* V445 Oph RR* 16 24 41.2156082791 -06 32 29.928559328   11.59 11.30     kF7.5hF6 136 0
32 V* VX Her RR* 16 30 40.8027020619 +18 22 00.573057888   10.74 11.31     kA6.5hF2.5 172 0
33 V* RW TrA RR* 17 00 46.6887966960 -66 39 49.950083772   11.96 11.95     kF0hF5 71 0
34 V* V452 Oph RR* 17 17 59.6772312552 +11 04 27.980350536     12.30     kF0hF5 57 0
35 V* ST Oph RR* 17 33 59.3723431416 -01 04 51.065996268   12.52 12.55     kA3hF0.5/kF0hF6.5 88 0
36 NGC 6388 GlC 17 36 17.461 -44 44 08.34           ~ 988 1
37 V* TY Pav RR* 17 48 42.8681186232 -62 35 59.886109248   12.81 11.85 11.28 12.069 kA5hF6 68 0
38 NGC 6441 GlC 17 50 13.06 -37 03 05.2           ~ 940 0
39 V* V455 Oph RR* 18 15 18.5275718352 +12 21 08.486845992           kA2hA7 64 0
40 V* V440 Sgr RR* 19 32 20.7825615584 -23 51 12.754574645   10.6 10.6     F0 125 0
41 V* DN Pav RR* 19 52 10.9440183936 -63 40 24.496721076     12.40     kA5hF3 55 0
42 V* V341 Aql RR* 20 32 31.5585950760 +00 35 07.048699728   11.0 10.89 10.8   kA1.5hA5.5 129 0
43 V* AA Aql RR* 20 38 15.0763128288 -02 53 25.015561872   11.96 12.14     kF3hF5 110 0
44 V* DX Del RR* 20 47 28.3555888679 +12 27 50.682410702 9.97 9.79 9.52     A7IIImF0 194 0
45 V* RV Cap RR* 21 01 28.8700813584 -15 13 46.090360344   11.11 10.97     kA1.5hA6.5 111 0
46 V* CP Aqr RR* 21 10 12.8490024720 -01 43 16.138701372   12.19 11.70     kF1.5hF7.5 70 0
47 V* SW Aqr RR* 21 15 17.8507300688 +00 04 34.870467055   11.56 11.51     kA0hA6 121 0
48 M 15 GlC 21 29 58.33 +12 10 01.2           ~ 3274 0
49 V* TZ Aqr RR* 22 01 55.5126167184 -05 36 02.527811064   12.33 11.58     kA4hA6 68 0
50 V* RW Gru RR* 22 42 06.9648685032 -44 09 12.304176876     12.44     kA5hF5 43 0
51 V* BH Peg RR* 22 53 01.0369924800 +15 47 16.609582176   10.88 10.36     kA9.5hF6.5 133 0
52 V* BO Aqr RR* 22 54 08.2705680144 -12 21 38.179952748   12.63 12.00     kA7hF1 64 0
53 V* BR Aqr RR* 23 38 32.8906588488 -09 19 07.469185188   11.38 11.31     kA6hA8 100 0

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