Name | Con | Spectral | Abs Mag | Dist (ly) | Δ Center | X | Y | Z |
---|---|---|---|---|---|---|---|---|
HD 161710 | Pav | K1 III | 1.384 | 966.954 | 0.000 | 806.350 | -449.605 | -287.677 |
HD 158948 | Ara | G2 IV/V | 1.831 | 975.677 | 46.013 | 793.150 | -493.332 | -282.117 |
5909201518367036032 | Pav | F5 | 2.116 | 999.144 | 45.064 | 816.232 | -491.517 | -300.965 |
HD 164959 | Pav | A2 III | 2.135 | 958.583 | 52.120 | 818.672 | -400.008 | -297.914 |
HD 158818 | Ara | F2 III/IV | 2.206 | 964.478 | 31.674 | 799.109 | -470.602 | -265.096 |
5911111885461849088 | Pav | 3.219 | 949.194 | 18.523 | 794.405 | -437.733 | -279.965 | |
6634111012028289024 | Pav | 3.512 | 960.205 | 23.967 | 801.543 | -432.699 | -303.972 | |
5909900429806052352 | Ara | 3.551 | 989.388 | 45.266 | 808.477 | -494.672 | -284.010 | |
6634158909504914304 | Pav | 3.741 | 972.587 | 19.149 | 812.804 | -440.005 | -302.937 | |
5910426133804240896 | Ara | 3.835 | 944.847 | 35.504 | 781.860 | -460.125 | -264.223 | |
5909652180696227456 | Pav | 3.872 | 982.949 | 28.961 | 810.100 | -478.216 | -285.204 | |
5911307323658248448 | Pav | 3.889 | 975.621 | 13.863 | 819.087 | -448.732 | -282.275 | |
6635323017441109376 | Pav | 4.047 | 952.754 | 50.004 | 813.136 | -400.440 | -293.768 | |
6634153549385197696 | Pav | 4.181 | 959.368 | 37.809 | 805.246 | -419.297 | -310.254 | |
5911418717926746112 | Pav | 4.185 | 942.681 | 28.770 | 793.207 | -433.347 | -267.912 | |
5911558940019744384 | Pav | 4.207 | 975.207 | 20.429 | 821.055 | -436.756 | -293.676 | |
5909703750363438592 | Ara | 4.373 | 947.517 | 28.761 | 785.406 | -456.642 | -269.265 | |
5911580724094524032 | Pav | 4.551 | 963.883 | 23.347 | 813.869 | -427.598 | -289.735 | |
5909509450343557760 | Pav | 4.563 | 986.799 | 26.698 | 813.184 | -468.295 | -305.476 | |
6634930590565078144 | Pav | 4.649 | 950.268 | 28.237 | 797.339 | -424.105 | -295.794 | |
5911464450739147520 | Pav | 4.662 | 963.762 | 26.488 | 817.064 | -435.227 | -268.181 | |
6635248834764652672 | Pav | 4.89 | 942.124 | 50.081 | 800.435 | -400.344 | -294.490 |