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List of stars in Pegasus
View on WikipediaThis is the list of notable stars in the constellation Pegasus, sorted by decreasing brightness.
| Name | B | F | G. | Var | HD | HIP | RA | Dec | vis. mag. |
abs. mag. |
Dist. (ly) | Sp. class | Notes | ||
|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|---|
| ε Peg | ε | 8 | 11 | 206778 | 107315 | 21h 44m 11.14s | +09° 52′ 30.0″ | 2.38 | −4.19 | 672 | K2Ibvar | Enif, Enf, Enir, Al Anf, Fom, Fum al Faras, Os Pegasi | |||
| β Peg | β | 53 | 217906 | 113881 | 23h 03m 46.33s | +28° 04′ 56.8″ | 2.44 | −1.49 | 199 | M2II-IIIvar | Scheat, Sheat, Seat Alpheras, Menkib | ||||
| α Peg | α | 54 | 218045 | 113963 | 23h 04m 45.62s | +15° 12′ 19.3″ | 2.49 | −0.67 | 140 | B9.5III | Markab, Marchab, Menkib al Faras, Matn al Faras | ||||
| γ Peg | γ | 88 | 886 | 1067 | 00h 13m 14.15s | +15° 11′ 01.0″ | 2.83 | −2.22 | 333 | B2IV | Algenib; β Cep variable | ||||
| η Peg | η | 44 | 215182 | 112158 | 22h 43m 00.13s | +30° 13′ 16.7″ | 2.93 | −1.16 | 215 | G2II-III.. | Matar, Sad al Matar | ||||
| ζ Peg | ζ | 42 | 214923 | 112029 | 22h 41m 27.67s | +10° 49′ 53.0″ | 3.41 | −0.62 | 208 | B8.5V | Homam, Homan, Humam, Al Hammam | ||||
| μ Peg | μ | 48 | 216131 | 112748 | 22h 50m 00.10s | +24° 36′ 06.1″ | 3.51 | 0.74 | 117 | M2III | Sadalbari, Sad al Bari, Sad al Nazi | ||||
| θ Peg | θ | 26 | 25 | 210418 | 109427 | 22h 10m 11.82s | +06° 11′ 52.0″ | 3.52 | 1.16 | 97 | A2V | Baham, Biham, Sad al Baham | |||
| ι Peg | ι | 24 | 210027 | 109176 | 22h 07m 00.47s | +25° 20′ 42.2″ | 3.77 | 3.42 | 38 | F5V | |||||
| λ Peg | λ | 47 | 215665 | 112440 | 22h 46m 31.84s | +23° 33′ 56.4″ | 3.97 | −1.45 | 395 | G8II-III | Sadalpheretz | ||||
| 1 Peg | 1 | 203504 | 105502 | 21h 22m 05.13s | +19° 48′ 15.7″ | 4.08 | 0.71 | 154 | K1III | ||||||
| κ Peg | κ | 10 | 206901 | 107354 | 21h 44m 38.70s | +25° 38′ 42.0″ | 4.14 | 1.40 | 115 | F5IV | Jih | ||||
| ξ Peg | ξ | 46 | 215648 | 112447 | 22h 46m 41.44s | +12° 10′ 26.7″ | 4.20 | 3.15 | 53 | F7V | |||||
| π Peg | π | 29 | 210459 | 109410 | 22h 09m 59.25s | +33° 10′ 41.8″ | 4.28 | −0.16 | 252 | F5III | Woo | ||||
| 9 Peg | 9 | 206859 | 107348 | 21h 44m 30.69s | +17° 21′ 00.2″ | 4.34 | −2.87 | 901 | G5Ib | ||||||
| υ Peg | υ | 68 | 220657 | 115623 | 23h 25m 22.66s | +23° 24′ 14.4″ | 4.42 | 0.79 | 173 | F8IV | Alkarab | ||||
| 2 Peg | 2 | 204724 | 106140 | 21h 29m 56.88s | +23° 38′ 19.8″ | 4.52 | −1.14 | 442 | M1III | ||||||
| 55 Peg | 55 | 42 | 218329 | 114144 | 23h 07m 00.26s | +09° 24′ 34.3″ | 4.54 | −0.43 | 322 | M2III | |||||
| 70 Peg | 70 | 221115 | 115919 | 23h 29m 09.26s | +12° 45′ 37.8″ | 4.54 | 0.86 | 178 | G8III | ||||||
| τ Peg | τ | 62 | 220061 | 115250 | 23h 20m 38.22s | +23° 44′ 25.3″ | 4.58 | 1.03 | 167 | A5V | Salm, Kerb, El Khereb, Markab; δ Sct variable | ||||
| ψ Peg | ψ | 84 | 224427 | 118131 | 23h 57m 45.55s | +25° 08′ 29.3″ | 4.63 | −0.98 | 432 | M3III | |||||
| 56 Peg | 56 | 218356 | 114155 | 23h 07m 06.74s | +25° 28′ 06.0″ | 4.76 | −1.32 | 537 | K0IIp | ||||||
| 32 Peg | 32 | 212097 | 110371 | 22h 21m 19.33s | +28° 19′ 49.9″ | 4.78 | −1.57 | 607 | B9III | ||||||
| 35 Peg | 35 | 33 | 212943 | 110882 | 22h 27m 51.48s | +04° 41′ 47.1″ | 4.78 | 1.33 | 160 | K0III | |||||
| χ Peg | χ | 89 | 1013 | 1168 | 00h 14m 36.11s | +20° 12′ 24.1″ | 4.79 | −0.21 | 326 | M2III | |||||
| ο Peg | ο | 43 | 214994 | 112051 | 22h 41m 45.41s | +29° 18′ 27.7″ | 4.80 | −0.05 | 305 | A1IV | |||||
| 31 Peg | 31 | IN | 212076 | 110386 | 22h 21m 31.07s | +12° 12′ 18.6″ | 4.82 | −2.55 | 970 | B2IV-V | IN Peg; Be star | ||||
| ν Peg | ν | 22 | 20 | 209747 | 109068 | 22h 05m 40.69s | +05° 03′ 29.8″ | 4.86 | 0.32 | 263 | K4III | ||||
| ρ Peg | ρ | 50 | 40 | 216735 | 113186 | 22h 55m 13.62s | +08° 48′ 57.9″ | 4.91 | 0.22 | 282 | A1V | ||||
| 78 Peg | 78 | 222842 | 117073 | 23h 43m 59.44s | +29° 21′ 41.6″ | 4.93 | 0.65 | 234 | K0III | ||||||
| 72 Peg | 72 | 221673 | 116310 | 23h 33m 57.15s | +31° 19′ 31.2″ | 4.97 | −1.16 | 548 | K4III | ||||||
| 57 Peg | 57 | 43 | GZ | 218634 | 114347 | 23h 09m 31.45s | +08° 40′ 37.8″ | 5.05 | −1.79 | 762 | M4Sv | GZ Peg | |||
| φ Peg | φ | 81 | 223768 | 117718 | 23h 52m 29.29s | +19° 07′ 13.3″ | 5.06 | −0.58 | 437 | M2III | |||||
| 14 Peg | 14 | 207650 | 107763 | 21h 49m 50.68s | +30° 10′ 27.4″ | 5.07 | 0.23 | 302 | A1Vs | ||||||
| 16 Peg | 16 | OQ | 208057 | 108022 | 21h 53m 03.76s | +25° 55′ 30.5″ | 5.09 | −0.89 | 512 | B3V | OQ Peg; Be star | ||||
| 66 Peg | 66 | 220363 | 115444 | 23h 23m 04.56s | +12° 18′ 50.2″ | 5.09 | 0.06 | 330 | K3III | ||||||
| 77 Peg | 77 | 48 | 222764 | 117020 | 23h 43m 22.36s | +10° 19′ 53.4″ | 5.09 | −1.91 | 817 | M2III | |||||
| 59 Peg | 59 | 45 | 218918 | 114520 | 23h 11m 44.19s | +08° 43′ 12.5″ | 5.15 | 0.70 | 253 | A5Vn | |||||
| σ Peg | σ | 49 | 39 | 216385 | 112935 | 22h 52m 23.77s | +09° 50′ 08.0″ | 5.16 | 3.02 | 88 | F7IV | ||||
| 12 Peg | 12 | 207089 | 107472 | 21h 46m 04.36s | +22° 56′ 56.0″ | 5.29 | −2.41 | 1128 | K0Ib | ||||||
| 7 Peg | 7 | 9 | 206487 | 107151 | 21h 42m 15.44s | +05° 40′ 48.5″ | 5.30 | −0.72 | 522 | M2III | |||||
| 82 Peg | 82 | HT | 223781 | 117730 | 23h 52m 37.12s | +10° 56′ 50.4″ | 5.30 | 1.49 | 188 | A4Vn | HT Peg;δ Sct variable | ||||
| 71 Peg | 71 | HW | 221615 | 116264 | 23h 33m 28.09s | +22° 29′ 55.7″ | 5.33 | −0.90 | 575 | M5IIIa | HW Peg | ||||
| 13 Peg | 13 | 6 | V373 | 207652 | 107788 | 21h 50m 08.64s | +17° 17′ 09.4″ | 5.34 | 2.72 | 109 | F2III-IV | V373 Peg | |||
| 210889 | 109654 | 22h 12m 47.81s | +34° 36′ 17.0″ | 5.34 | 0.87 | 256 | K2III | ||||||||
| 64 Peg | 64 | 220222 | 115355 | 23h 21m 54.93s | +31° 48′ 44.9″ | 5.35 | −1.69 | 834 | B6III | ||||||
| 30 Peg | 30 | 30 | 211924 | 110298 | 22h 20m 27.56s | +05° 47′ 22.2″ | 5.37 | −1.88 | 918 | B5IV | |||||
| 58 Peg | 58 | 44 | 218700 | 114389 | 23h 10m 01.47s | +09° 49′ 19.6″ | 5.39 | −1.00 | 619 | B9III | |||||
| 51 Peg | 51 | 217014 | 113357 | 22h 57m 27.85s | +20° 46′ 07.3″ | 5.45 | 4.52 | 50 | G5V | Helvetios,[1] has a planet b | |||||
| 5 Peg | 5 | 205852 | 106787 | 21h 37m 45.37s | +19° 19′ 06.9″ | 5.46 | 0.49 | 321 | F1IV | ||||||
| 75 Peg | 75 | KS | 222133 | 116611 | 23h 37m 56.77s | +18° 24′ 02.2″ | 5.49 | 1.17 | 239 | A1Vn | KS Peg; β Lyr variable | ||||
| 37 Peg | 37 | 35 | 213235 | 111062 | 22h 29m 57.95s | +04° 25′ 55.4″ | 5.51 | 1.90 | 172 | F5IVs | |||||
| 15 Peg | 15 | 207978 | 107975 | 21h 52m 29.96s | +28° 47′ 37.3″ | 5.52 | 3.31 | 90 | F6IVwvar | ||||||
| 17 Peg | 17 | 208565 | 108339 | 21h 56m 56.39s | +12° 04′ 35.5″ | 5.54 | −0.11 | 440 | A2Vnn | ||||||
| 86 Peg | 86 | 87 | 476 | 00h 05m 41.94s | +13° 23′ 46.6″ | 5.55 | 0.26 | 373 | G5III | ||||||
| 67 Peg | 67 | 220599 | 115591 | 23h 24m 50.82s | +32° 23′ 05.5″ | 5.56 | −0.40 | 506 | B9III | ||||||
| 87 Peg | 87 | 448 | 729 | 00h 09m 02.34s | +18° 12′ 43.3″ | 5.57 | 0.81 | 292 | G9III | ||||||
| 34 Vul | (34) | 203344 | 105411 | 21h 21m 04.24s | +23° 51′ 22.5″ | 5.58 | 0.91 | 280 | K1III | ||||||
| π1 Peg | π1 | 27 | 210354 | 109352 | 22h 09m 13.68s | +33° 10′ 21.0″ | 5.58 | 0.89 | 283 | G6III: | |||||
| 63 Peg | 63 | 220088 | 115271 | 23h 20m 49.50s | +30° 24′ 54.3″ | 5.58 | −0.05 | 435 | M0III | ||||||
| 36 Peg | 36 | 34 | 213119 | 110986 | 22h 29m 07.95s | +09° 07′ 44.7″ | 5.60 | −0.65 | 579 | K5III | |||||
| 20 Peg | 20 | 209166 | 108693 | 22h 01m 05.32s | +13° 07′ 11.9″ | 5.61 | 1.39 | 228 | F4III | ||||||
| 11 Peg | 11 | 12 | 207203 | 107575 | 21h 47m 13.96s | +02° 41′ 10.1″ | 5.63 | −0.15 | 467 | A1V | 27 Aquarii | ||||
| 73 Peg | 73 | 221758 | 116355 | 23h 34m 38.21s | +33° 29′ 50.2″ | 5.63 | 0.77 | 305 | K0III: | ||||||
| 38 Peg | 38 | 213323 | 111068 | 22h 30m 01.79s | +32° 34′ 21.6″ | 5.64 | 0.16 | 407 | B9.5V | ||||||
| 19 Peg | 19 | 18 | 209167 | 108699 | 22h 01m 09.24s | +08° 15′ 25.8″ | 5.65 | −0.71 | 609 | K5III | |||||
| 4 Peg | 4 | 7 | 205924 | 106856 | 21h 38m 31.87s | +05° 46′ 18.0″ | 5.66 | 2.02 | 174 | A9IV-Vn | |||||
| 218792 | 114449 | 23h 10m 42.62s | +17° 35′ 40.0″ | 5.68 | −0.27 | 505 | K4III | ||||||||
| 208108 | 108060 | 21h 53m 37.37s | +19° 40′ 06.2″ | 5.69 | 1.45 | 230 | A0Vs | ||||||||
| 23 Peg | 23 | 209833 | 109056 | 22h 05m 34.65s | +28° 57′ 50.4″ | 5.69 | 0.84 | 304 | B9Vn | ||||||
| 214850 | 111974 | 22h 40m 52.52s | +14° 32′ 55.9″ | 5.72 | 3.14 | 107 | G3V+... | ||||||||
| 210074 | 109209 | 22h 07m 28.52s | +19° 28′ 31.6″ | 5.74 | 1.81 | 199 | F2V: | ||||||||
| 209761 | 109023 | 22h 05m 11.32s | +26° 40′ 25.0″ | 5.75 | 0.32 | 397 | K2III | ||||||||
| 34 Peg | 34 | 32 | 212754 | 110785 | 22h 26m 37.22s | +04° 23′ 37.1″ | 5.76 | 2.78 | 129 | F7V | |||||
| 52 Peg | 52 | 217232 | 113503 | 22h 59m 11.80s | +11° 43′ 44.2″ | 5.76 | 1.20 | 266 | A7V | ||||||
| NZ Peg | NZ | 206043 | 106897 | 21h 39m 01.11s | +20° 15′ 55.6″ | 5.77 | 2.81 | 127 | F2V | γ Dor variable | |||||
| 80 Peg | 80 | 51 | HH | 223637 | 117628 | 23h 51m 21.25s | +09° 18′ 48.6″ | 5.77 | −1.20 | 807 | M3III | HH Peg | |||
| 207840 | 107887 | 21h 51m 34.24s | +19° 49′ 35.9″ | 5.78 | −0.49 | 584 | B8III | ||||||||
| 210502 | 109471 | 22h 10m 37.46s | +11° 37′ 28.8″ | 5.78 | −0.63 | 625 | M1III | ||||||||
| 25 Peg | 25 | 210129 | 109240 | 22h 07m 50.33s | +21° 42′ 11.1″ | 5.79 | −0.86 | 698 | B7Vn | ||||||
| 213179 | 110992 | 22h 29m 10.21s | +26° 45′ 47.6″ | 5.79 | −1.85 | 1098 | K2II | ||||||||
| 85 Peg | 85 | 224930 | 171 | 00h 02m 09.65s | +27° 05′ 04.2″ | 5.80 | 5.33 | 40 | G3V | ||||||
| 21 Peg | 21 | 209459 | 108875 | 22h 03m 19.02s | +11° 23′ 11.6″ | 5.83 | −0.27 | 541 | B9.5V | ||||||
| NV Peg | NV | 204585 | 106062 | 21h 28m 59.76s | +22° 10′ 45.9″ | 5.84 | −0.49 | 603 | M4III | ||||||
| 40 Peg | 40 | 214567 | 111810 | 22h 38m 52.62s | +19° 31′ 21.0″ | 5.84 | 0.50 | 381 | G8II | ||||||
| 219139 | 114641 | 23h 13m 26.51s | +11° 03′ 54.1″ | 5.85 | 0.79 | 335 | G5III: | ||||||||
| IM Peg | IM | 216489 | 112997 | 22h 53m 02.28s | +16° 50′ 28.5″ | 5.86 | 0.93 | 316 | K1III SB | RS CVn variable | |||||
| 211006 | 109730 | 22h 13m 38.65s | +28° 36′ 28.9″ | 5.87 | 1.45 | 249 | K2III | ||||||||
| 214995 | 112067 | 22h 41m 57.40s | +14° 30′ 59.2″ | 5.92 | 1.36 | 267 | K0III: | ||||||||
| HD 210702 | 210702 | 109577 | 22h 11m 51.33s | +16° 02′ 26.1″ | 5.93 | 2.19 | 182 | K1III | has a planet (b) | ||||||
| 79 Peg | 79 | 223461 | 117500 | 23h 49m 39.35s | +28° 50′ 32.4″ | 5.95 | 1.39 | 267 | A2m | ||||||
| HN Peg | HN | 206860 | 107350 | 21h 44m 31.19s | +14° 46′ 20.0″ | 5.96 | 4.64 | 60 | G0V | BY Draconis variable | |||||
| 210762 | 109602 | 22h 12m 08.09s | +24° 57′ 02.3″ | 5.97 | −3.88 | 3047 | K0 | ||||||||
| HR 8799 | V342 | 218396 | 114189 | 23h 07m 28.65s | +21° 08′ 03.7″ | 5.97 | 2.96 | 130 | A5V | V342 Peg; has four planets (b, c, d & e) | |||||
| 69 Peg | 69 | HV | 220933 | 115806 | 23h 27m 40.37s | +25° 10′ 02.5″ | 5.99 | 0.73 | 367 | A0MNp... | HV Peg; α² CVn variable | ||||
| 47 G. Peg | 47 | 222377 | 116768 | 23h 39m 54.99s | +09° 40′ 38.4″ | 5.99 | 2.16 | 190 | A2m | ||||||
| 18 Peg | 18 | 17 | 209008 | 108612 | 22h 00m 07.92s | +06° 43′ 02.8″ | 6.00 | −1.58 | 1069 | B3III | |||||
| 212988 | 110873 | 22h 27m 46.22s | +31° 50′ 23.9″ | 6.00 | −1.29 | 937 | K2 | ||||||||
| 206540 | 107173 | 21h 42m 32.95s | +10° 49′ 27.6″ | 6.06 | −0.59 | 697 | B5IV | ||||||||
| IK Peg | IK | 204188 | 105860 | 21h 26m 26.61s | +19° 22′ 32.2″ | 6.08 | 2.76 | 150 | A8m | ||||||
| 210210 | 109276 | 22h 08m 17.26s | +25° 32′ 37.0″ | 6.08 | 1.40 | 281 | F1IV | ||||||||
| 204862 | 106243 | 21h 31m 09.62s | +12° 08′ 15.0″ | 6.10 | 0.57 | 417 | B9.5V | ||||||||
| 221662 | 116307 | 23h 33m 55.50s | +20° 50′ 27.5″ | 6.10 | −1.42 | 1042 | M3III | ||||||||
| 214200 | 111567 | 22h 36m 07.90s | +35° 34′ 39.5″ | 6.11 | 0.57 | 417 | K0 | ||||||||
| V343 Peg | V343 | 218395 | 114187 | 23h 07m 27.74s | +32° 49′ 31.3″ | 6.13 | 0.24 | 491 | A3 | ||||||
| 23 Psc | (23) | 223755 | 117710 | 23h 52m 23.42s | +21° 40′ 16.0″ | 6.13 | 0.01 | 547 | M2III | ||||||
| 13 G. Peg | 13 | 208110 | 108090 | 21h 53m 57.72s | +06° 51′ 53.2″ | 6.14 | 0.63 | 413 | G0IIIs | ||||||
| 218235 | 114081 | 23h 06m 18.00s | +18° 31′ 03.4″ | 6.16 | 2.98 | 141 | F6Vs | ||||||||
| 206027 | 106872 | 21h 38m 45.16s | +25° 29′ 55.7″ | 6.18 | 0.65 | 416 | G9III | ||||||||
| V372 Peg | V372 | 207223 | 107558 | 21h 47m 04.70s | +17° 11′ 38.7″ | 6.18 | 2.67 | 164 | F3V | ||||||
| 210460 | 109439 | 22h 10m 18.96s | +19° 36′ 59.6″ | 6.18 | 2.46 | 181 | G0V | ||||||||
| 31 G. Peg | 31 | 211976 | 110341 | 22h 20m 55.77s | +08° 11′ 12.1″ | 6.18 | 3.67 | 104 | F6V | ||||||
| 224303 | 118048 | 23h 56m 41.52s | +22° 38′ 53.2″ | 6.18 | −0.15 | 603 | M2III | ||||||||
| 3 Peg | 3 | 6 | 205811 | 106783 | 21h 37m 43.61s | +06° 37′ 06.2″ | 6.19 | 1.71 | 257 | A2V | |||||
| 60 Peg | 60 | 218935 | 114526 | 23h 11m 49.31s | +26° 50′ 51.3″ | 6.19 | 1.84 | 242 | G8III-IV | ||||||
| 33 Peg | 33 | 212395 | 110548 | 22h 23m 39.36s | +20° 50′ 53.8″ | 6.20 | 3.55 | 111 | F7V | ||||||
| 29 G. Peg | 29 | 211287 | 109939 | 22h 15m 59.81s | +08° 32′ 58.6″ | 6.21 | 0.79 | 395 | A1Vn | ||||||
| 205541 | 106605 | 21h 35m 27.03s | +24° 27′ 07.9″ | 6.22 | −0.41 | 689 | A4V | ||||||||
| 417 | 716 | 00h 08m 52.07s | +25° 27′ 46.3″ | 6.24 | 0.69 | 419 | K0III | ||||||||
| 225276 | 399 | 00h 04m 55.93s | +26° 38′ 55.7″ | 6.25 | −0.11 | 610 | K4IIIb | ||||||||
| 1048 | 1193 | 00h 14m 55.87s | +22° 17′ 03.3″ | 6.25 | 1.06 | 355 | A1p | ||||||||
| 205539 | 106595 | 21h 35m 19.02s | +28° 11′ 51.7″ | 6.25 | 1.97 | 235 | F0IV | ||||||||
| 212670 | 110696 | 22h 25m 40.68s | +18° 26′ 39.3″ | 6.26 | 0.05 | 568 | K0 | ||||||||
| 74 Peg | 74 | 222098 | 116592 | 23h 37m 39.66s | +16° 49′ 31.8″ | 6.26 | 1.02 | 363 | A1V | ||||||
| 202128 | 104771 | 21h 13m 28.77s | +15° 58′ 56.8″ | 6.27 | 1.51 | 292 | A7Vn | ||||||||
| 207563 | 107734 | 21h 49m 26.87s | +20° 27′ 44.8″ | 6.27 | −2.49 | 1842 | B2V | ||||||||
| HO Peg | HO | 207932 | 107956 | 21h 52m 18.17s | +21° 16′ 23.2″ | 6.27 | −1.69 | 1273 | M8III | ||||||
| 45 Peg | 45 | 215510 | 112358 | 22h 45m 28.19s | +19° 21′ 59.1″ | 6.27 | 1.11 | 351 | G6III: | ||||||
| 207134 | 107502 | 21h 46m 23.84s | +25° 33′ 48.1″ | 6.28 | 0.98 | 374 | K3III: | ||||||||
| 65 Peg | 65 | 220318 | 115407 | 23h 22m 40.50s | +20° 49′ 43.5″ | 6.28 | 0.41 | 487 | B9.5V | ||||||
| 210594 | 109493 | 22h 10m 51.70s | +30° 33′ 11.0″ | 6.30 | 0.76 | 418 | A8IV | ||||||||
| 214298 | 111649 | 22h 37m 04.86s | +12° 34′ 36.8″ | 6.30 | −0.74 | 836 | K5 | ||||||||
| 76 Peg | 76 | 222683 | 116972 | 23h 42m 43.81s | +16° 20′ 08.5″ | 6.30 | 0.82 | 406 | K0 | ||||||
| OY Peg | OY | 210090 | 109212 | 22h 07m 29.95s | +18° 00′ 02.8″ | 6.31 | −1.00 | 945 | M1 | ||||||
| 219927 | 115148 | 23h 19m 27.40s | +34° 47′ 35.5″ | 6.32 | −0.33 | 697 | B8III | ||||||||
| GX Peg | GX | 213534 | 111191 | 22h 31m 34.37s | +29° 32′ 34.2″ | 6.33 | 0.85 | 408 | A5m | δ Sct variable | |||||
| 41 Peg | 41 | 214698 | 111884 | 22h 39m 47.01s | +19° 40′ 52.1″ | 6.33 | −0.12 | 635 | A2V | ||||||
| 219110 | 114607 | 23h 13m 04.01s | +29° 26′ 29.8″ | 6.34 | 0.78 | 422 | G8III | ||||||||
| 213644 | 111296 | 22h 32m 46.90s | +15° 51′ 47.6″ | 6.35 | −0.30 | 698 | K0 | ||||||||
| 208202 | 108119 | 21h 54m 17.44s | +19° 43′ 05.3″ | 6.36 | 1.12 | 364 | K0III+... | ||||||||
| 209288 | 108766 | 22h 02m 01.37s | +10° 58′ 25.7″ | 6.36 | −1.71 | 1342 | B5IIIn | ||||||||
| 209693 | 108969 | 22h 04m 34.51s | +32° 56′ 30.3″ | 6.36 | −0.99 | 962 | G5Ia | ||||||||
| 210461 | 109445 | 22h 10m 22.02s | +14° 37′ 47.7″ | 6.36 | 0.79 | 424 | K0III | ||||||||
| 214979 | 112032 | 22h 41m 31.28s | +30° 57′ 57.1″ | 6.36 | −0.67 | 832 | K5 | ||||||||
| 219310 | 114742 | 23h 14m 36.42s | +24° 06′ 10.4″ | 6.36 | 0.41 | 504 | K2III | ||||||||
| 215549 | 112368 | 22h 45m 34.64s | +30° 26′ 36.3″ | 6.37 | 2.59 | 186 | K1III-IV | ||||||||
| 209709 | 109009 | 22h 05m 03.47s | +14° 48′ 57.4″ | 6.38 | 0.41 | 509 | M2.5III: | ||||||||
| 211432 | 109977 | 22h 16m 29.66s | +27° 48′ 14.5″ | 6.38 | 0.94 | 399 | G9III | ||||||||
| 220288 | 115389 | 23h 22m 28.58s | +25° 55′ 06.6″ | 6.38 | −1.22 | 1079 | K3III | ||||||||
| 2 G. Peg | 2 | 204445 | 106021 | 21h 28m 24.83s | +08° 11′ 44.6″ | 6.39 | −0.83 | 906 | M1 | ||||||
| HD 208527 | 208527 | 108296 | 21h 56m 23.98s | +21° 14′ 23.4″ | 6.39 | −1.34 | 1148 | M1III[2] | |||||||
| HR Peg | HR | 216672 | 113131 | 22h 54m 35.62s | +16° 56′ 30.7″ | 6.39 | −0.97 | 967 | S5,1 | ||||||
| 3 G. Peg | 3 | 204603 | 106103 | 21h 29m 34.49s | +06° 34′ 53.0″ | 6.41 | −0.60 | 823 | K0 | ||||||
| 219291 | 114725 | 23h 14m 21.72s | +29° 46′ 18.7″ | 6.41 | 1.15 | 368 | F6IVw | ||||||||
| V354 Peg | V354 | 221394 | 116119 | 23h 31m 43.05s | +28° 24′ 12.7″ | 6.41 | 0.57 | 481 | A1p Sr(CrEu) | α² CVn variable | |||||
| 221493 | 116187 | 23h 32m 29.03s | +23° 50′ 37.2″ | 6.41 | −0.23 | 694 | K5 | ||||||||
| 204560 | 106064 | 21h 28m 59.92s | +17° 54′ 21.3″ | 6.42 | 0.31 | 544 | K5 | ||||||||
| 214203 | 111601 | 22h 36m 36.34s | +11° 41′ 47.8″ | 6.42 | 1.11 | 376 | A1III | ||||||||
| 224758 | 34 | 00h 00m 23.87s | +26° 55′ 05.7″ | 6.43 | 1.95 | 256 | F7.5IV-V | ||||||||
| 205011 | 106306 | 21h 31m 50.15s | +23° 50′ 42.6″ | 6.43 | 0.43 | 517 | G8Ib | ||||||||
| 206793 | 107297 | 21h 43m 58.12s | +22° 48′ 55.4″ | 6.43 | 0.16 | 585 | K2 | ||||||||
| 39 Peg | 39 | V643 | 213617 | 111278 | 22h 32m 35.38s | +20° 13′ 47.8″ | 6.43 | 2.81 | 172 | F1V | V643 Pegasi; γ Dor variable | ||||
| 41 G. Peg | 41 | 217166 | 113445 | 22h 58m 34.85s | +09° 21′ 26.0″ | 6.43 | 3.98 | 101 | G2V+... | ||||||
| 218101 | 113994 | 23h 05m 06.40s | +16° 33′ 48.1″ | 6.43 | 3.40 | 132 | G8IV | ||||||||
| 218261 | 114096 | 23h 06m 31.71s | +19° 54′ 39.0″ | 6.44 | 4.18 | 92 | F7V | ||||||||
| 221905 | 116465 | 23h 35m 55.94s | +24° 33′ 39.6″ | 6.44 | −1.49 | 1254 | M1III | ||||||||
| 205420 | 106527 | 21h 34m 33.97s | +22° 45′ 16.7″ | 6.45 | 2.25 | 226 | F7V | ||||||||
| 28 Peg | 28 | 210516 | 109458 | 22h 10m 30.18s | +20° 58′ 40.8″ | 6.45 | −0.09 | 663 | A3III | ||||||
| 221113 | 115915 | 23h 29m 05.70s | +23° 02′ 53.8″ | 6.45 | 0.44 | 520 | G9III | ||||||||
| V363 Peg | V363 | 224186 | 117986 | 23h 55m 54.63s | +15° 13′ 49.1″ | 6.45 | −0.35 | 746 | M3 | ||||||
| 209149 | 108632 | 22h 00m 26.71s | +33° 00′ 20.8″ | 6.46 | 2.35 | 217 | F5III | ||||||||
| PT Peg | PT | 212047 | 110346 | 22h 21m 00.05s | +26° 56′ 06.6″ | 6.46 | −0.47 | 793 | M4III | ||||||
| 225292 | 410 | 00h 05m 01.13s | +27° 40′ 29.3″ | 6.47 | 0.88 | 427 | G8II | ||||||||
| 434 | 728 | 00h 09m 00.16s | +28° 14′ 51.2″ | 6.47 | 1.16 | 377 | A4Vm | ||||||||
| 205422 | 106550 | 21h 34m 45.89s | +18° 19′ 44.0″ | 6.47 | −0.30 | 736 | K2 | ||||||||
| 10 G. Peg | 10 | 206689 | 107271 | 21h 43m 39.79s | +07° 31′ 43.7″ | 6.47 | 0.89 | 426 | K0 | ||||||
| 219196 | 114686 | 23h 13m 59.34s | +19° 38′ 02.1″ | 6.47 | −0.47 | 795 | K2 | ||||||||
| 213025 | 110907 | 22h 28m 11.15s | +27° 01′ 08.0″ | 6.48 | 0.63 | 482 | G8III | ||||||||
| 205603 | 106643 | 21h 36m 05.09s | +15° 04′ 56.0″ | 6.50 | 0.82 | 447 | G8II | ||||||||
| HD 208897 | 208897 | 108513 | 21h 58m 59.64s | +19° 01′ 13.4″ | 6.50 | 2.48 | 208 | K0 | has a planet (b) | ||||||
| 210890 | 109691 | 22h 13m 10.01s | +18° 16′ 47.6″ | 6.50 | −0.31 | 751 | K2 | ||||||||
| 211076 | 109788 | 22h 14m 18.45s | +17° 11′ 22.4″ | 6.50 | 1.07 | 398 | K4III | ||||||||
| 61 Peg | 61 | 219477 | 114844 | 23h 15m 46.28s | +28° 14′ 52.5″ | 6.51 | −0.83 | 956 | G5III | ||||||
| MT Peg | 217813 | 113829 | 23h 03m 04.98s | +20° 55′ 06.9″ | 6.62 | 4.65 | 79 | G1V | BY Dra variable | ||||||
| HD 220773 | 220773 | 115697 | 23h 26m 27.0s | +08° 38′ 38″ | 7.09 | 160 | F9 | has a planet (b) | |||||||
| V376 Peg | V376 | 209458 | 108859 | 22h 03m 10.77s | +18° 53′ 03.6″ | 7.65 | 4.28 | 154 | F8-G0V | has the transiting planet HD 209458 b (Osiris) | |||||
| HD 219828 | 219828 | 115100 | 23h 18m 46.73s | +18° 38′ 44.6″ | 8.02 | 3.47 | 264 | G0IV | has two planets (b & c) | ||||||
| HD 214823 | 214823 | 111928 | 22h 40m 19.9s | +31° 47′ 15″ | 8.08 | G0V | has a planet (b) | ||||||||
| HD 220197 | 220197 | 115359 | 23h 21m 58.0s | +16° 37′ 57″ | 9.00 | 210 | F8V | has a planet (b) | |||||||
| HIP 109600 | 109600 | 22h 12m 06.0s | +29° 03′ 57″ | 9.16 | 191 | G5 | has a planet (b) | ||||||||
| BD+14°4559 | 104780 | 21h 13m 35.99s | +14° 41′ 21.8″ | 9.66 | 6.17 | 163 | K2V | Solaris,[3] has a planet (b) | |||||||
| HAT-P-8 | 22h 52m 09.86s | +35° 26′ 49.6″ | 10.17 | 3.36 | 750 | has a transiting planet (b) | |||||||||
| WASP-134 | 21h 50m 17.0s | +04° 11′ 40″ | 11.3 | 636 | G4 | has two transiting planets (b and c) | |||||||||
| WASP-21 | 23h 09m 58.25s | +18° 23′ 45.9″ | 11.55 | 4.75 | 750 | G3V | Tangra,[4] has a transiting planet (b) | ||||||||
| WASP-52 | 23h 13m 59.0s | +08° 45′ 41″ | 12 | 457 | K2V | Anadolu,[5] has a transiting planet (b) | |||||||||
| WASP-60 | 23h 15m 58s | +31° 27′ 46″ | 12.18 | 1305 | G1V | Morava,[6] has a transiting planet (b) | |||||||||
| WASP-10 | 23h 15m 58s | +31° 27′ 46″ | 12.7 | 7.9 | 290 | K0V | has a transiting planet (b) | ||||||||
| WASP-102 | 22h 25m 51.4s | +15° 51′ 24″ | 12.73 | G0 | has a transiting planet (b) | ||||||||||
| WASP-114 | 21h 50m 40.0s | +10° 27′ 47″ | 12.74 | 1500 | G0 | has a transiting planet (b) | |||||||||
| WASP-59 | 23h 18m 30.0s | +24° 53′ 21″ | 13 | 408 | K5V | has a transiting planet (b) | |||||||||
| V391 Pegasi | V391 | 22h 04m 12.2s | +26° 25′ 08″ | 14.57 | 3.84 | 4561 | sdB | has a planet (b) | |||||||
Table legend:
| |||||||||||||||
See also
[edit]References
[edit]- ^ Final Results of NameExoWorlds Public Vote Released
- ^ B.-C. Lee; I. Han; M.-G. Park (2012). "Planetary companions orbiting M giants HD 208527 and HD 220074". Astronomy & Astrophysics. 549: A2. arXiv:1211.2051. Bibcode:2013A&A...549A...2L. doi:10.1051/0004-6361/201220301. S2CID 73522393.
- ^ "Poland". NameExoWorlds. Retrieved 2020-03-12.
- ^ "Bulgaria". NameExoWorlds. Retrieved 2020-03-12.
- ^ "Turkey". NameExoWorlds. Retrieved 2020-03-12.
- ^ "Serbia". NameExoWorlds. Retrieved 2020-03-12.
- ESA (1997). "The Hipparcos and Tycho Catalogues". Retrieved 2006-12-26.
- Kostjuk, N. D. (2002). "HD-DM-GC-HR-HIP-Bayer-Flamsteed Cross Index". Retrieved 2006-12-26.
- Roman, N. G. (1987). "Identification of a Constellation from a Position". Retrieved 2006-12-26.
- Gould, B. A. "Uranometria Argentina". Reprinted and updated by Pilcher, F. Archived from the original on 2012-02-27. Retrieved 2010-07-16.
- "Naming Stars". Retrieved 13 December 2017.
List of stars in Pegasus
View on GrokipediaOverview
Constellation Background
Pegasus is a large northern constellation that occupies an area of 1,121 square degrees in the sky, ranking seventh in size among the 88 modern constellations.[3] It lies in the fourth quadrant of the northern hemisphere (NQ4) and is bordered by Andromeda, Aquarius, Delphinus, Equuleus, Lacerta, Pisces, and Vulpecula.[3] The constellation's boundaries, as defined by the International Astronomical Union (IAU), follow lines of right ascension and declination established in 1930 following the IAU's General Assembly in 1928. These boundaries encompass a right ascension range from 21h 12.6m to 00h 14.6m and a declination range from +2.33° to +36.61°.[8] In Greek mythology, Pegasus represents the immortal winged horse born from the neck of the Gorgon Medusa when she was slain by Perseus; it was sired by Poseidon, the god of the sea, and later tamed by the hero Bellerophon, who rode it to defeat the Chimera.[9] Pegasus is prominently visible during autumn evenings from northern latitudes, culminating high in the sky in October for optimal observation.[10]Stellar Composition
The constellation Pegasus contains approximately 175 stars brighter than apparent magnitude 6.5, which are visible to the naked eye under favorable conditions. These stars form a diverse population in terms of luminosity, with the brightest examples reaching magnitudes near 2.4 and contributing significantly to the constellation's prominent asterisms, while fainter members cluster around the visibility limit of magnitude 6. This distribution highlights Pegasus as a rich field for amateur astronomers, offering a mix of steady and variable lights across its 1,121 square degrees.[11] The spectral composition of these stars is dominated by G-type and K-type giants among the brighter cohort, such as Matar (G2II) and Sadalbari (G8III), due to the intermediate age of the stellar population in this sector of the Orion Arm, where stars have evolved beyond the main sequence over billions of years. Hotter main-sequence stars of B and A spectral types, like Algenib (B2IV) and Markab (A0IV), are also represented, but O-type stars are notably absent, reflecting the scarcity of recent, massive star formation in the local galactic disk. This assemblage typifies Population I stars, metal-rich and born in the plane of the Milky Way, with evolved giants indicating a history of steady evolution rather than bursts of youth.[11][12] Distances to the brighter stars in Pegasus generally range from 100 to 500 light-years, as seen in examples like Homam (204 light-years) and Scheat (196 light-years), situating them within the solar neighborhood of the Orion Arm. Some extend farther, up to around 700 light-years, such as Enif at 672 light-years, which serves as a representative supergiant in the constellation's evolved population. Fainter naked-eye stars may reach distances of up to 2,000 light-years or more, though precise measurements from Gaia data confirm the overall proximity of the visible ensemble to our local galactic environment.[11]The Great Square Asterism
Component Stars
The Great Square asterism in Pegasus is formed by four prominent stars: Alpha Pegasi (Markab), Beta Pegasi (Scheat), Gamma Pegasi (Algenib), and Alpha Andromedae (Alpheratz, historically designated as Delta Pegasi). These stars outline a roughly square shape that spans approximately 15 degrees along each side, making it a distinctive feature visible to the naked eye under dark skies.[13] Alpha Pegasi, known as Markab, occupies the southeast corner of the square. It is classified as an A0IV subgiant star with an apparent visual magnitude of 2.48 and lies at a distance of about 133 light-years from Earth.[14][15][16][17] Beta Pegasi, or Scheat, marks the northwest corner. This M2.5II-III red giant exhibits irregular variability with a mean apparent magnitude of 2.42 and is located approximately 196 light-years away.[18][19][16][17] Gamma Pegasi, called Algenib, forms the southwest corner. It is a B2IV subgiant with an apparent visual magnitude of 2.84, situated at a distance of roughly 470 light-years.[20][21][16] Alpha Andromedae, or Alpheratz, lies at the northeast corner and was traditionally included in Pegasus as Delta Pegasi before modern constellation boundaries reassigned it to Andromeda. This B8IVp chemically peculiar star has an apparent visual magnitude of 2.06 and is the closest of the four at about 97 light-years.[22][23][16][17]Observational and Historical Notes
The Great Square of Pegasus serves as a key seasonal marker in the northern hemisphere, rising into the evening sky around September, near the autumnal equinox, and becoming prominently visible high overhead by October.[24] This positioning makes it an effective indicator of the shift to autumnal skies, transitioning observers from summer constellations to fall patterns.[25] Historically, the asterism was recognized in Ptolemy's Almagest in the 2nd century CE, where the constellation Pegasus was cataloged among the 48 ancient Greek figures, with the square's stars outlining the winged horse's body.[26] The Great Square has long aided in locating neighboring constellations, such as guiding observers to Andromeda via its shared star Alpheratz and to Pisces through its eastern extension.[27] In cultural lore, the asterism symbolizes the winged horse Pegasus from Greek mythology, born from the blood of Medusa and tamed by Bellerophon to defeat the Chimaera, while Babylonians viewed the four stars as IKU, a celestial field plowed by an adjacent asterism.[8] Its distinct shape has facilitated celestial navigation, serving as a reliable signpost for ancient astronomers and sailors to orient other sky features.[28] For modern observers, the Great Square's apparent span of approximately 15 degrees across the sky makes it an accessible target for amateur astronomers, often employed to star-hop to deep-sky objects like the Andromeda Galaxy.[29] However, the asterism lacks long-term alignment in proper motion, as its component stars lie at varying distances—Alpheratz at 97 light-years, Scheat at 196 light-years, Markab at 133 light-years, and Algenib at 470 light-years—causing their relative positions to gradually distort over millennia.[29][20]Bright Stars
Magnitude 2.0 to 2.5
The brightest stars in the constellation Pegasus, with apparent magnitudes ranging from 2.0 to 2.5, form key points in the celestial figure of the winged horse and are easily observable under suburban skies. These include Epsilon Pegasi (Enif), Beta Pegasi (Scheat), and Alpha Pegasi (Markab). Enif stands out as the most luminous and distant among them, representing the nose in the traditional asterism of Pegasus.[4] Epsilon Pegasi, or Enif, is classified as a K2 Ib supergiant with an apparent magnitude of 2.39 and lies approximately 690 light-years away.[30][4] It possesses a mass of about 12 solar masses and radiates with a luminosity of roughly 7,500 times that of the Sun, making it a prominent evolved star in the constellation.[4][31] Beta Pegasi, commonly called Scheat, is a red giant of spectral type M2.5 II-III, notable for spectral peculiarities including a low surface temperature of around 3,700 K and strong infrared emission relative to its visual brightness.[32][33] Its apparent magnitude fluctuates between 2.31 and 2.74 due to semi-regular variability, with details covered in the Variable Stars section.[3] The table below summarizes the primary attributes of these stars:| Bayer designation | Common name | Apparent magnitude | Spectral type | Distance (ly) | Coordinates (RA, Dec J2000) |
|---|---|---|---|---|---|
| ε Peg | Enif | 2.39 | K2 Ib | 690 | 21h 44m 11s, +09° 52' 30" |
| β Peg | Scheat | 2.42 (var. 2.31–2.74) | M2.5 II-III | 196 | 23h 03m 46s, +28° 04' 58" |
| α Peg | Markab | 2.48 | A0 IV | 133 | 23h 04m 46s, +15° 12' 19" |
Magnitude 2.5 to 4.0
The stars in Pegasus with apparent magnitudes between 2.5 and 4.0 form key elements in defining the constellation's distinctive shape, particularly contributing to the outline of the Great Square asterism and adjacent features visible to the naked eye under dark skies. These moderately bright stars include subgiants and main-sequence objects of various spectral types, ranging from hot B-type to cooler G-type, at distances from tens to hundreds of light-years. Their positions and motions provide insights into the local stellar population's dynamics. Gamma Pegasi, or Algenib, is a B2IV subgiant shining at magnitude 2.84, situated about 470 light-years distant, and also forms a corner of the Great Square; it exhibits a low projected rotational velocity of 8 km/s, atypical for B-type stars. Eta Pegasi, known as Matar, is a G8II+F0V binary system with a combined magnitude of 2.95 and a distance of roughly 196 light-years, briefly noted here for its role in extending the constellation's northern outline (detailed multiplicity in the Multiple Star Systems section). Further outlining the figure, Zeta Pegasi (Homam) is a B8.5IV subgiant of magnitude 3.41 at about 229 light-years, while Iota Pegasi, an F5V main-sequence star, appears at magnitude 3.77 and lies just 39 light-years away. The table below summarizes their key astrometric and photometric parameters.| Star Name | Apparent Magnitude (V) | Spectral Type | Distance (ly) | RA (J2000) | Dec (J2000) | Proper Motion (mas/yr, RA/Dec) |
|---|---|---|---|---|---|---|
| Gamma Pegasi (Algenib) | 2.84 | B2IV | 470 | 00h 13m 14.2s | +15° 11' 01" | +0.49 / -10.73 |
| Eta Pegasi (Matar) | 2.95 | G8II+F0V | 196 | 22h 43m 00.1s | +30° 13' 16" | +19.96 / -18.97 |
| Zeta Pegasi (Homam) | 3.41 | B8.5IV | 229 | 22h 41m 27.7s | +10° 49' 53" | +77.22 / -11.38 |
| Iota Pegasi | 3.77 | F5V | 39 | 22h 07m 00.7s | +25° 20' 42" | +295.48 / +27.44 |
Variable Stars
Semiregular and Irregular Variables
Semiregular variables in Pegasus are late-type giants or supergiants that display light curves with periods of variation interrupted by episodes of irregularity, typically resulting from non-radial pulsations and convective processes in their extended envelopes. These stars, classified under types such as SRc and SRd in the General Catalogue of Variable Stars (GCVS), show amplitudes generally less than 2 magnitudes and periods from 30 to several hundred days.[35] The variability arises primarily from convective instabilities in the outer layers of these evolved stars, where large-scale turbulent motions lead to oscillatory modes that modulate brightness without strict periodicity.[36] Beta Pegasi, commonly known as Scheat, exemplifies an SRd-type semiregular variable, an M2.5 giant with pulsation periods ranging from approximately 40 to 150 days and a visual amplitude of about 0.4 magnitudes.[37] Its light curve, as monitored by the American Association of Variable Star Observers (AAVSO), reveals semi-periodic brightenings interspersed with quieter phases, reflecting the interplay of multiple pulsation modes driven by convective turnover in its atmosphere. This variability causes Scheat's apparent magnitude to fluctuate between 2.31 and 2.74.[38]Pulsating Variables
Pulsating variables in Pegasus are stars whose brightness changes periodically due to the expansion and contraction of their outer layers, driven by instabilities in their interiors. These stars occupy specific regions in the Hertzsprung-Russell diagram, such as the instability strip for Delta Scuti types or the horizontal branch for RR Lyrae types, reflecting stages of post-main-sequence evolution where helium core burning or shell instabilities enable pulsations. In Pegasus, these variables range from hot B-type stars with short periods to cooler Population II objects, offering probes into stellar structure through asteroseismology. Observations reveal multiple modes in many cases, allowing modeling of internal density and rotation profiles. RT Pegasi exemplifies a classical Delta Scuti variable, pulsating with a primary period of 0.51 days and a magnitude variation from 9.57 to 9.75, while exhibiting multiple modes that complicate its light curve but enrich seismic analysis.[39] XX Pegasi, an RR Lyrae ab-type star of Population II origin, shows a period of 0.58 days and amplitude from 10.2 to 11.0 magnitudes, typical of horizontal branch evolution after the red giant phase where helium flashes trigger radial pulsations.[40] Such stars in Pegasus highlight the diversity of pulsation mechanisms, from high-order p-modes in Delta Scuti variables on or near the main sequence to fundamental mode pulsations in RR Lyrae stars. Delta Scuti variables like those in Pegasus are generally F-type stars (A-F spectral range) evolving through the classical instability strip, where partial helium ionization zones drive κ-mechanism pulsations with periods of hours to days and low amplitudes (up to 0.2 mag). RR Lyrae types, conversely, reside on the horizontal branch as evolved low-mass stars (~0.5-0.8 M⊙), pulsating radially with periods around 0.2-1 day and amplitudes of 0.5-2 mag, serving as standard candles due to their uniform absolute magnitudes near M_V ≈ 0.6.[41] Multi-mode pulsators among them, such as certain Delta Scuti examples, reveal non-radial oscillations (l=1,2) that map internal convection zones.[42] The following table summarizes key pulsating variables in Pegasus, focusing on brighter or well-studied examples with their primary periods, amplitude ranges, and spectral classifications (data as of 2020 unless noted):| Star Name | Type | Primary Period (days) | Magnitude Range | Spectral Type | Notes |
|---|---|---|---|---|---|
| γ Pegasi | Beta Cephei | 0.15 | 2.83–2.95 | B2 IV | Short-period, non-radial modes dominant.[3] |
| ζ Pegasi | SPB | ~1.0 | 3.41 (small amp.) | B8 V | Slowly pulsating B-star with monosinusoidal variation.[43] |
| τ Pegasi | Delta Scuti | 0.04 | ~4.58 (var. 0.1) | A5 V | Multiperiodic with periods 0.94–1.30 hours; rapid rotation.[44] |
| IK Pegasi | Delta Scuti | 0.04 | 6.10–6.25 | A0 V | Binary system; 22.9 cycles per day.[45] |
| RT Pegasi | Delta Scuti | 0.51 | 9.57–9.75 | F5 | Multiple modes; classical short-period pulsator.[39] |
| XX Pegasi | RR Lyrae ab | 0.58 | 10.2–11.0 | A | Population II; horizontal branch location.[40] |
| DY Pegasi | SX Phe | 0.07 | ~10.5 (var. 0.3) | A2-F0 | Population II subtype of Delta Scuti; short period.[46] |
| GX Pegasi | Delta Scuti | 0.18 (multi) | 10.2–10.6 | F0 | Five observed frequencies; theoretical modeling applied.[42] |
| BP Pegasi | Delta Scuti | 0.18 (double-radial) | ~10.0 (high amp.) | F2 | High-amplitude; ASAS data reveals modes.[47] |
Multiple Star Systems
Double Stars
Visual double stars in the constellation Pegasus are pairs of stars that appear close together in the sky and can be resolved with small telescopes, providing opportunities to observe orbital motion over time if they are physical binaries. These systems offer insights into stellar evolution and dynamics, with separations typically ranging from a few arcseconds to tens of arcseconds. Among the notable examples is Eta Pegasi, known as Matar, a bright giant star with a faint companion that forms a striking visual pair. The primary component, Eta Pegasi A, is a G2II bright giant with an apparent magnitude of 2.95, while the companion, Eta Pegasi B, is an F0V star with a magnitude of 8.12. The current separation between A and B is 90.4 arcseconds, making it easily resolvable even in modest instruments. The system is located at a distance of 214 light years from Earth.[50][51][52] Another example is Iota Pegasi, a visual binary system consisting of a primary F5V main-sequence star of magnitude 3.76 and a faint companion of magnitude approximately 11.4. The pair has a separation of about 123.7 arcseconds, likely an optical alignment rather than a physical binary, as no orbital motion has been confirmed. The system lies 39 light years away. Orbital data for the wide pair is not established, but the primary itself is a close spectroscopic binary with a period of 10.2 days.[53][54]| Bayer Name | Separation (arcsec) | Position Angle (°) | Magnitudes (A/B) |
|---|---|---|---|
| η Pegasi | 90.4 | 338 (2000) | 2.95 / 8.12 |
| ι Pegasi | 123.7 | 23 (2012) | 3.76 / 11.4 |
Triple and Higher-Order Systems
In the constellation Pegasus, triple and higher-order star systems are relatively rare but provide valuable insights into stellar formation and dynamical interactions. These hierarchical systems typically consist of an inner close binary orbited by a more distant companion, allowing for the study of orbital stability and evolutionary processes through combined visual, astrometric, and spectroscopic observations. One prominent example is κ Pegasi, a nearby triple system at approximately 115 light years, comprising a wide visual pair where one component is itself a close spectroscopic binary. The inner binary in κ Pegasi (components Ba and Bb) is a single-lined spectroscopic system with an orbital period of 5.9715 days and a semimajor axis of 0.087 AU, characterized by a low eccentricity of 0.0073, indicating a nearly circular orbit. The primary Ba is an F5 IV subgiant, while Bb is inferred to be a late G or early K dwarf based on mass function estimates. The outer orbit involves component A, another F5 IV subgiant, around the Ba-Bb pair, with a period of 4227 days (about 11.6 years), semimajor axis of 8.14 AU, eccentricity of 0.318, and inclination of 107.9°. The mutual inclination between the inner and outer orbits is 43.8°, which places the system near the threshold for Kozai-Lidov oscillations; these secular perturbations could induce eccentricity variations in the inner orbit, potentially influencing long-term dynamical stability without leading to ejection, as no disruptions have been observed over decades of monitoring.[56][57] Another notable triple system is DI Pegasi, an Algol-type eclipsing binary with a distant tertiary companion detected through light-time effects in the timing of primary and secondary minima. The inner binary has an orbital period of 0.7118 days (17.07 hours), with spectroscopic elements including radial velocity semi-amplitudes K₁ = 185.7 km/s for the primary and K₂ = 109.7 km/s for the secondary, yielding individual masses of approximately 1.19 M⊙ and 0.70 M⊙ assuming an edge-on orbit. The outer orbit has a period of about 54.6 years, attributed to the gravitational influence of the third component, though its separation remains uncertain at around 5 arcseconds, corresponding to approximately 1350 AU at the system's distance of about 880 light-years. This configuration highlights mass transfer in the inner pair, with the tertiary providing constraints on the system's age and evolution.[57][58] Higher-order systems in Pegasus include historical observations suggesting quadruple configurations, such as early spectroscopic analyses of κ Pegasi that identified four distinct line profiles under optimal conditions, implying an additional unresolved companion; however, modern astrometry confirms only three bound components, with the fourth likely a foreground or background interloper. Orbital eccentricities in these systems, ranging from near-zero in close pairs to moderate values like 0.318 in wider orbits, contribute to their stability by minimizing close encounters, while inclinations near 90°-125° enable detailed modeling of three-body dynamics. These systems underscore the prevalence of hierarchical architectures in stellar multiples, aiding simulations of formation via fragmentation in protostellar disks.[59]| System Name | Number of Components | Inner Period (days) | Inner Separation (AU) | Outer Period (years) | Outer Separation (arcsec / AU) |
|---|---|---|---|---|---|
| κ Pegasi | 3 | 5.97 | 0.087 | 11.6 | 0.235 / 8.14 |
| DI Pegasi | 3 | 0.712 | ~0.004 | 54.6 | ~5 / ~1350 |
Exoplanet-Hosting Stars
Pegasus hosts approximately 20 unique stars with confirmed exoplanets, encompassing over 40 planets discovered through various methods including radial velocity, transit, and direct imaging, as of November 2025.[60] This section focuses on landmark discoveries using the radial velocity and transit methods.Radial Velocity Discoveries
The radial velocity method has yielded significant exoplanet discoveries around stars in the constellation Pegasus, primarily identifying massive, short-period gas giants known as hot Jupiters through measurements of stellar Doppler shifts induced by planetary gravitational tugs. These detections rely on monitoring periodic variations in the star's radial velocity semi-amplitude , which quantifies the amplitude of the wobble and provides constraints on the planet's minimum mass (), orbital period, and eccentricity. In Pegasus, such systems highlight compact architectures where planets orbit at small semi-major axes, receiving intense stellar irradiation. One landmark discovery is 51 Pegasi b, the first exoplanet confirmed around a main-sequence star similar to the Sun, announced in 1995. Orbiting the G2V star 51 Pegasi (apparent magnitude 5.49), this hot Jupiter has an orbital period of 4.23 days, a minimum mass of (), near-zero eccentricity (), and induces a stellar radial velocity semi-amplitude of . The close-in orbit, at a semi-major axis of approximately 0.05 AU, challenged models of planetary formation and migration, suggesting dynamical processes that transport massive planets inward from wider orbits.[61] Another notable system is HD 209458, a G0V star (apparent magnitude 7.65) hosting the hot Jupiter HD 209458 b, detected via radial velocity in 1999 and nicknamed the "Osiris" planet due to its evaporating atmosphere observed later. This planet has an orbital period of 3.52 days, a minimum mass of (), low eccentricity (), and a stellar radial velocity semi-amplitude of , with a semi-major axis of 0.047 AU. The system's architecture exemplifies the hot Jupiter class, with the planet's proximity enabling detailed follow-up studies on atmospheric escape driven by stellar radiation.[62]| Star Name | Planet(s) | Discovery Year | Orbital Period (days) | Minimum Mass (, ) | Eccentricity | Radial Velocity Semi-Amplitude (m/s) |
|---|---|---|---|---|---|---|
| 51 Pegasi | 51 Pegasi b | 1995 | 4.23 | 0.46 | 0.01 | 55.9 |
| HD 209458 | HD 209458 b | 1999 | 3.52 | 0.63 | <0.008 | 84 |
Transit Method Discoveries
The transit method has revealed several exoplanets orbiting stars in the constellation Pegasus by detecting periodic dips in stellar brightness caused by planetary transits. This photometric approach allows direct measurement of planetary radii and inclinations, complementing radial velocity data for mass determinations. Among these, HD 209458 b stands out as the first exoplanet confirmed via transit observations, orbiting the G0V star HD 209458 at a distance of approximately 157 light-years. HD 209458 b, a hot Jupiter with a radius of 1.38 Jupiter radii (R_J) and an orbital period of 3.524 days, was initially detected by radial velocity in 1999 but confirmed as transiting in 2000 through ground-based photometry showing a 1.5% depth in the star's light curve and an inclination of nearly 87 degrees. The planet's close-in orbit results in extreme temperatures exceeding 1,000 K, making it a benchmark for studying inflated gas giants. Transmission spectroscopy of its transit has provided key insights into its atmosphere, including the first detection of sodium absorption lines in 2002, indicating a hazy upper atmosphere with scattered stellar light. Further observations revealed an extended hydrogen envelope escaping the planet due to intense stellar irradiation, observed via Lyman-alpha absorption during transits, suggesting significant atmospheric mass loss over the planet's lifetime. Later studies using Hubble Space Telescope data confirmed the presence of silicate clouds and hazes, contributing to the planet's low albedo and influencing its transmission spectrum.| Host Star | Planet | Radius (R_J) | Transit Depth (%) | Inclination (degrees) | Orbital Period (days) | Discovery Year |
|---|---|---|---|---|---|---|
| HD 209458 | HD 209458 b | 1.38 | 1.48 | 86.1 | 3.524 | 2000 |
Other Notable Stars
Supergiant and Giant Stars
Supergiant and giant stars in Pegasus exemplify the late evolutionary stages of stars with initial masses ranging from about 2 to 20 solar masses, where core hydrogen exhaustion leads to shell burning and significant expansion. On the Hertzsprung-Russell diagram, these stars cluster in the cool, luminous upper-right region, distinct from the main sequence; giants (luminosity class III) form a horizontal branch for lower-mass stars undergoing helium shell burning, while supergiants (class I) occupy a more vertical extension for higher-mass counterparts, reflecting greater core contraction and higher luminosities from advanced fusion of heavier elements like helium to carbon and oxygen.[63] This placement highlights their paths toward eventual mass loss, potentially culminating in planetary nebulae for giants or core-collapse supernovae for many supergiants.[64] Prominent examples include ε Pegasi (Enif) and β Pegasi (Scheat), detailed in the Bright Stars section. For further reading on their parameters, see that section. Another notable giant is η Pegasi (Matar), a yellow giant of spectral type G2 II, with an effective temperature of about 4,930 K, radius of 68 R⊙, and bolometric luminosity around 95 L⊙, located 221 light-years away. The table below presents selected parameters for key supergiant and giant stars in Pegasus, emphasizing their scale and low surface gravities characteristic of evolved phases. Updated values reflect recent measurements as of 2025.| Star | Luminosity Class | Radius (R⊙) | log g (cgs) |
|---|---|---|---|
| ε Pegasi (Enif) | Ib | 183 | 1.01 |
| β Pegasi (Scheat) | II-III | 109 | 1.20 |
| η Pegasi (Matar) | II | 68 | 2.3 |
