THE TAU ASSOCIATION: A 60 MYR-OLD COEVAL GROUP AT 150 pc FROM THE SUN
Abstract
We present an analysis of the newly identified Tau Association (MUTA) of young stars at 150 pc from the Sun that is part of the large Cas-Tau structure, coeval and co-moving with the Persei cluster. This association is also located in the vicinity of the Taurus-Auriga star-forming region and the Pleiades association, although it is unrelated to them. We identify more than 500 candidate members of MUTA using Gaia DR2 data and the BANYAN tool (Gagné et al., 2018) and we determine an age of Myr for its population based on an empirical comparison of its color-magnitude diagram sequence with those of other nearby young associations. The MUTA association is related to the Theia 160 group of Kounkel & Covey (2019) and corresponds to the e Tau group of Liu et al. (2020). It is also part of the Cas-Tau group of Blaauw (1956). As part of this analysis, we introduce an iterative method based on spectral templates to perform an accurate correction of interstellar extinction of Gaia DR2 photometry, needed because of its wide photometric bandpasses. We show that the members of MUTA display an expected increased rate of stellar activity and faster rotation rates compared with older stars, and that literature measurements of the lithium equivalent width of nine G0 to K3-type members are consistent with our age determination. We show that the present-day mass function of MUTA is consistent with other known nearby young associations. We identify WD 0340+103 as a hot, massive white dwarf remnant of a B2 member that left its planetary nebula phase only 270,000 years ago, posing an independent age constraint of Myr for MUTA, consistent with our isochrone age. This relatively large collection of co-moving young stars near the Sun indicates that more work is required to unveil the full kinematic structure of the complex of young stars surrounding Persei and Cas-Tau.
1 INTRODUCTION
Young stellar associations in the Solar neighborhood ( 200 pc) are valuable laboratories to study stellar evolution and refine our age-dating methods because they contain groups of stars with many different masses that formed coevally from the same molecular cloud (e.g., Zuckerman & Song, 2004; Torres et al., 2008). Their proximity is valuable because their members appear brighter, but it also causes them to be spread over larger areas of the sky, which makes their initial identification less straightforward. Obtaining credible lists of members with low contamination by unrelated field stars is challenging and typically requires measuring the six-dimensional position and space velocity of each member. As these stars formed from a single molecular cloud, they share the same velocities typically within 2–4 km s-1, allowing us to distinguish them from most field stars.
Until recently, trigonometric distance measurements were only available for a limited set of bright stars (e.g., Perryman et al. 1997), and radial velocity measurements of stars in the Solar neighborhood were even more limited to small-scale samples (e.g., see Gontcharov, 2006; White et al., 2007). This led to the identification of co-moving and coeval massive stars that represented only the tip of the iceberg of each young association of stars in our neighborhood (Zuckerman & Song, 2004; Torres et al., 2008). Efforts have been made to identify the lower-mass population based on various methods that can assign membership probabilities with missing parts of the 6-dimensional space and velocity, including the convergent point method (Mamajek, 2005; Torres et al., 2006) and various other flavors of selection cuts in space-velocity and/or photometry (Zuckerman & Song, 2004; Kraus et al., 2014; Riedel et al., 2017; Shkolnik et al., 2017) as well as methods based on Bayesian statistics (Malo et al., 2013; Gagné et al., 2014, 2018).
The second data release of the Gaia mission (Gaia DR2 hereafter; )111 changed this landscape completely in April of 2018 by providing trigonometric distance measurements for 1.3 billion stars with an unprecedented precision, as well as radial velocities for more than 7.2 million bright stars. This allowed us to complete the 6-dimensional kinematics for a number of stars on a completely new scale, which led to a plethora of scientific discoveries that quickly unveiled the spatial and kinematic structure of the Solar neighborhood as well as the Milky Way in general. Some of these discoveries include many new associations of stars (Oh et al., 2017; Faherty et al., 2018; Gagné et al., 2018a; Kounkel & Covey, 2019; Meingast et al., 2019), a large number of new M-type members of known associations (Gagné et al., 2018c; Gagné & Faherty, 2018; Luhman, 2018; Reino et al., 2018; Zuckerman, 2019; Tang et al., 2019), as well as the discovery of tidal disruption tails around three older, nearby clusters: the Hyades (Röser et al., 2019), Praesepe (Röser & Schilbach, 2019) and Coma Ber (Tang et al., 2019).

This paper presents the discovery and characterization the MUTA association, based on an initial list of massive co-moving and coeval members that had been discovered in historical surveys but never before published. The advent of Gaia DR2 allowed us to complete this list and characterize MUTA such that it will become yet another important laboratory for the investigation of stellar evolution and the grounds for discovery of age-calibrated brown dwarfs and exoplanets. In Section 2, we present the initial list of MUTA members, which we use to build a spatial-kinematic model (Section 3) to search for additional members with the BANYAN Bayesian identification tool (Gagné et al., 2018) in Section 4. In Section 5, we present an iterative method to correct interstellar extinction in Gaia DR2 color-magnitude diagrams, required because the photometric bandpasses are wider than usual. We discuss the properties of MUTA as a whole and its individual members in Section 6, including their present-day mass function and stellar activity indicators, and a comparison with the Galactic kinematic structures recently unveiled by Kounkel & Covey (2019). We summarize and conclude this work in Section 7.
2 INITIAL SAMPLE OF MEMBERS
The existence of a distinct group of co-moving young stars in the vicinity of the Taurus-Auriga (Kenyon et al., 2008) star-forming region first appeared in a spatial distribution of Cas-Tau OB-type stars assembled by Blaauw (1956). Cas-Tau was identified by Blaauw (1956) as an extended group of co-moving stars with an expansion age of 50 Myr that seems to be on the way to being dissolved. They noted that Cas-Tau may share a common origin with an extended stream of stars around the Persei cluster (e.g., see Heckmann & Lübeck, 1958; Lodieu et al., 2019) identified by Rasmuson (1921). An over-density in the Cas-Tau stars seemed to be located at Galactic coordinates , and was recovered as part of the de Zeeuw et al. (1999) census of nearby OB associations (see their Fig. 19). This over-density overlaps with subgroup 5 of Cas-Tau defined by Blaauw (1956), with five B-type stars in common (29 Tau, 30 Tau, 35 Eri, Tau, Eri) and one additional star (40 Tau) not in common that seems to be an un related background star. Combining this list of 12 early-type stars assembled by de Zeeuw et al. (1999) to other co-moving B, A and F-type stars in the range from 170° to 205° and from 40° to 27° as well as nearby ROSAT entries (Boller et al., 2016) in the same region yielded a total set of 35 stars that appeared to be young and co-moving within 15 of the average proper motions of the de Zeeuw et al. (1999) list ( = 21.0 , = 20.5 ). Four of these 37 stars are clear outliers either in (HD 23110, TYC 657–794–2, and HD 28796) or (HIP 18778) and were excluded from our initial list. The resulting 33 stars are listed in Table 2 with their properties. We tentatively named this group Tau Association (MUTA) after one of its brightest members. We assigned initial members with MUTA identification numbers (from 1 to 30) in order of decreasing -band brightness. We assigned the same MUTA ID to binaries with separations below 15′′.
In a more recent analysis or the Gaia Data Release 1 (DR1), Oh et al. (2017) recovered about a third of the stars in Table 2 as three broken up groups of co-moving systems, which they named Groups 43 (6 matches), 52 (3 matches) and 60 (4 matches). The overlap between our initial list of MUTA members and the Oh et al. (2017) sample are shown in Figure 1, where part of the Taurus star-forming region can be seen at a similar distance from the Sun (see e.g. Wichmann et al. 2000), and the Hyades cluster (Perryman et al., 1998) also appears in the foreground. The method that Oh et al. (2017) used to identify systems of co-moving stars works directly in proper motion and parallax space, which tends to recover spatially large moving groups only as broken parts, explaining why the spatially extended MUTA was broken up in three groups, similarly to other nearby young moving groups (Faherty et al., 2018).

We cross-matched our initial list of MUTA members with Gaia DR2 data to build a color-magnitude sequence shown in Figure 2 to demonstrate they constitute massive OBA-type stars () and a well-defined sequence of later-type stars (), providing further evidence that they are coeval and young.
MUTA | Spectral | R.A. | Decl. | DistanceaaGaia DR2 distances assuming a 0.029 mas zero point (Lindegren et al., 2018). | Gaia DR2 | ||
---|---|---|---|---|---|---|---|
ID | Name | Type | (hh:mm:ss.sss) | (dd:mm:ss.ss) | (pc) | mag | Ref.bbReferences for spectral types. |
1 | Eri | B3+A3 | 04:45:30.167 | –03:15:16.97 | 16 | ||
2 | Tau | B3IV | 04:15:32.079 | +08:53:32.14 | 5 | ||
3 A | 30 Tau | B3V | 03:48:16.292 | +11:08:35.52 | 5 | ||
3 B | TYC 661–1404–1 | F5+F5 | 03:48:16.835 | +11:08:40.16 | 2 | ||
4 | 35 Eri | B5V | 04:01:32.077 | –01:32:59.02 | 5 | ||
5 | 29 Tau | B3+A7 | 03:45:40.466 | +06:02:59.78 | 4 | ||
6 | HD 28375 | B5V | 04:28:32.142 | +01:22:50.65 | 14 | ||
7 | HD 28843 | B9III | 04:32:37.573 | –03:12:34.60 | 15 | ||
8 | HD 19698 | B8V | 03:10:38.828 | +11:52:21.07 | 1 | ||
9 | HR 1307 | B8V | 04:13:34.588 | +10:12:44.52 | 13 | ||
10 | V766 Tau | B9 | 03:51:15.896 | +13:02:45.52 | 9 | ||
11 | HD 28715 | B9 | 04:31:50.463 | +05:45:51.74 | 3 | ||
12 | HD 24456 | B9.5V | 03:53:30.257 | +02:07:08.57 | 10 | ||
13 | HD 23990 | B9.5V | 03:49:46.521 | +09:24:26.60 | 6 | ||
14 | HD 23538 | A0 | 03:46:26.278 | +13:30:32.46 | 3 | ||
15 | HD 25978 | B9V | 04:07:11.204 | +12:16:05.10 | 12 | ||
16 | HD 26323 | A2V | 04:10:06.873 | +07:41:52.12 | 10 | ||
17 | HD 27687 | A3 | 04:22:24.213 | +06:31:45.14 | 3 | ||
18 | HD 28356 | A3 | 04:28:32.733 | +06:05:52.07 | 3 | ||
19 A | HD 23376 | G5 | 03:44:58.957 | +08:19:10.09 | 3 | ||
19 B | TYC 658–1007–2 | 03:44:59.048 | +08:19:13.81 | – | |||
20 | HIP 17133 | A0 | 03:40:09.988 | +13:11:55.07 | 3 | ||
21 | HD 286374 | F5 | 03:56:19.224 | +11:25:10.84 | 11 | ||
22 | PPM 119410 | F8 | 03:50:50.558 | +11:00:05.12 | 8 | ||
23 | [LH98] 108 | G5IV | 03:50:28.436 | +16:31:14.80 | 7 | ||
24 | RX J0348.5+0832 | G7 | 03:48:31.461 | +08:31:36.43 | 2 | ||
25 | TYC 80–202–1 | 04:15:51.119 | +07:07:03.76 | – | |||
26 | TYC 662–217–1 | 03:59:42.158 | +12:10:08.14 | – | |||
27 | RX J0338.3+1020 | G9 | 03:38:18.266 | +10:20:16.32 | 2 | ||
28 | TYC 664–136–1 | 03:51:39.673 | +14:47:47.84 | – | |||
29 | RX J0358.2+0932 | K3 | 03:58:12.749 | +09:32:21.97 | 2 | ||
30 A | TYC 668–737–1 | 04:21:24.386 | +08:53:54.34 | – | |||
30 B | 2MASS J04212444+0853488 | 04:21:24.473 | +08:53:48.52 | – |
Note. — See section 2 for more details.
References. — (1) Cowley et al. 1969; (2) Magazzù et al. 1997; (3) Cannon & Pickering 1993; (4) Beavers & Cook 1980; (5) Lesh 1968; (6) Abt 2008; (7) White et al. 2007; (8) Wright et al. 2003; (9) Cowley 1968; (10) Grenier et al. 1999; (11) Nesterov et al. 1995; (12) Bidelman et al. 1988; (13) Cowley 1972; (14) Molnar 1972; (15) Jaschek & Jaschek 1980; (16) van Leeuwen 2007.
MUTA | Parallax | RV | RV | |||
---|---|---|---|---|---|---|
ID | Name | () | () | (mas) | (km s-1) | Ref. |
1 | Eri | 1 | ||||
2 | Tau | 1 | ||||
3 A | 30 Tau | 1 | ||||
4 | 35 Eri | 1 | ||||
5 | 29 Tau | 3 | ||||
6 | HD 28375 | 1 | ||||
7 | HD 28843 | 6 | ||||
8 | HD 19698 | 1 | ||||
9 | HR 1307 | 6 | ||||
10 | V766 Tau | 5 | ||||
12 | HD 24456 | 1 | ||||
15 | HD 25978 | 6 | ||||
16 | HD 26323 | 1 | ||||
18 | HD 28356 | 2 | ||||
19 A | HD 23376 | 2 | ||||
20 | HIP 17133 | 2 | ||||
21 | HD 286374 | 2 | ||||
22 | PPM 119410 | 2 | ||||
23 | [LH98] 108 | 4 | ||||
24 | RX J0348.5+0832 | 2 | ||||
25 | TYC 80–202–1 | 2 | ||||
26 | TYC 662–217–1 | 2 | ||||
27 | RX J0338.3+1020 | 2 | ||||
29 | RX J0358.2+0932 | 2 | ||||
30 A | TYC 668–737–1 | 2 |
The earliest-type member in our initial list is 29 Tau (MUTA 5), a B3 V-type star (Beavers & Cook, 1980), which corresponds to a mass of 5.4 (Pecaut & Mamajek, 2013). Hohle et al. (2010) and Gullikson et al. (2016) estimated the mass of 29 Tau based on evolutionary tracks and found respective values of and , consistent with the expected mass for a B3 star. Following the evolutionary tracks of Choi et al. (2016), such a star has a main-sequence life of only 80 Myr, indicating that the MUTA association is likely younger than the Pleiades.
We note that both Tau (MUTA 2) and Ari are known eclipsing binaries (Avvakumova et al., 2013). While the first is part of our initial list of members, Ari was identified in an earlier parsing of de Zeeuw et al. (1999) but was not included because of its discrepant motion (it is separated from the other stars by 6.3 km s-1). A further analysis of their respective light curves might be useful for constraining models of stellar structure at young ages.
3 A KINEMATIC MODEL OF MUTA MEMBERS
The BANYAN tool (Gagné et al., 2018) makes it possible to identify additional stars with similar Galactic positions and space velocities compared to our initial list of MUTA members, if we provide it a 6-dimensional multivariate Gaussian model for MUTA in space. One of the main benefits of BANYAN is its ability to recover stars with only partial kinematics, often a consequence of missing radial velocity or parallax measurements. The BANYAN tool currently includes kinematic models for 29 nearby young associations, which consist of the 27 associations described in Gagné et al. (2018), as well as the recently discovered Volans-Carina (Gagné et al., 2018a) and the Argus associations (Makarov & Urban, 2000), whose census of members was recently revised by Zuckerman (2019).
We compiled literature radial velocity measurements for the stars listed in Table 2 to identify a set of 25 core members with complete kinematics (see Table 2). This list excludes any gravitationally bound companion to avoid artificially giving each system more weight in the kinematic construction of the MUTA model (consistent with the model construction method of Gagné et al. 2018). HD 28715, HD 23990, HD 23538, and HD 27687 (MUTA 11, 13, 14, and 17, respectively) currently do not have radial velocity measurements and were not included in Table 2 although they are likely part of MUTA based on their position in a color-magnitude diagram (see Figure 2) and their common proper motion and parallax compared to the other members.
The methodology described in Gagné et al. (2018; see their Section 5) was used to build a multivariate Gaussian model of the stars listed in Table 2. In summary, a 6-dimensional average vector and covariance matrix in space were built by calculating the average, variance and covariances of the 25 core members with full kinematics listed in Table 2. When calculating the averages, variances and covariances, the individual measurements were weighted proportionally to the squared inverse of their individual error bars to minimize the impact of low quality measurements. The covariance matrix is then regularized to ensure its determinant is finite and positive with a singular value decomposition step. The resulting model is shown in Figure 3.
The multivariate Gaussian model in space that was found to best represent MUTA has the following central position and covariance matrix :
both in units of pc and km s-1.
The average sky position of MUTA members is 04:01:29.54, 07:59:33.3 (°, °) with a standard deviation of 5° in both directions. The average galactic coordinates are (°, °) with a standard deviation of (°, °). The total velocity of the members averages 28.3 km s-1 with a standard deviation of 2.3 km s-1. The values we find correspond to a convergent point of °, ° in right ascension and declination (06:53:31, 29:19:30).

4 A SEARCH FOR ADDITIONAL MEMBERS
The kinematic model described in Section 3 was combined with the BANYAN tool to identify candidate members of MUTA in Gaia DR2 data. We pre-selected only Gaia DR2 entries with right ascensions in the range 10–150°, declinations in the range 20 to 40° and trigonometric distances within 300 pc of the Sun. These limits are significantly wider than the ranges of sky positions (47° to 72° and 3.5° to 16.5°, respectively) and distances (all in the range 130–220 pc) of the initial list of members. The sky positions, proper motions and parallaxes from Gaia DR2 were used to determine a membership probability, as well as the Gaia DR2 radial velocities when available. We selected only the stars with Bayesian membership probabilities above 90% and a maximum likelihood separation of less than 5 km s-1 from the core of our MUTA kinematic model in space as new candidate members. The latter criterion avoids selecting stars that would fit all BANYAN models poorly, including its model of the local Galactic neighborhood.
These selection criteria resulted in a set of 503 additional candidate members which are listed in Table 3. Their common proper motion is illustrated in Figure 4 and their positions in a Gaia DR2 color versus absolute magnitude are shown in Figure 5. Their sky positions are located in the range 37–74° and 4° to 29° in right ascension and declination, and their trigonometric distances are in the range 100–220 pc, indicating that our initial filtering of Gaia DR2 entries was likely appropriate to encompass the full distribution of MUTA members.


4.1 A Search for Co-Moving Systems
We complemented our search for MUTA members with a subsequent search for stars co-moving with any one of the 540 members and candidate members. All Gaia DR2 entries within 180′′ of each MUTA candidate were inspected to find objects co-moving within 10 and for which the proper motion difference is smaller than 5% of the measurement. For most Gaia DR2 entries, a parallax measurement is also available: in these cases, we also required the trigonometric distance of the two objects to be within 5 pc of each other222Throughout this work, we used a parallax zero-point of 0.029 mas (Lindegren et al., 2018) to convert parallaxes to trigonometric distances. We determined trigonometric distances where is the parallax with a standard error propagation, which is accurate enough for the current purposes given the nearby distances of the stars under consideration., and we set a maximum parallax difference at 5% of the parallax measurement.
This search identified 26 co-moving systems (52 components total) for which both components were already in the list of candidates, and 2 stars (2MASS J03424511+0754507 and 2MASS J02581815+2456552) not already included in our list, each seemingly co-moving with a pair of stars in our list of candidates but failing to meet our membership selection criteria (i.e., their Bayesian membership probabilities are 49% and 0% respectively). In addition to those, we identified 15 systems (21 system components) for which only one component was in our list of candidates because the other component failed to pass our membership selection criteria. All objects were added to our list of low-likelihood candidates for completion, and all co-moving systems are listed in Table 4.
MUTA | Object | R.A. | Decl. | Parallax | RV | Gaia DR2 | ||
---|---|---|---|---|---|---|---|---|
ID | Name | (hh:mm:ss.sss) | (dd:mm:ss.ss) | () | () | (mas) | (km s-1) | mag |
31 | 2MASS J02363660+2026331 | 02:36:36.648 | +20:26:32.84 | 15.289 | ||||
32 | 2MASS J02424085+2558585 | 02:42:40.905 | +25:58:58.08 | 16.090 | ||||
33 | HD 17008 | 02:44:30.027 | +28:00:53.61 | 7.909 | ||||
34 | 2MASS J02484851+1319378 | 02:48:48.553 | +13:19:37.66 | 14.077 | ||||
35 | TYC 1785–155–1 | 02:49:43.813 | +25:53:11.25 | 11.679 | ||||
36 | 2MASS J02513636+2811000 | 02:51:36.407 | +28:10:59.60 | 13.629 | ||||
37 | 2MASS J02515956+1458162 | 02:51:59.618 | +14:58:15.78 | 19.815 | ||||
38 | 2MASS J02523886+2300093 | 02:52:38.911 | +23:00:08.53 | 18.548 | ||||
39 | GSC 01230–00749 | 02:55:04.011 | +20:55:18.64 | 11.948 | ||||
40 | 2MASS J02571995+2408232 | 02:57:19.993 | +24:08:22.54 | 12.207 | ||||
41 | TYC 1790–927–1 | 02:57:43.023 | +26:32:03.61 | 11.326 | ||||
42 B | Gaia DR2 113410746049727744 | 02:58:16.476 | +24:56:42.65 | 16.776 | ||||
42 A | 2MASS J02581643+2456424 | 02:58:16.484 | +24:56:41.76 | 15.193 | ||||
43 | 2MASS J02582387+2341382 | 02:58:23.907 | +23:41:37.47 | 15.832 | ||||
44 | TYC 1786–525–1 | 02:58:43.640 | +25:53:38.92 | 10.611 | ||||
45 | 2MASS J03060696+1820259 | 03:06:06.995 | +18:20:25.43 | 19.550 | ||||
46 | 2MASS J03072480+2512266 | 03:07:24.844 | +25:12:25.96 | 14.311 | ||||
47 | 2MASS J03080089+1229304 | 03:08:00.939 | +12:29:29.89 | 15.820 | ||||
48 | HAT 258–02140 | 03:08:12.369 | +25:59:26.76 | 12.372 | ||||
49 | 2MASS J03092962+1436212 | 03:09:29.670 | +14:36:21.03 | 13.889 | ||||
50 | 2MASS J03094950+2033183 | 03:09:49.537 | +20:33:17.96 | 18.117 | ||||
51 | 2MASS J03111256+2655141 | 03:11:12.603 | +26:55:13.54 | 15.099 | ||||
52 | 2MASS J03111286+2208510 | 03:11:12.890 | +22:08:50.60 | 15.496 | ||||
53 | HAT 306–07804 | 03:12:31.219 | +17:52:45.99 | 15.091 | ||||
54 | WISEA J031350.31+152530.2 | 03:13:50.319 | +15:25:29.96 | 20.723 | ||||
55 | 2MASS J03145892+2442227 | 03:14:58.962 | +24:42:22.03 | 18.409 | ||||
56 | HAT 259–01962 | 03:16:28.094 | +24:07:40.18 | 11.905 | ||||
57 | WISEA J031644.41+203733.1 | 03:16:44.427 | +20:37:32.91 | 20.812 | ||||
58 | 2MASS J03173044+1708397 | 03:17:30.472 | +17:08:39.41 | 16.287 | ||||
59 | 2MASS J03174414+2633589 | 03:17:44.180 | +26:33:58.50 | 17.935 | ||||
60 | 2MASS J03184219+0924050 | 03:18:42.227 | +09:24:04.57 | 16.087 | ||||
61 | 2MASS J03191104+1508330 | 03:19:11.110 | +15:08:32.00 | 18.175 | ||||
62 | 2MASS J03194193+1130168 | 03:19:41.968 | +11:30:16.39 | 16.531 | ||||
63 | 2MASS J03195293+2059291 | 03:19:52.955 | +20:59:28.69 | 15.967 | ||||
64 | 2MASS J03201019+2333336 | 03:20:10.218 | +23:33:33.44 | 13.859 | ||||
65 | HD 20635 | 03:20:12.410 | +28:19:22.21 | 8.856 | ||||
66 | 2MASS J03202513+1622136 | 03:20:25.170 | +16:22:13.22 | 19.099 | ||||
67 | HAT 307–08212 | 03:21:38.153 | +18:31:27.69 | 15.190 | ||||
68 | HAT 307–05183 | 03:21:47.767 | +18:31:36.03 | 13.895 | ||||
69 | 2MASS J03215583+2140162 | 03:21:55.877 | +21:40:15.73 | 14.569 | ||||
70 | 2MASS J03223315+1715182 | 03:22:33.202 | +17:15:17.93 | 16.049 | ||||
71 | 2MASS J03223957+1420316 | 03:22:39.615 | +14:20:31.22 | 16.419 | ||||
72 | HAT 259–12052 | 03:22:54.201 | +22:12:41.40 | 15.856 | ||||
73 | 2MASS J03233089+1903574 | 03:23:30.933 | +19:03:56.97 | 16.285 | ||||
74 | 2MASS J03235482+0859547 | 03:23:54.865 | +08:59:54.52 | 16.129 | ||||
75 | 2MASS J03240542+2016260 | 03:24:05.456 | +20:16:25.53 | 17.238 | ||||
76 | 2MASS J03245387+1422189 | 03:24:53.906 | +14:22:18.48 | 18.930 | ||||
77 | 2MASS J03252139+2048507 | 03:25:21.425 | +20:48:50.36 | 20.471 | ||||
78 | 2MASS J03252961+1819289 | 03:25:29.653 | +18:19:29.07 | 18.850 | ||||
79 | 2MASS J03261339+2816284 | 03:26:13.431 | +28:16:27.98 | 15.526 | ||||
80 | 2MASS J03263469+2021019 | 03:26:34.742 | +20:21:01.57 | 18.653 | ||||
81 | TYC 1245–1095–1 | 03:27:29.236 | +22:06:51.08 | 10.523 | ||||
82 | 2MASS J03283913+1945195 | 03:28:39.166 | +19:45:19.10 | 19.382 | ||||
83 | HAT 259–04655 | 03:29:33.974 | +20:51:37.51 | 13.614 | ||||
84 | 2MASS J03293496+1200269 | 03:29:34.998 | +12:00:26.54 | 19.577 | ||||
85 | 2MASS J03294963+0919493 | 03:29:49.665 | +09:19:48.97 | 15.420 | ||||
86 | 2MASS J03300964+1419314 | 03:30:09.685 | +14:19:30.98 | 16.324 | ||||
87 | HAT 259–09674 | 03:30:10.617 | +20:19:25.25 | 14.673 | ||||
88 | 2MASS J03303685+1610599 | 03:30:36.887 | +16:10:59.58 | 15.934 | ||||
89 | 2MASS J03305533+1804535 | 03:30:55.357 | +18:04:52.97 | 18.539 | ||||
90 | 2MASS J03312734+2015412 | 03:31:27.389 | +20:15:40.71 | 15.685 | ||||
91 | HAT 259–13539 | 03:31:31.957 | +20:49:10.44 | 15.419 | ||||
92 | 2MASS J03322249+1213231 | 03:32:22.541 | +12:13:22.52 | 19.743 | ||||
93 | 2MASS J03324777+1528240 | 03:32:47.809 | +15:28:23.64 | 16.278 | ||||
94 | V1267 Tau | 03:33:11.649 | +10:35:55.67 | 11.861 | ||||
95 | HD 22073 | 03:33:46.512 | +08:17:25.71 | 8.647 | ||||
96 | 2MASS J03350134+1418016 | 03:35:01.376 | +14:18:01.14 | 13.865 | ||||
97 B | 2MASS J03350317+1431358 | 03:35:03.209 | +14:31:35.33 | 18.097 | ||||
97 A | 2MASS J03350340+1431490 | 03:35:03.438 | +14:31:48.54 | 15.369 | ||||
98 | 2MASS J03352364+1000080 | 03:35:23.679 | +10:00:07.69 | 15.040 | ||||
99 | 2MASS J03352860+0811571 | 03:35:28.641 | +08:11:56.80 | 16.491 | ||||
100 | 2MASS J03353487+1253011 | 03:35:34.911 | +12:53:00.73 | 13.788 | ||||
101 | 2MASS J03355092+1516555 | 03:35:50.949 | +15:16:55.15 | 18.294 | ||||
102 | 2MASS J03360543+1026514 | 03:36:05.464 | +10:26:51.20 | 16.632 | ||||
103 | 2MASS J03360640+1307422 | 03:36:06.439 | +13:07:41.76 | 17.180 | ||||
104 B | 2MASS J03361732+2153271 | 03:36:17.360 | +21:53:26.42 | 18.454 | ||||
104 A | 2MASS J03361762+2153391 | 03:36:17.665 | +21:53:38.50 | 10.910 | ||||
105 | 2MASS J03361892+0441323 | 03:36:18.952 | +04:41:32.11 | 15.493 | ||||
106 | 2MASS J03364987+1908056 | 03:36:49.894 | +19:08:05.23 | 16.524 | ||||
107 | 2MASS J03371337+1307315 | 03:37:13.411 | +13:07:30.93 | 14.923 | ||||
108 | 2MASS J03371793+0847343 | 03:37:17.966 | +08:47:34.12 | 16.223 | ||||
109 | 2MASS J03373508+1705162 | 03:37:35.111 | +17:05:15.93 | 13.062 | ||||
110 | 2MASS J03375097+2242056 | 03:37:51.014 | +22:42:05.05 | 16.095 | ||||
111 | 2MASS J03384902+1021482 | 03:38:49.051 | +10:21:48.07 | 15.552 | ||||
112 | 2MASS J03385230+1635406 | 03:38:52.328 | +16:35:40.21 | 15.867 | ||||
113 | 2MASS J03391042+0927570 | 03:39:10.451 | +09:27:56.71 | 12.403 | ||||
114 | HAT 259–10551 | 03:39:21.160 | +21:49:08.74 | 14.824 | ||||
115 | TYC 1235–156–1 | 03:39:39.516 | +15:29:54.47 | 11.230 | ||||
116 | 2MASS J03403696+1117333 | 03:40:36.991 | +11:17:32.97 | 13.780 | ||||
117 B | 2MASS J03405723+1308577 | 03:40:57.261 | +13:08:57.23 | 18.437 | ||||
117 A | TYC 663–362–1 | 03:40:57.781 | +13:09:03.06 | 10.493 | ||||
118 | 2MASS J03410548+0527140 | 03:41:05.509 | +05:27:13.69 | 15.051 | ||||
119 | 2MASS J03410792+0917050 | 03:41:07.955 | +09:17:04.85 | 14.698 | ||||
120 | 2MASS J03413165+0401345 | 03:41:31.685 | +04:01:34.21 | 14.011 | ||||
121 | TYC 660–135–1 | 03:41:45.000 | +10:54:27.46 | 11.362 | ||||
122 | 2MASS J03420359+1631392 | 03:42:03.617 | +16:31:38.80 | 13.901 | ||||
123 | 2MASS J03423560+0945463 | 03:42:35.636 | +09:45:45.89 | 19.257 | ||||
124 | 2MASS J03425497+1114570 | 03:42:54.990 | +11:14:57.28 | 20.158 | ||||
125 | WD 0340+103 | 03:43:14.370 | +10:29:38.14 | 16.539 | ||||
126 | 2MASS J03431821+1222515 | 03:43:18.246 | +12:22:51.12 | 19.647 | ||||
127 | 2MASS J03433413+0701547 | 03:43:34.158 | +07:01:54.39 | 17.079 | ||||
128 | 2MASS J03441167+1405312 | 03:44:11.716 | +14:05:30.58 | 18.563 | ||||
129 | 2MASS J03441728+1118090 | 03:44:17.312 | +11:18:08.70 | 17.243 | ||||
130 A | 2MASS J03442859+0716100 | 03:44:28.602 | +07:16:10.10 | 16.327 | ||||
130 B | Gaia DR2 3277686910210391424 | 03:44:28.657 | +07:16:08.46 | 16.596 | ||||
131 | 2MASS J03443022+1130035 | 03:44:30.254 | +11:30:03.21 | 13.875 | ||||
132 | 2MASS J03443526+1257315 | 03:44:35.300 | +12:57:31.25 | 16.583 | ||||
133 | 2MASS J03444292+0944150 | 03:44:42.955 | +09:44:14.73 | 14.663 | ||||
134 | 2MASS J03444719+1034332 | 03:44:47.224 | +10:34:32.89 | 20.045 | ||||
135 | 2MASS J03450918+0612030 | 03:45:09.226 | +06:12:02.81 | 16.903 | ||||
136 | 2MASS J03451333+0836589 | 03:45:13.365 | +08:36:58.56 | 17.080 | ||||
140 | TYC 658–828–1 | 03:45:52.146 | +08:32:26.87 | 11.471 | ||||
141 | 2MASS J03460026+0628092 | 03:46:00.288 | +06:28:09.02 | 18.477 | ||||
142 | 2MASS J03460029+0836331 | 03:46:00.335 | +08:36:32.86 | 16.316 | ||||
143 | 2MASS J03460544+0553074 | 03:46:05.468 | +05:53:07.16 | 16.429 | ||||
144 A | 2MASS J03463553+1317056 | 03:46:35.533 | +13:17:06.31 | 17.335 | ||||
144 B | Gaia DR2 37943944413361792 | 03:46:35.594 | +13:17:04.31 | 17.365 | ||||
145 | 2MASS J03464763+1514201 | 03:46:47.664 | +15:14:19.68 | 18.282 | ||||
146 | 2MASS J03465210+0704410 | 03:46:52.139 | +07:04:40.66 | 14.155 | ||||
147 | 2MASS J03465422+0720390 | 03:46:54.253 | +07:20:38.64 | 17.957 | ||||
148 | 2MASS J03465779+0956432 | 03:46:57.820 | +09:56:42.80 | 17.712 | ||||
149 | 2MASS J03471144+0526234 | 03:47:11.466 | +05:26:23.15 | 14.611 | ||||
150 | BD+04 589 | 03:47:13.551 | +05:26:23.49 | 9.310 | ||||
151 | 2MASS J03471736+1155459 | 03:47:17.401 | +11:55:45.34 | 19.801 | ||||
152 | 2MASS J03472334+1533235 | 03:47:23.378 | +15:33:23.17 | 16.537 | ||||
153 B | Gaia DR2 44752086050666368 | 03:47:23.645 | +18:43:18.70 | 17.855 | ||||
153 A | TYC 1252–301–1 | 03:47:23.901 | +18:43:17.68 | 11.689 | ||||
154 | 2MASS J03472375+1313154 | 03:47:23.802 | +13:13:14.89 | 20.281 | ||||
155 | 2MASS J03472378+1648282 | 03:47:23.810 | +16:48:27.82 | 16.900 | ||||
156 | 2MASS J03472404+0953136 | 03:47:24.078 | +09:53:13.26 | 18.901 | ||||
157 | BD+07 543 | 03:47:31.345 | +07:57:26.39 | 10.266 | ||||
158 | TYC 661–560–1 | 03:47:53.694 | +11:48:57.98 | 10.072 | ||||
159 | TYC 71–542–1 | 03:47:56.865 | +06:16:06.67 | 11.164 | ||||
160 | 2MASS J03481036+1608419 | 03:48:10.391 | +16:08:41.59 | 17.616 | ||||
161 | 2MASS J03484419+1213118 | 03:48:44.233 | +12:13:11.48 | 13.336 | ||||
162 | 2MASS J03485029+2002281 | 03:48:50.333 | +20:02:27.56 | 12.807 | ||||
163 | 2MASS J03485472+0727538 | 03:48:54.752 | +07:27:53.54 | 16.744 | ||||
164 | 2MASS J03492243+0242209 | 03:49:22.457 | +02:42:20.68 | 13.386 | ||||
165 | 2MASS J03492441+0049520 | 03:49:24.445 | +00:49:51.87 | 14.293 | ||||
166 | 2MASS J03492817+1958226 | 03:49:28.213 | +19:58:22.15 | 17.267 | ||||
167 | 2MASS J03493857+0640562 | 03:49:38.593 | +06:40:55.89 | 19.592 | ||||
168 | 2MASS J03494198+1035258 | 03:49:42.006 | +10:35:25.51 | 15.108 | ||||
169 | 2MASS J03495031+1440552 | 03:49:50.345 | +14:40:54.73 | 16.373 | ||||
170 | 2MASS J03500539+1204146 | 03:50:05.425 | +12:04:14.18 | 17.785 | ||||
171 | 2MASS J03501719+1129445 | 03:50:17.220 | +11:29:44.31 | 16.115 | ||||
172 | 2MASS J03502412+0602279 | 03:50:24.145 | +06:02:27.52 | 17.900 | ||||
173 | 2MASS J03502880+1356125 | 03:50:28.831 | +13:56:12.16 | 14.507 | ||||
174 | 2MASS J03503310+0855492 | 03:50:33.122 | +08:55:48.93 | 17.080 | ||||
175 | 2MASS J03504400+1148329 | 03:50:44.033 | +11:48:32.54 | 16.036 | ||||
176 | 2MASS J03505375+1042075 | 03:50:53.778 | +10:42:07.07 | 16.627 | ||||
177 B | Gaia DR2 3277369048270999936 | 03:50:56.968 | +07:30:53.92 | 20.438 | ||||
177 A | 2MASS J03505694+0730565 | 03:50:56.976 | +07:30:56.18 | 16.916 | ||||
178 | 2MASS J03510483+0910174 | 03:51:04.862 | +09:10:17.03 | 18.489 | ||||
179 | 2MASS J03510528+1431333 | 03:51:05.296 | +14:31:33.07 | 16.510 | ||||
180 | 2MASS J03510854+0829205 | 03:51:08.572 | +08:29:20.31 | 16.382 | ||||
181 | 2MASS J03510859+2007324 | 03:51:08.635 | +20:07:32.13 | 18.781 | ||||
183 | 2MASS J03514618+0553543 | 03:51:46.218 | +05:53:54.13 | 16.807 | ||||
184 | 2MASS J03514810+0850170 | 03:51:48.120 | +08:50:16.66 | 18.627 | ||||
185 | 2MASS J03520563+1545160 | 03:52:05.659 | +15:45:15.71 | 15.497 | ||||
186 | 2MASS J03521195+1936160 | 03:52:11.985 | +19:36:15.78 | 19.095 | ||||
187 | 2MASS J03523091+1225547 | 03:52:30.941 | +12:25:54.15 | 19.914 | ||||
188 B | Gaia DR2 3301507795268229248 | 03:52:40.165 | +08:30:30.19 | 17.668 | ||||
188 A | 2MASS J03524018+0830333 | 03:52:40.220 | +08:30:33.13 | 16.006 | ||||
189 | 2MASS J03524910+1423538 | 03:52:49.132 | +14:23:53.30 | 20.410 | ||||
190 | WD 0350+098 | 03:53:15.739 | +09:56:33.41 | 17.098 | ||||
191 | 2MASS J03535812+0520312 | 03:53:58.148 | +05:20:30.94 | 16.996 | ||||
192 | 2MASS J03543000+0419403 | 03:54:30.036 | +04:19:40.10 | 16.268 | ||||
193 | 2MASS J03543784+0742234 | 03:54:37.870 | +07:42:23.14 | 18.159 | ||||
194 | 2MASS J03544964+0437268 | 03:54:49.676 | +04:37:26.45 | 14.724 | ||||
195 | 2MASS J03545074+1232061 | 03:54:50.776 | +12:32:05.61 | 12.524 | ||||
196 | 2MASS J03550706+0741539 | 03:55:07.096 | +07:41:53.55 | 19.272 | ||||
197 | 2MASS J03551351+0648484 | 03:55:13.543 | +06:48:48.01 | 19.036 | ||||
198 | 2MASS J03551355+0332501 | 03:55:13.587 | +03:32:49.83 | 18.214 | ||||
199 | 2MASS J03552065+0955146 | 03:55:20.677 | +09:55:14.28 | 16.318 | ||||
200 | 2MASS J03554367+0729535 | 03:55:43.715 | +07:29:53.14 | 18.250 | ||||
201 | 2MASS J03554401+0918030 | 03:55:44.053 | +09:18:02.63 | 16.500 | ||||
202 | HD 285262 | 03:55:50.274 | +16:08:33.53 | 9.657 | ||||
203 | 2MASS J03555345+0305143 | 03:55:53.461 | +03:05:14.22 | 11.717 | ||||
204 | HD 286380 | 03:56:20.741 | +10:47:47.24 | 10.293 | ||||
205 | TYC 665–460–1 | 03:56:31.738 | +13:42:38.55 | 11.718 | ||||
206 | 2MASS J03564937+1010254 | 03:56:49.397 | +10:10:25.01 | 17.467 | ||||
207 | 2MASS J03570495+0255022 | 03:57:04.974 | +02:55:01.98 | 18.701 | ||||
208 | 2MASS J03573875+1142322 | 03:57:38.786 | +11:42:31.85 | 14.377 | ||||
209 | 2MASS J03585885+1947174 | 03:58:58.880 | +19:47:16.92 | 15.233 | ||||
210 | 2MASS J03585948+0605315 | 03:58:59.503 | +06:05:31.21 | 17.435 | ||||
211 | 2MASS J03590008+0350125 | 03:59:00.112 | +03:50:12.26 | 17.500 | ||||
212 | 2MASS J03591525+0817203 | 03:59:15.275 | +08:17:19.83 | 13.249 | ||||
213 | 2MASS J03595819+0527061 | 03:59:58.221 | +05:27:05.66 | 17.954 | ||||
214 | 2MASS J04000097+1136402 | 04:00:01.009 | +11:36:40.01 | 16.114 | ||||
215 | 2MASS J04000304+0839111 | 04:00:03.068 | +08:39:10.67 | 16.703 | ||||
216 | 2MASS J04003178+0235333 | 04:00:31.808 | +02:35:33.07 | 15.539 | ||||
217 | 2MASS J04003789+0921594 | 04:00:37.913 | +09:21:59.15 | 15.592 | ||||
218 | 2MASS J04004014+0806279 | 04:00:40.176 | +08:06:27.61 | 18.413 | ||||
219 | 2MASS J04005555+1306243 | 04:00:55.592 | +13:06:24.00 | 16.165 | ||||
220 | 2MASS J04005940+0826212 | 04:00:59.429 | +08:26:20.90 | 18.532 | ||||
221 | 2MASS J04011013+0824204 | 04:01:10.160 | +08:24:20.04 | 16.796 | ||||
222 | 2MASS J04011073+1459513 | 04:01:10.773 | +14:59:51.01 | 18.212 | ||||
223 | 2MASS J04012320+0342315 | 04:01:23.221 | +03:42:31.11 | 15.515 | ||||
224 | 2MASS J04014357+0345102 | 04:01:43.594 | +03:45:09.93 | 17.282 | ||||
225 B | 2MASS J04021257+0817410 | 04:02:12.593 | +08:17:40.67 | 17.316 | ||||
225 A | 2MASS J04021281+0817400 | 04:02:12.839 | +08:17:39.75 | 16.635 | ||||
226 | 2MASS J04024742+0946340 | 04:02:47.438 | +09:46:33.61 | 13.898 | ||||
227 | 2MASS J04032655+1218397 | 04:03:26.599 | +12:18:39.32 | 18.748 | ||||
228 | 2MASS J04033422+0617517 | 04:03:34.258 | +06:17:51.37 | 17.197 | ||||
229 | 2MASS J04035178+0709082 | 04:03:51.798 | +07:09:07.97 | 17.710 | ||||
230 | 2MASS J04041708+0924123 | 04:04:17.095 | +09:24:11.81 | 20.892 | ||||
231 A | 2MASS J04044937+0935076 | 04:04:49.382 | +09:35:07.13 | 15.410 | ||||
231 B | Gaia DR2 3301900595795159040 | 04:04:49.493 | +09:35:07.71 | 16.845 | ||||
232 | 2MASS J04045070+0956109 | 04:04:50.733 | +09:56:10.59 | 16.198 | ||||
233 | 2MASS J04050036+1000386 | 04:05:00.348 | +10:00:38.31 | 20.494 | ||||
234 | 2MASS J04051287+0710190 | 04:05:12.893 | +07:10:18.85 | 17.087 | ||||
235 | 2MASS J04052254+0615339 | 04:05:22.561 | +06:15:33.36 | 17.489 | ||||
236 B | Gaia DR2 3297969498128206208 | 04:05:40.167 | +07:22:12.08 | 20.068 | ||||
236 A | 2MASS J04054018+0722109 | 04:05:40.210 | +07:22:10.83 | 17.633 | ||||
237 | 2MASS J04054131+1715471 | 04:05:41.327 | +17:15:46.81 | 15.456 | ||||
238 | 2MASS J04061902+0845408 | 04:06:19.044 | +08:45:40.59 | 20.583 | ||||
239 | 2MASS J04064005+0856259 | 04:06:40.090 | +08:56:25.62 | 17.955 | ||||
240 | 2MASS J04064920+1000435 | 04:06:49.247 | +10:00:43.19 | 19.063 | ||||
241 | 2MASS J04070083+0607080 | 04:07:00.864 | +06:07:07.56 | 15.701 | ||||
242 | 2MASS J04072953–0115000 | 04:07:29.559 | –01:15:00.13 | 15.713 | ||||
243 | 2MASS J04074422+0959349 | 04:07:44.244 | +09:59:34.57 | 17.906 | ||||
244 | TYC 666–80–1 | 04:09:47.527 | +07:48:03.29 | 10.367 | ||||
245 | 2MASS J04100909+0216157 | 04:10:09.119 | +02:16:15.24 | 18.136 | ||||
246 | 2MASS J04104612+1040529 | 04:10:46.132 | +10:40:52.68 | 18.900 | ||||
247 | 2MASS J04110212+0822096 | 04:11:02.165 | +08:22:09.33 | 20.313 | ||||
248 | 2MASS J04112808+1143403 | 04:11:28.115 | +11:43:40.10 | 16.337 | ||||
249 | 2MASS J04114261+0534427 | 04:11:42.638 | +05:34:42.48 | 19.039 | ||||
250 | 2MASS J04114611+1508252 | 04:11:46.135 | +15:08:24.90 | 15.689 | ||||
251 | 2MASS J04121099+0248564 | 04:12:11.023 | +02:48:56.36 | 17.809 | ||||
252 | 2MASS J04121147+0638125 | 04:12:11.490 | +06:38:12.26 | 19.670 | ||||
253 | 2MASS J04121402+0543526 | 04:12:14.058 | +05:43:52.28 | 19.065 | ||||
254 | TYC 74–1393–1 | 04:12:18.449 | +00:01:31.28 | 11.151 | ||||
255 | 2MASS J04140593+0150284 | 04:14:05.959 | +01:50:28.17 | 15.828 | ||||
256 | 2MASS J04142242+1103304 | 04:14:22.433 | +11:03:29.92 | 15.203 | ||||
257 | 2MASS J04143043+0509324 | 04:14:30.466 | +05:09:31.97 | 20.586 | ||||
258 | 2MASS J04151163+0745505 | 04:15:11.657 | +07:45:50.08 | 17.161 | ||||
259 | 2MASS J04153196+0208232 | 04:15:31.984 | +02:08:23.22 | 14.735 | ||||
260 | 2MASS J04153792+0545414 | 04:15:37.957 | +05:45:41.10 | 16.185 | ||||
261 | 2MASS J04154515+1053367 | 04:15:45.165 | +10:53:36.50 | 18.902 | ||||
262 | 2MASS J04154665+0921245 | 04:15:46.680 | +09:21:24.17 | 15.906 | ||||
263 | HD 26991 | 04:16:01.464 | +00:27:13.71 | 7.334 | ||||
264 | 2MASS J04160164+0208148 | 04:16:01.666 | +02:08:14.71 | 18.332 | ||||
265 B | Gaia DR2 3254162137382331136 | 04:16:13.147 | –01:19:54.96 | 16.068 | ||||
266 | 2MASS J04161776+0807409 | 04:16:17.792 | +08:07:40.48 | 14.648 | ||||
267 | UCAC2 30946195 | 04:17:18.672 | –02:16:02.15 | 11.491 | ||||
268 | 2MASS J04172026+0831017 | 04:17:20.280 | +08:31:01.47 | 13.908 | ||||
269 | TYC 77–1284–1 | 04:17:24.077 | +03:14:44.87 | 10.509 | ||||
270 | 2MASS J04180199+0912488 | 04:18:02.016 | +09:12:48.54 | 15.983 | ||||
271 | 2MASS J04181095+0934586 | 04:18:10.980 | +09:34:58.24 | 17.228 | ||||
272 | 2MASS J04181171+0159007 | 04:18:11.727 | +01:59:00.56 | 16.180 | ||||
273 | 2MASS J04183610+0614399 | 04:18:36.121 | +06:14:39.52 | 13.615 | ||||
274 | 2MASS J04184388+1108254 | 04:18:43.885 | +11:08:25.18 | 15.866 | ||||
275 | 2MASS J04191246+0659166 | 04:19:12.488 | +06:59:16.41 | 16.876 | ||||
276 | 2MASS J04195888+0813546 | 04:19:58.900 | +08:13:54.44 | 16.740 | ||||
277 A | 2MASS J04200165+0759584 | 04:20:01.666 | +07:59:57.72 | 15.336 | ||||
277 B | Gaia DR2 3298956138016754048 | 04:20:01.719 | +07:59:58.51 | 16.289 | ||||
278 B | Gaia DR2 3254797311502540032 | 04:20:02.874 | +00:10:08.62 | 19.318 | ||||
279 | 2MASS J04201617+0959534 | 04:20:16.202 | +09:59:53.06 | 17.379 | ||||
280 A | CRTS J042024.3+001725 | 04:20:24.319 | +00:17:25.43 | 13.280 | ||||
281 | 2MASS J04205517+0649544 | 04:20:55.204 | +06:49:53.97 | 15.510 | ||||
282 | 2MASS J04210781–0111328 | 04:21:07.848 | –01:11:33.15 | 14.264 | ||||
283 | 2MASS J04212496+0613103 | 04:21:24.983 | +06:13:10.05 | 16.537 | ||||
284 | 2MASS J04213975+1111071 | 04:21:39.778 | +11:11:06.72 | 18.801 | ||||
285 | 2MASS J04215979+0447054 | 04:21:59.842 | +04:47:05.75 | 20.507 | ||||
286 | 2MASS J04220837+0847244 | 04:22:08.399 | +08:47:24.15 | 17.842 | ||||
287 | 2MASS J04221374+0945434 | 04:22:13.765 | +09:45:43.00 | 18.255 | ||||
288 | BD–03 753 | 04:22:23.528 | –02:40:04.13 | 9.741 | ||||
289 | 2MASS J04222577+0734399 | 04:22:25.798 | +07:34:39.52 | 17.076 | ||||
290 | BD+05 638 | 04:22:33.022 | +05:41:38.82 | 9.033 | ||||
291 | 2MASS J04234971–0309472 | 04:23:49.737 | –03:09:47.47 | 13.303 | ||||
292 | 2MASS J04235045+0037286 | 04:23:50.454 | +00:37:28.52 | 18.361 | ||||
293 | 2MASS J04240254–0055122 | 04:24:02.572 | –00:55:12.59 | 19.772 | ||||
294 | 2MASS J04244312+0819072 | 04:24:43.162 | +08:19:07.03 | 15.048 | ||||
295 | 2MASS J04245775+0725550 | 04:24:57.780 | +07:25:54.80 | 12.059 | ||||
296 | 2MASS J04251032+0632542 | 04:25:10.358 | +06:32:53.95 | 15.807 | ||||
297 | 2MASS J04262075+0027363 | 04:26:20.785 | +00:27:36.01 | 11.352 | ||||
298 | 2MASS J04263992+0710085 | 04:26:39.939 | +07:10:08.17 | 14.349 | ||||
299 | 2MASS J04270667+0908332 | 04:27:06.684 | +09:08:32.74 | 11.726 | ||||
300 | 2MASS J04271508+0634143 | 04:27:15.116 | +06:34:14.34 | 16.367 | ||||
301 | 2MASS J04272511+0004224 | 04:27:25.145 | +00:04:22.60 | 13.191 | ||||
302 | 2MASS J04274452–0403155 | 04:27:44.547 | –04:03:15.90 | 16.999 | ||||
303 | 2MASS J04275113+0755147 | 04:27:51.156 | +07:55:14.29 | 17.084 | ||||
304 | 2MASS J04281033+0345325 | 04:28:10.354 | +03:45:32.06 | 16.336 | ||||
305 A | BD–03 789 | 04:28:37.716 | –03:15:44.58 | 9.988 | ||||
305 B | 2MASS J04283839–0315371 | 04:28:38.423 | –03:15:37.42 | 14.304 | ||||
306 | 2MASS J04290785+0111529 | 04:29:07.865 | +01:11:52.42 | 14.623 | ||||
307 | 2MASS J04294933+0108565 | 04:29:49.346 | +01:08:56.18 | 16.631 | ||||
308 | 2MASS J04300516+0545074 | 04:30:05.173 | +05:45:07.11 | 18.810 | ||||
309 | 2MASS J04300781–0004307 | 04:30:07.834 | –00:04:31.19 | 12.606 | ||||
310 | 2MASS J04315156+0458221 | 04:31:51.590 | +04:58:21.80 | 16.708 | ||||
311 | 2MASS J04322380+0836544 | 04:32:23.819 | +08:36:54.17 | 15.013 | ||||
312 | 2MASS J04333159+0017365 | 04:33:31.610 | +00:17:36.29 | 15.762 | ||||
313 | 2MASS J04333390+0939039 | 04:33:33.919 | +09:39:03.60 | 19.055 | ||||
314 | 2MASS J04334594+0621571 | 04:33:45.976 | +06:21:56.83 | 17.598 | ||||
315 | 2MASS J04335466+0058219 | 04:33:54.685 | +00:58:21.56 | 13.321 | ||||
316 | 2MASS J04340478+0221361 | 04:34:04.800 | +02:21:35.96 | 18.168 | ||||
317 | 2MASS J04341114+0212190 | 04:34:11.143 | +02:12:18.67 | 17.255 | ||||
318 B | Gaia DR2 3279527149078835712 | 04:34:19.467 | +02:26:25.91 | 15.960 | ||||
318 A | 2MASS J04341953+0226260 | 04:34:19.560 | +02:26:25.89 | 12.150 | ||||
319 | 2MASS J04342738+0227328 | 04:34:27.421 | +02:27:32.60 | 14.651 | ||||
320 | 2MASS J04342758+0513284 | 04:34:27.592 | +05:13:28.18 | 20.103 | ||||
321 | 2MASS J04343476–0144108 | 04:34:34.776 | –01:44:11.12 | 15.958 | ||||
322 | WISEA J043452.91–005432.9 | 04:34:52.905 | –00:54:32.97 | 20.665 | ||||
323 | 2MASS J04350272+0733430 | 04:35:02.756 | +07:33:42.74 | 18.271 | ||||
324 A | HD 29182 | 04:35:53.776 | +05:06:15.36 | 8.692 | ||||
325 B | Gaia DR2 3282460371222713728 | 04:36:33.274 | +05:11:31.41 | 16.270 | ||||
325 A | 2MASS J04363330+0511304 | 04:36:33.328 | +05:11:29.84 | 14.831 | ||||
326 | 2MASS J04364894+0309231 | 04:36:48.955 | +03:09:22.90 | 18.510 | ||||
327 | 2MASS J04370987+0910564 | 04:37:09.894 | +09:10:56.04 | 18.517 | ||||
328 | 2MASS J04372578–0210117 | 04:37:25.800 | –02:10:12.12 | 16.275 | ||||
329 A | 2MASS J04372971–0051241 | 04:37:29.730 | –00:51:24.47 | 13.223 | ||||
329 B | Gaia DR2 3229491776511286016 | 04:37:29.780 | –00:51:25.66 | 16.507 | ||||
330 | 2MASS J04381823+0310336 | 04:38:18.245 | +03:10:33.35 | 15.963 | ||||
331 B | Gaia DR2 3201810884087980800 | 04:38:27.437 | –03:42:46.23 | 18.416 | ||||
332 | 2MASS J04382994+0258279 | 04:38:29.963 | +02:58:27.54 | 14.967 | ||||
333 | 2MASS J04383297+0534306 | 04:38:32.989 | +05:34:30.14 | 18.382 | ||||
334 | 2MASS J04390108+0436555 | 04:39:01.103 | +04:36:55.25 | 17.795 | ||||
335 | 2MASS J04390925+0011215 | 04:39:09.277 | +00:11:21.38 | 18.487 | ||||
336 | 2MASS J04391308–0045039 | 04:39:13.102 | –00:45:04.39 | 15.326 | ||||
337 | BD+06 731 | 04:39:15.500 | +07:01:43.92 | 9.261 | ||||
338 A | TYC 4739–1225–1 | 04:39:20.251 | –03:14:21.79 | 10.962 | ||||
339 | 2MASS J04403353+0245052 | 04:40:33.544 | +02:45:04.87 | 19.753 | ||||
340 | 2MASS J04403721+0340342 | 04:40:37.219 | +03:40:33.91 | 18.793 | ||||
341 | 2MASS J04411983+0238201 | 04:41:19.851 | +02:38:19.86 | 14.996 | ||||
342 | 2MASS J04413233–0226442 | 04:41:32.362 | –02:26:44.48 | 17.805 | ||||
343 | HD 29850 | 04:42:08.711 | –01:39:54.10 | 8.874 | ||||
344 | 2MASS J04421064–0313504 | 04:42:10.660 | –03:13:50.71 | 16.565 | ||||
345 | HD 29839 | 04:42:13.732 | +02:59:23.74 | 7.218 | ||||
346 B | 2MASS J04421451+0250336 | 04:42:14.531 | +02:50:33.42 | 17.743 | ||||
346 A | 2MASS J04421498+0250387 | 04:42:14.998 | +02:50:38.54 | 14.830 | ||||
347 | 2MASS J04421761+0410207 | 04:42:17.635 | +04:10:20.28 | 17.235 | ||||
348 | 2MASS J04421931+0255038 | 04:42:19.321 | +02:55:03.57 | 16.619 | ||||
349 | 2MASS J04423067+0305301 | 04:42:30.685 | +03:05:29.79 | 17.224 | ||||
350 | TYC 91–702–1 | 04:42:54.742 | +04:00:11.23 | 10.839 | ||||
351 | TYC 83–1232–1 | 04:43:04.063 | +00:49:47.45 | 11.189 | ||||
352 | 2MASS J04430440+0234219 | 04:43:04.418 | +02:34:21.69 | 16.110 | ||||
353 | 2MASS J04431309+0048174 | 04:43:13.116 | +00:48:17.19 | 14.479 | ||||
354 | 2MASS J04435852–0106309 | 04:43:58.538 | –01:06:31.17 | 16.474 | ||||
355 | 2MASS J04441632+0202201 | 04:44:16.349 | +02:02:19.80 | 16.092 | ||||
356 | 2MASS J04444613–0327546 | 04:44:46.150 | –03:27:54.91 | 13.114 | ||||
357 | HD 30124 | 04:45:03.984 | +05:52:17.71 | 8.421 | ||||
358 | 2MASS J04452559+0047028 | 04:45:25.612 | +00:47:02.68 | 14.895 | ||||
359 | 2MASS J04463404+0413418 | 04:46:34.055 | +04:13:41.71 | 14.095 | ||||
360 | 2MASS J04465626–0311357 | 04:46:56.284 | –03:11:36.12 | 17.308 | ||||
361 | 2MASS J04472676+0011355 | 04:47:26.782 | +00:11:35.27 | 17.629 | ||||
362 | V1831 Ori | 04:50:04.711 | +01:50:42.31 | 11.522 | ||||
363 | 2MASS J04514147+0205555 | 04:51:41.493 | +02:05:55.24 | 15.520 | ||||
364 | BD–02 1047 | 04:52:07.364 | –01:58:57.43 | 9.860 | ||||
365 | 2MASS J04523044–0110409 | 04:52:30.465 | –01:10:41.31 | 15.408 | ||||
366 | 2MASS J04524130–0135000 | 04:52:41.324 | –01:35:00.29 | 16.022 | ||||
367 | 2MASS J04530475–0127086 | 04:53:04.767 | –01:27:08.86 | 14.235 | ||||
368 | HD 31125 | 04:53:04.828 | –01:16:33.04 | 7.918 | ||||
369 | TYC 4745–475–1 | 04:53:12.066 | –03:49:10.26 | 11.383 | ||||
370 | 2MASS J04543831–0151186 | 04:54:38.330 | –01:51:18.88 | 12.986 | ||||
371 B | Gaia DR2 3228318975563766784 | 04:54:46.875 | –00:01:10.21 | 14.858 | ||||
372 A | TYC 4741–307–1 | 04:56:18.287 | –01:53:33.04 | 10.775 | ||||
376 | TYC 665–150–1 | 03:57:21.412 | +12:58:16.37 | 10.833 | ||||
2MASS J02300007+2815305 | 02:30:00.126 | +28:15:30.00 | 18.285 | |||||
2MASS J02355804+1946474 | 02:35:58.096 | +19:46:47.02 | 15.679 | |||||
2MASS J02365857+1822006 | 02:36:58.621 | +18:22:00.16 | 16.235 | |||||
Gaia DR2 127856640916806528 | 02:38:41.656 | +28:08:56.54 | 18.202 | |||||
2MASS J02514834+1542531 | 02:51:48.392 | +15:42:52.31 | 18.896 | |||||
2MASS J02564263+2122182 | 02:56:42.677 | +21:22:17.63 | 15.925 | |||||
2MASS J02571402+1329246 | 02:57:14.061 | +13:29:24.21 | 16.207 | |||||
2MASS J02591008+2830202 | 02:59:10.136 | +28:30:19.82 | 15.027 | |||||
2MASS J02592884+1417534 | 02:59:28.891 | +14:17:52.96 | 16.197 | |||||
2MASS J03001278+1151455 | 03:00:12.823 | +11:51:45.10 | 17.869 | |||||
2MASS J03022099+2253470 | 03:02:21.016 | +22:53:46.60 | 18.013 | |||||
WISEA J030230.82+240842.1 | 03:02:30.837 | +24:08:41.81 | 20.528 | |||||
2MASS J03032741+1404418 | 03:03:27.453 | +14:04:41.40 | 16.078 | |||||
2MASS J03070447+2934216 | 03:07:04.519 | +29:34:20.77 | 16.917 | |||||
2MASS J03081211+1521139 | 03:08:12.158 | +15:21:13.34 | 15.788 | |||||
2MASS J03085284+1052232 | 03:08:52.883 | +10:52:22.78 | 15.423 | |||||
2MASS J03091404+2018084 | 03:09:14.086 | +20:18:07.96 | 15.424 | |||||
Gaia DR2 59117372971786880 | 03:17:00.436 | +18:27:21.96 | 17.380 | |||||
2MASS J03175490+0420281 | 03:17:54.941 | +04:20:27.63 | 17.871 | |||||
2MASS J03192523+1845233 | 03:19:25.273 | +18:45:22.78 | 17.349 | |||||
Gaia DR2 59375998722290304 | 03:19:26.873 | +19:44:53.78 | 19.613 | |||||
2MASS J03204354+2356091 | 03:20:43.590 | +23:56:08.36 | 16.447 | |||||
Ari | 03:21:13.653 | +21:08:49.13 | 5.265 | |||||
2MASS J03212919+1604380 | 03:21:29.223 | +16:04:37.59 | 17.589 | |||||
2MASS J03213476+1654136 | 03:21:34.794 | +16:54:13.30 | 18.366 | |||||
2MASS J03215751+1601394 | 03:21:57.552 | +16:01:39.10 | 15.977 | |||||
2MASS J03230385+1709370 | 03:23:03.904 | +17:09:36.49 | 15.894 | |||||
2MASS J03244896+1020589 | 03:24:49.008 | +10:20:58.39 | 17.448 | |||||
2MASS J03245419+1555078 | 03:24:54.240 | +15:55:07.18 | 18.275 | |||||
2MASS J03250457+0728193 | 03:25:04.592 | +07:28:18.82 | 17.360 | |||||
Gaia DR2 9977797439144320 | 03:25:04.736 | +07:28:20.43 | 18.012 | |||||
2MASS J03261888+2153335 | 03:26:18.933 | +21:53:32.98 | 16.861 | |||||
2MASS J03270898+0933595 | 03:27:09.019 | +09:33:59.24 | 18.677 | |||||
2MASS J03274866+0547180 | 03:27:48.706 | +05:47:17.65 | 17.397 | |||||
2MASS J03282792+1524230 | 03:28:27.961 | +15:24:22.57 | 16.798 | |||||
2MASS J03284348+0843451 | 03:28:43.521 | +08:43:44.79 | 20.658 | |||||
2MASS J03292961+1051560 | 03:29:29.653 | +10:51:55.53 | 15.263 | |||||
2MASS J03304846+1034093 | 03:30:48.497 | +10:34:08.92 | 14.607 | |||||
2MASS J03310140+1200052 | 03:31:01.444 | +12:00:04.75 | 16.609 | |||||
2MASS J03313540+0645326 | 03:31:35.446 | +06:45:32.52 | 16.243 | |||||
2MASS J03322564+1857138 | 03:32:25.671 | +18:57:13.38 | 17.956 | |||||
2MASS J03323893+1512173 | 03:32:38.982 | +15:12:16.99 | 19.335 | |||||
2MASS J03334166+1924263 | 03:33:41.669 | +19:24:26.22 | 20.217 | |||||
Gaia DR2 40541334474313728 | 03:34:33.106 | +12:12:29.76 | 19.087 | |||||
2MASS J03350086+1539436 | 03:35:00.896 | +15:39:43.16 | 16.458 | |||||
WISEA J033651.60+154553.3 | 03:36:51.600 | +15:45:53.00 | 20.777 | |||||
2MASS J03373345+0616472 | 03:37:33.487 | +06:16:46.69 | 15.625 | |||||
WISEA J033742.99+191646.7 | 03:37:42.991 | +19:16:46.69 | 20.716 | |||||
2MASS J03375620+0841417 | 03:37:56.241 | +08:41:41.50 | 15.761 | |||||
2MASS J03380150+1638387 | 03:38:01.544 | +16:38:38.07 | 16.476 | |||||
2MASS J03402733+0811017 | 03:40:27.369 | +08:11:01.28 | 18.544 | |||||
2MASS J03412704+0811542 | 03:41:27.091 | +08:11:53.99 | 18.093 | |||||
2MASS J03422624+1416494 | 03:42:26.282 | +14:16:48.95 | 14.273 | |||||
TYC 71–674–1 | 03:43:48.922 | +06:22:09.72 | 11.764 | |||||
2MASS J03453877+2113077 | 03:45:38.814 | +21:13:07.23 | 17.873 | |||||
WISEA J034623.66+130512.5 | 03:46:23.699 | +13:05:13.10 | 20.643 | |||||
2MASS J03463262+1825551 | 03:46:32.653 | +18:25:54.77 | 17.291 | |||||
2MASS J03473025+0203437 | 03:47:30.270 | +02:03:43.20 | 17.765 | |||||
2MASS J03475182+1043255 | 03:47:51.852 | +10:43:25.14 | 17.095 | |||||
2MASS J03480732+1342170 | 03:48:07.349 | +13:42:16.44 | 14.689 | |||||
2MASS J03483524+0931435 | 03:48:35.249 | +09:31:43.42 | 19.038 | |||||
Gaia DR2 39495385383245568 | 03:48:36.265 | +13:47:27.18 | 19.501 | |||||
2MASS J03485224+0620302 | 03:48:52.278 | +06:20:29.88 | 16.797 | |||||
2MASS J03502829+1753586 | 03:50:28.333 | +17:53:58.17 | 16.941 | |||||
2MASS J03505011+1205084 | 03:50:50.135 | +12:05:08.14 | 17.045 | |||||
2MASS J03522921+1037209 | 03:52:29.239 | +10:37:20.63 | 19.289 | |||||
2MASS J03523586+0709204 | 03:52:35.898 | +07:09:20.05 | 15.097 | |||||
2MASS J03531715+1823316 | 03:53:17.251 | +18:23:30.59 | 20.569 | |||||
2MASS J03531923+1321065 | 03:53:19.280 | +13:21:06.14 | 18.676 | |||||
2MASS J03541484+1618297 | 03:54:14.874 | +16:18:29.32 | 20.408 | |||||
2MASS J03544106+0912233 | 03:54:41.079 | +09:12:23.12 | 18.979 | |||||
WISEA J035552.96+051855.6 | 03:55:52.992 | +05:18:56.29 | 20.961 | |||||
2MASS J03565177+0511102 | 03:56:51.810 | +05:11:10.05 | 19.460 | |||||
WISEA J035656.05+112815.8 | 03:56:56.042 | +11:28:15.36 | 20.562 | |||||
2MASS J03573966+1441432 | 03:57:39.695 | +14:41:42.55 | 19.217 | |||||
2MASS J03574260+0551215 | 03:57:42.630 | +05:51:21.16 | 16.049 | |||||
2MASS J03580299+1726283 | 03:58:03.024 | +17:26:27.95 | 16.133 | |||||
2MASS J03581131+0611071 | 03:58:11.336 | +06:11:07.00 | 18.454 | |||||
2MASS J03585422+1318017 | 03:58:54.255 | +13:18:01.14 | 17.977 | |||||
2MASS J04001889+1117530 | 04:00:18.930 | +11:17:52.66 | 13.739 | |||||
2MASS J04004600+1543113 | 04:00:46.046 | +15:43:10.84 | 16.738 | |||||
2MASS J04011928+0132374 | 04:01:19.312 | +01:32:37.10 | 18.292 | |||||
2MASS J04013237+0002523 | 04:01:32.411 | +00:02:51.85 | 18.162 | |||||
2MASS J04021909+1117014 | 04:02:19.090 | +11:17:01.23 | 18.698 | |||||
2MASS J04023974+0356420 | 04:02:39.778 | +03:56:41.76 | 19.951 | |||||
2MASS J04034941+0951155 | 04:03:49.434 | +09:51:14.90 | 17.903 | |||||
2MASS J04040646+1132063 | 04:04:06.475 | +11:32:05.86 | 19.636 | |||||
2MASS J04043739+0730434 | 04:04:37.407 | +07:30:42.90 | 18.936 | |||||
2MASS J04044493+0611385 | 04:04:44.961 | +06:11:38.14 | 20.092 | |||||
2MASS J04044544+1052456 | 04:04:45.463 | +10:52:45.52 | 17.747 | |||||
Gaia DR2 3260444330208719104 | 04:05:07.086 | +03:53:23.29 | 18.802 | |||||
2MASS J04053132+0742252 | 04:05:31.344 | +07:42:24.88 | 17.506 | |||||
2MASS J04060831+0540134 | 04:06:08.318 | +05:40:13.35 | 16.840 | |||||
2MASS J04074808+0757523 | 04:07:48.105 | +07:57:52.14 | 18.604 | |||||
2MASS J04080091+1031113 | 04:08:00.930 | +10:31:11.12 | 20.540 | |||||
2MASS J04080870+0909272 | 04:08:08.721 | +09:09:26.86 | 18.712 | |||||
2MASS J04083351+0457383 | 04:08:33.534 | +04:57:37.83 | 18.685 | |||||
Gaia DR2 3305092233237657984 | 04:08:34.341 | +12:22:22.55 | 20.756 | |||||
2MASS J04092969+1615365 | 04:09:29.713 | +16:15:36.06 | 16.540 | |||||
2MASS J04104079+1029064 | 04:10:40.805 | +10:29:05.83 | 19.498 | |||||
2MASS J04112019–0103368 | 04:11:20.182 | –01:03:37.12 | 17.335 | |||||
2MASS J04114302+1201505 | 04:11:43.049 | +12:01:50.53 | 18.826 | |||||
2MASS J04114604+1131038 | 04:11:46.059 | +11:31:03.41 | 18.413 | |||||
Gaia DR2 3284355203419497088 | 04:11:52.187 | +04:26:32.33 | 18.059 | |||||
2MASS J04121061+0742039 | 04:12:10.657 | +07:42:03.47 | 20.471 | |||||
2MASS J04122904+0942220 | 04:12:29.061 | +09:42:21.64 | 17.708 | |||||
2MASS J04124666+0614198 | 04:12:46.682 | +06:14:19.72 | 18.456 | |||||
2MASS J04131221+0836469 | 04:13:12.240 | +08:36:46.65 | 19.861 | |||||
2MASS J04144878+1348588 | 04:14:48.806 | +13:48:58.59 | 18.052 | |||||
2MASS J04153145–0125053 | 04:15:31.476 | –01:25:05.46 | 18.644 | |||||
2MASS J04160719+0411019 | 04:16:07.210 | +04:11:01.68 | 17.148 | |||||
2MASS J04162916+0722379 | 04:16:29.187 | +07:22:37.84 | 16.108 | |||||
2MASS J04164032+0030538 | 04:16:40.348 | +00:30:53.49 | 17.956 | |||||
WISEA J041646.88+040134.1 | 04:16:46.901 | +04:01:33.88 | 20.238 | |||||
Gaia DR2 3253988341527871488 | 04:18:21.383 | –01:20:55.20 | 19.121 | |||||
2MASS J04191862+0707428 | 04:19:18.640 | +07:07:42.59 | 18.766 | |||||
Gaia DR2 3255556657429771008 | 04:19:31.874 | +00:23:34.72 | 20.755 | |||||
2MASS J04201559–0132340 | 04:20:15.622 | –01:32:34.38 | 17.779 | |||||
2MASS J04213553+0128517 | 04:21:35.551 | +01:28:51.35 | 17.804 | |||||
WISEA J042242.08+025448.7 | 04:22:42.098 | +02:54:48.47 | 20.330 | |||||
HD 27860 | 04:24:14.495 | +12:09:28.39 | 5.925 | |||||
2MASS J04254368+0506464 | 04:25:43.699 | +05:06:46.15 | 18.873 | |||||
2MASS J04265837+0126246 | 04:26:58.385 | +01:26:24.36 | 16.156 | |||||
2MASS J04270307+0148468 | 04:27:03.095 | +01:48:46.71 | 19.640 | |||||
2MASS J04272827–0236149 | 04:27:28.295 | –02:36:15.14 | 18.229 | |||||
2MASS J04283451+0129362 | 04:28:34.531 | +01:29:36.10 | 18.082 | |||||
WISEA J042913.82–002417.0 | 04:29:13.841 | –00:24:17.21 | 19.750 | |||||
2MASS J04304508+0756242 | 04:30:45.103 | +07:56:23.69 | 18.181 | |||||
2MASS J04304930+1019441 | 04:30:49.319 | +10:19:43.77 | 18.784 | |||||
2MASS J04310354+0036313 | 04:31:03.558 | +00:36:31.10 | 16.009 | |||||
2MASS J04325031–0253281 | 04:32:50.340 | –02:53:28.45 | 17.697 | |||||
WISEA J043304.99+053543.9 | 04:33:04.994 | +05:35:43.68 | 20.832 | |||||
2MASS J04345817–0050299 | 04:34:58.194 | –00:50:30.19 | 14.079 | |||||
WISEA J043503.94+034239.6 | 04:35:03.926 | +03:42:39.41 | 20.967 | |||||
Gaia DR2 3204500079076340480 | 04:35:09.342 | –03:32:16.93 | 19.324 | |||||
2MASS J04351726+0310298 | 04:35:17.290 | +03:10:29.61 | 17.823 | |||||
2MASS J04353654+0204009 | 04:35:36.562 | +02:04:00.59 | 18.411 | |||||
2MASS J04404378+0409468 | 04:40:43.808 | +04:09:46.58 | 16.839 | |||||
2MASS J04415810+0223059 | 04:41:58.131 | +02:23:05.76 | 17.125 | |||||
2MASS J04424602+0723403 | 04:42:46.049 | +07:23:39.96 | 17.422 | |||||
WISEA J044514.79+020926.4 | 04:45:14.811 | +02:09:25.97 | 20.345 | |||||
2MASS J04451739–0046433 | 04:45:17.416 | –00:46:43.56 | 16.242 | |||||
2MASS J04455269+0118408 | 04:45:52.712 | +01:18:40.47 | 17.350 | |||||
2MASS J04482662+0236432 | 04:48:26.639 | +02:36:43.03 | 17.480 | |||||
2MASS J04502730–0318287 | 04:50:27.329 | –03:18:29.05 | 16.208 | |||||
2MASS J04503202–0050182 | 04:50:32.037 | –00:50:18.54 | 18.272 |
Note. — The MUTA identifiers listed in this table are defined in Section 4.4. Some identifiers listed here contain only one component of a binary system (either A or B) because the other component was recovered in either comover searches of sections 4.1 and 4.4. Only a portion of the table is shown here. The full table is available as online-only additional material. Targets without a MUTA ID number were flagged as problematic (i.e., low-likelihood candidates). See section 4 for more details.
MUTA | R.A. | Decl. | Parallax | Gaia DR2 | Sep. | Pos. Ang. | |||
---|---|---|---|---|---|---|---|---|---|
ID | Name | (hh:mm:ss.sss) | (dd:mm:ss.ss) | () | () | (mas) | mag | (′′) | (°) |
5 | 29 Tau | 03:45:40.466 | +06:02:59.78 | ||||||
137 | 2MASS J03454104+0602349 | 03:45:41.066 | +06:02:34.59 | ||||||
138 | 2MASS J03454269+0603039 | 03:45:42.712 | +06:03:03.66 | ||||||
139 | 2MASS J03454440+0603283 | 03:45:44.425 | +06:03:28.04 | ||||||
10 | V766 Tau | 03:51:15.896 | +13:02:45.52 | ||||||
182 | 2MASS J03511041+1302467 | 03:51:10.454 | +13:02:46.16 | ||||||
19 A | HD 23376 | 03:44:58.957 | +08:19:10.09 | ||||||
19 B | TYC 658–1007–2 | 03:44:59.048 | +08:19:13.81 | ||||||
30 A | TYC 668–737–1 | 04:21:24.386 | +08:53:54.34 | ||||||
30 B | 2MASS J04212444+0853488 | 04:21:24.473 | +08:53:48.52 | ||||||
42 A | 2MASS J02581643+2456424 | 02:58:16.484 | +24:56:41.76 | 15.193 | |||||
42 B | Gaia DR2 113410746049727744 | 02:58:16.476 | +24:56:42.65 | 16.776 | |||||
373 | 2MASS J02581815+2456552 | 02:58:18.198 | +24:56:54.67 | 20.136 | |||||
130 A | 2MASS J03442859+0716100 | 03:44:28.602 | +07:16:10.10 | ||||||
130 B | Gaia DR2 3277686910210391424 | 03:44:28.657 | +07:16:08.46 | ||||||
144 A | 2MASS J03463553+1317056 | 03:46:35.533 | +13:17:06.31 | ||||||
144 B | Gaia DR2 37943944413361792 | 03:46:35.594 | +13:17:04.31 | ||||||
149 | 2MASS J03471144+0526234 | 03:47:11.466 | +05:26:23.15 | ||||||
150 | BD+04 589 | 03:47:13.551 | +05:26:23.49 | ||||||
159 | TYC 71–542–1 | 03:47:56.865 | +06:16:06.67 | ||||||
374 | 2MASS J03475024+0617499 | 03:47:50.279 | +06:17:49.65 | ||||||
188 A | 2MASS J03524018+0830333 | 03:52:40.220 | +08:30:33.13 | ||||||
188 B | Gaia DR2 3301507795268229248 | 03:52:40.165 | +08:30:30.19 | ||||||
231 A | 2MASS J04044937+0935076 | 04:04:49.382 | +09:35:07.13 | ||||||
231 B | Gaia DR2 3301900595795159040 | 04:04:49.493 | +09:35:07.71 | ||||||
236 A | 2MASS J04054018+0722109 | 04:05:40.210 | +07:22:10.83 | ||||||
236 B | Gaia DR2 3297969498128206208 | 04:05:40.167 | +07:22:12.08 | ||||||
265 A | 2MASS J04161320–0119554 | 04:16:13.253 | –01:19:55.93 | ||||||
265 B | Gaia DR2 3254162137382331136 | 04:16:13.147 | –01:19:54.96 | ||||||
267 | UCAC2 30946195 | 04:17:18.672 | –02:16:02.15 | ||||||
375 | HD 27162 | 04:17:17.915 | –02:16:26.41 | ||||||
287 A | 2MASS J04200281+0010109 | 04:20:02.840 | +00:10:10.78 | ||||||
287 B | Gaia DR2 3254797311502540032 | 04:20:02.874 | +00:10:08.62 | ||||||
280 A | CRTS J042024.3+001725 | 04:20:24.319 | +00:17:25.43 | ||||||
280 B | Gaia DR2 3254823940299749376 | 04:20:24.331 | +00:17:26.71 | ||||||
305 A | BD–03 789 | 04:28:37.716 | –03:15:44.58 | ||||||
305 B | 2MASS J04283839–0315371 | 04:28:38.423 | –03:15:37.42 | ||||||
324 A | HD 29182 | 04:35:53.776 | +05:06:15.36 | ||||||
324 B | TYC 90–953–1 | 04:35:52.439 | +05:05:30.40 | ||||||
325 A | 2MASS J04363330+0511304 | 04:36:33.328 | +05:11:29.84 | ||||||
325 B | Gaia DR2 3282460371222713728 | 04:36:33.274 | +05:11:31.41 | ||||||
338 A | TYC 4739–1225–1 | 04:39:20.251 | –03:14:21.79 | ||||||
338 B | 2MASS J04392073–0314301 | 04:39:20.752 | –03:14:30.44 | ||||||
346 A | 2MASS J04421498+0250387 | 04:42:14.998 | +02:50:38.54 | ||||||
346 B | 2MASS J04421451+0250336 | 04:42:14.531 | +02:50:33.42 | ||||||
351 | TYC 83–1232–1 | 04:43:04.063 | +00:49:47.45 | ||||||
353 | 2MASS J04431309+0048174 | 04:43:13.116 | +00:48:17.19 | ||||||
371 A | 2MASS J04544679–0001085 | 04:54:46.790 | –00:01:08.42 | ||||||
371 B | Gaia DR2 3228318975563766784 | 04:54:46.875 | –00:01:10.21 | ||||||
372 A | TYC 4741–307–1 | 04:56:18.287 | –01:53:33.04 | ||||||
372 B | 2MASS J04561830–0153393 | 04:56:18.315 | –01:53:39.53 | ||||||
2MASS J03250457+0728193 | 03:25:04.592 | +07:28:18.82 | |||||||
Gaia DR2 9977797439144320 | 03:25:04.736 | +07:28:20.43 | |||||||
HD 23110 | 03:42:45.949 | +07:54:10.34 | |||||||
TYC 657–794–2 | 03:42:46.021 | +07:54:09.49 | |||||||
2MASS J03424511+0754507 | 03:42:45.157 | +07:54:50.35 |
Note. — See section 4.1 for more details.
One notable case of a star with co-moving components is 29 Tau, the most massive member of MUTA. 29 Tau (MUTA 5, Gaia DR2 3276605295710700032) is a B3 + A7 binary star (Beavers & Cook, 1980), with three co-moving systems within 70′′: 29 Tau B (MUTA 139; 2MASS J03454440+0603283; Gaia DR2 3276604922051089664), which is itself a spectral binary (Mason et al., 2001); 29 Tau C (MUTA 137; 2MASS J03454104+0602349; Gaia DR2 3276604544094119424); and 29 Tau D (MUTA 138; 2MASS J03454269+0603039; Gaia DR2 3276604544093968896). In addition to these six system components, there are two other Gaia DR2 entries within 42′′ of 29 Tau (Gaia DR2 3276604509734231808 and Gaia DR2 3276605265648475776) located within 300 pc of the Sun with inconsistent proper motions and parallaxes. Both of them have re-normalised unit weight error (RUWE) values of 1.1 which is not clearly indicative of bad parallax solutions, and indicates that they are probably unrelated to 29 Tau. For this reason, we ignored them in this analysis but we would recommend re-visiting this when further Gaia data releases are published. Two additional MUTA candidates are within 700–715′′ of 29 Tau: MUTA 143 (2MASS J03460544+0553074; Gaia DR2 3276586333432639744) and MUTA 135 (2MASS J03450918+0612030; Gaia DR2 3276798401738487808). Gaia DR2 3276584478006772224 also seems co-moving with 29 Tau at a separation of 9775, but was not recovered in our search because its MUTA probability (89.7%) is below our selection threshold.
Cross-matching our list of candidates with the Oh et al. (2017) catalog of co-moving systems yielded a total of 28 matches, to Groups 39, 43, 52, 60, 124, 242, 1099 and 1109. Each of these groups have a total of members between 2 and 7. We verified that each of these groups were included in their entirety in our list of MUTA candidates, and found 4 missing components of Group 39 and one missing component of Group 1109. We added these objects to our list of low-likelihood MUTA candidates despite their BANYAN membership probabilities below 90% (ranging from 0% to 64%) for completion. As demonstrated by Faherty et al. (2018), the algorithm of Oh et al. (2017) tends to break up nearby associations in many sub-groups because of the strong variations and correlations in direct kinematic observables (sky position, proper motion and parallax) caused by their wide distributions on the sky. The full list of matches between our candidates and Oh et al. (2017) groups are shown in Table 5.
4.2 Red Giant Stars
One candidate member of the MUTA association, HD 27860, is located far above the main sequence and within the red giant branch in Figure 5. A literature search revealed that this object has a spectral type K2 III (Woolley et al., 1981), consistent with its position in the color-magnitude diagram. Based on the compilations of stars within 40 pc established by Gray et al. (2003) and Gray et al. (2006), stars with the same spectral type have an average color and absolute magnitude 333See also http://www.pas.rochester.edu/~emamajek/spt/K2III.txt.
Using the three-dimensional extinction map STructuring by Inversion of the Local InterStellar Medium (STILISM; Lallement et al., 2014; Capitanio et al., 2017; Lallement et al., 2018)444Available at https://stilism.obspm.fr, we can expect HD 27860 to be subject to an extinction based on its sky position and distance, which translates to (using a total to selective extinction ratio for this photometric band). Correcting its observed properties in the same photometric bands ( and ; ESA 1997) for extinction yields an intrinsic color of and an absolute magnitude , placing it closer in colors to the average value for K3 III giants ().
Using the bolometric correction of Flower (1996) for this color (), we estimate a bolometric magnitude and . We estimated its effective temperature at K by interpolating its extinction-corrected color and comparing them with averages from Gray et al. (2003) and Gray et al. (2006) for spectral types K2 III and K3 III. These physical parameters are consistent with a luminosity class III; the Bertelli et al. (2009) solar-metallicity isochrones predict a mass of 2.44 , a surface gravity and an age of 650 Myr.
HD 27860 seems significantly too old to be a member of MUTA based on the color-magnitude sequence of this young association (Figure 5). The main-sequence turn-off of a 650 Myr association would be located at spectral types A0 or later555See http://www.pas.rochester.edu/~emamajek/EEM_dwarf_UBVIJHK_colors_Teff.txt (i.e., at absolute Gaia DR2 magnitudes ). The fact that MUTA includes several members more massive than A0 strongly suggests that HD 27860 is a chance interloper despite its high 98.6% Bayesian membership probability, and we therefore reject it from our list of candidate members.
4.3 White Dwarfs


A subset of MUTA members are located below the main sequence and within the color-magnitude sequence of white dwarfs in Figure 2. We flagged all candidates with an absolute -band magnitude fainter than and a color (shown in Figure 6) as likely white dwarfs, and compared them to total age isochrones obtained by combining MIST stellar main-sequence lifetimes (Choi et al., 2016) and the the Montréal white dwarf cooling tracks (Fontaine et al., 2001)666Available at http://www.astro.umontreal.ca/~bergeron/CoolingModels/, see also Holberg & Bergeron (2006); Kowalski & Saumon (2006); Tremblay et al. (2011) and Bergeron et al. (2011). in Figure 7.
All but two white dwarfs in our sample are clearly much older than 150 Myr, inconsistent with the main-sequence turn-off age of MUTA ( 80 Myr). The two youngest and hottest white dwarfs in this figure are WD 0350+098 (MUTA 190; other designations include 1RXS J035315.5+095700, SDSS J035315.72+095633.7) and WD 0340+103 (MUTA 125; other designations include RBS 466, 1RXS J034314.1+102941, and
SDSS J034314.35+102938.4), and are discussed further in Section 6.4.

We can estimate a false-positive rate for our list of MUTA candidate members based on the fact that we uncovered 10 white dwarfs that are clearly too old for this young association. The number density of white dwarfs, objects pc-3 (Hollands et al., 2018), is small compared with that of main-sequence stars ( objects pc-3; Kirkpatrick et al. 2012). Assuming that white dwarfs have similar kinematics to main-sequence stars, this means we could expect as many as stars in our sample to be contaminants if we applied no other cuts than BANYAN probabilities based on proper motion and parallax without radial velocity measurements (none of the white dwarf contaminants have radial velocity measurements). An additional 28 Gaia DR2 sources would have been uncovered in our survey if we used only these observables and no other criteria, leaving our estimated number of contaminants to in our final list of candidates, or % of our full sample of 503 objects. The majority of contaminants are expected to be M dwarfs.
4.4 Poor Astrometric Solutions
The Gaia DR2 team recommends placing low confidence in astrometric solutions with a RUWE larger than 1.4777As described at https://www.cosmos.esa.int/web/gaia/dr2-known-issues.. We therefore flagged all 52 MUTA candidates and members with RUWE (shown in Figure 8) and consider them as low-likelihood candidates; we consider that an observational follow-up of these objects will potentially be useful, but should be less prioritary. It is likely that some of these issues will be resolved in the next Gaia DR2 data release.
4.5 Visual Inspection of Finder Charts

We generated finder charts for all MUTA objects with available survey data from DSS, SDSS (Alam et al., 2015), UKIDSS (Lawrence et al., 2007), VHS (McMahon et al., 2013), Pan-STARRS (Chambers et al., 2016), WISE (Wright et al., 2010) and 2MASS (Skrutskie et al., 2006) data with the finder_charts.py Python package (Gagné et al., 2018)888Available at https://github.com/jgagneastro/finder_charts., on which we overlaid Gaia DR2 catalog entries with arrows and symbol sizes indicating their individual proper motions and distances. We used these figures to identify and correct any mismatches in our automated cross-matches to 2MASS and WISE, which tends to happen when a target has a missing entry in either catalog.
We also verified that binaries and co-moving systems had the correct component attached to each catalog, and noted 12 stars that visually appeared co-moving with one of our targets at a similar distance, but were not recovered with our co-moving search described in Section 4.1. Those usually have Gaia DR2 proper motions or parallaxes that are slight mis-matches to our MUTA candidate or member, and are listed in Table 6. It is possible that some of these systems suffer from a bad parallax solution, either because they are themselves multiple systems (e.g., 30 Tau and TYC 661–1404–1, respectively MUTA 3 A and MUTA 3 B), or contaminated by a background source (althoug they all have RUWE ). We listed these systems that almost seem co-moving in Table 6 for later follow-up, but we excluded them from the current analysis.
A number of MUTA candidates are located well below the main sequence in a Gaia DR2 color-magnitude diagram (see Figure 5), but yet not faint enough to be credible white dwarfs (see Section 4.3). A fraction of these objects failed the Gaia DR2 RUWE selection criterion for good astrometric solutions, indicating that bad parallax solutions are likely part of the explanation. Figure 9 shows a finder chart for one such object (WISEA J033742.99+191646.7)999All finder charts are available as online-only supplementary data.. In this example, the finder chart shows that it is well detected at red-optical wavelengths (e.g., Pan-STARRS) and in WISE , but too faint to be detected in 2MASS in the near-infrared. This unusual combination indicates a likely contribution from two distinct blackbodies. The presence of an accretion disks could potentially explain this, however those usually result in much redder Gaia DR2 colors, which would push the object far to the right of, rather than below, the main sequence. The simplest explanation seems to be that this object is a blend of two sources, maybe located at different distances, but at an angular separation small enough that they are unresolved in all the aforementioned surveys.
We assigned MUTA identifiers (31 to 372) to all candidate members that were not rejected or defined as low-likelihood candidates based either on their poor astrometric solutions, ages that are definitely too old, or problematic position in a color-magnitude diagram. We ordered these identifiers by right ascension. Stars identified in Section 4.1 as co-moving with a well-behaved MUTA candidate or member which did not have a MUTA identified were assigned identifiers 373–375. Those still without identifiers that belong in one of the Oh et al. (2017) groups associated with MUTA were assigned identifiers 376–382, and those visually identified as co-moving with a well-behaved candidate in this section were assigned identifiers 383–386.
MUTA | Gaia DR2 | Oh et al. (2017) | Object | |
---|---|---|---|---|
ID | Name | ID | Group | TypeaaInitial: members of MUTA from our initial list. Candidates: candidates of MUTA recovered in Section 4. Incomplete: Targets missing from our list of MUTA initial members and new candidates. |
368 | HD 31125 | 3226496187146449920 | 39 | Candidates |
369 | TYC 4745–475–1 | 3224698799168916864 | 39 | Candidates |
372 A | TYC 4741–307–1 | 3225639289631939456 | 39 | Candidates |
379 | BD+00 884 | 3231439080323844864 | 39 | Incomplete |
380 | HD 32264 | 3225291882613467520 | 39 | Incomplete |
381 | HD 32721 | 3212973572810773120 | 39 | Incomplete |
382 | HD 33023 | 3212956839618107648 | 39 | Incomplete |
10 | V766 Tau | 37136834159399808 | 43 | Initial |
21 | HD 286374 | 3303308245556503296 | 43 | Initial |
22 | PPM 119410 | 36595943156045824 | 43 | Initial |
26 | TYC 662–217–1 | 3304906145189468416 | 43 | Initial |
28 | TYC 664–136–1 | 39841357885932288 | 43 | Initial |
377 | HIP 18778 | 3301831773241303552 | 43 | Initial |
13 | HD 23990 | 3302396166303947904 | 52 | Initial |
19 A | HD 23376 | 3278197770802258944 | 52 | Initial |
19 B | TYC 658–1007–2 | 3278197766505583232 | 52 | Initial |
95 | HD 22073 | 11397988505713536 | 52 | Candidates |
140 | TYC 658–828–1 | 3278300987456845440 | 52 | Candidates |
17 | HD 27687 | 3286590824092307200 | 60 | Initial |
18 | HD 28356 | 3285720938596464640 | 60 | Initial |
25 | TYC 80–202–1 | 3297372944352021120 | 60 | Initial |
30 A | TYC 668–737–1 | 3299167141170181888 | 60 | Initial |
290 | BD+05 638 | 3284966433101477376 | 60 | Candidates |
33 | HD 17008 | 127148009968227584 | 124 | Candidates |
35 | TYC 1785–155–1 | 114510012864474112 | 124 | Candidates |
41 | TYC 1790–927–1 | 115353480017970560 | 124 | Candidates |
11 | HD 28715 | 3285542336676520448 | 242 | Initial |
324 A | HD 29182 | 3282435563491664896 | 242 | Candidates |
324 B | TYC 90–953–1 | 3282434979377650176 | 242 | Incomplete |
20 | HIP 17133 | 38088873789758720 | 1099 | Initial |
117 A | TYC 663–362–1 | 38076641722829440 | 1099 | Candidates |
376 | TYC 665–150–1 | 38398936068862464 | 1109 | Candidates |
378 | HD 286412 | 3305439511410844800 | 1109 | Incomplete |
Note. — See section 4.1 for more details.
MUTA | R.A. | Decl. | Parallax | Gaia DR2 | Sep. | Pos. Ang. | |||
---|---|---|---|---|---|---|---|---|---|
ID | Name | (hh:mm:ss.sss) | (dd:mm:ss.ss) | () | () | (mas) | mag | (′′) | (°) |
3 A | 30 Tau | 03:48:16.292 | +11:08:35.52 | 5.040 | |||||
3 B | TYC 661-1404-1 | 03:48:16.835 | +11:08:40.16 | 9.269 | |||||
5 | 29 Tau | 03:45:40.466 | +06:02:59.78 | 5.295 | |||||
383 | 2MASS J03453759+0603048 | 03:45:37.587 | +06:03:04.31 | 15.481 | |||||
97 A | 2MASS J03350340+1431490 | 03:35:03.438 | +14:31:48.54 | 15.369 | |||||
97 B | 2MASS J03350317+1431358 | 03:35:03.209 | +14:31:35.33 | 18.097 | |||||
104 A | 2MASS J03361762+2153391 | 03:36:17.665 | +21:53:38.50 | 10.910 | |||||
104 B | 2MASS J03361732+2153271 | 03:36:17.360 | +21:53:26.42 | 18.454 | |||||
117 A | TYC 663–362–1 | 03:40:57.781 | +13:09:03.06 | 10.493 | |||||
117 B | 2MASS J03405723+1308577 | 03:40:57.261 | +13:08:57.23 | 18.437 | |||||
153 A | TYC 1252–301–1 | 03:47:23.901 | +18:43:17.68 | 11.689 | |||||
153 B | Gaia DR2 44752086050666368 | 03:47:23.645 | +18:43:18.70 | 17.855 | |||||
177 A | 2MASS J03505694+0730565 | 03:50:56.976 | +07:30:56.18 | 16.916 | |||||
177 B | Gaia DR2 3277369048270999936 | 03:50:56.968 | +07:30:53.92 | 20.438 | |||||
225 A | 2MASS J04021281+0817400 | 04:02:12.839 | +08:17:39.75 | 16.635 | |||||
225 B | 2MASS J04021257+0817410 | 04:02:12.593 | +08:17:40.67 | 17.316 | |||||
271 | 2MASS J04181095+0934586 | 04:18:10.980 | +09:34:58.24 | 17.228 | |||||
384 | 2MASS J04181193+0934365 | 04:18:11.958 | +09:34:36.14 | 16.800 | |||||
277 A | 2MASS J04200165+0759584 | 04:20:01.666 | +07:59:57.72 | 15.336 | |||||
277 B | Gaia DR2 3298956138016754048 | 04:20:01.719 | +07:59:58.51 | 16.289 | |||||
279 | 2MASS J04201617+0959534 | 04:20:16.202 | +09:59:53.06 | 17.379 | |||||
385 | TYC 671–129–1 | 04:20:16.048 | +09:59:46.25 | 10.795 | |||||
318 A | 2MASS J04341953+0226260 | 04:34:19.560 | +02:26:25.89 | 12.150 | |||||
318 B | Gaia DR2 3279527149078835712 | 04:34:19.467 | +02:26:25.91 | 15.960 | |||||
329 A | 2MASS J04372971–0051241 | 04:37:29.730 | –00:51:24.47 | 13.223 | |||||
329 B | Gaia DR2 3229491776511286016 | 04:37:29.780 | –00:51:25.66 | 16.507 | |||||
331 A | 2MASS J04382750-0342441 | 04:38:27.523 | –03:42:44.47 | 14.931 | |||||
331 B | Gaia DR2 3201810884087980800 | 04:38:27.437 | –03:42:46.23 | 18.416 | |||||
368 | HD 31125 | 04:53:04.828 | –01:16:33.04 | 7.918 | |||||
386 | HD 31124 | 04:53:04.574 | –01:15:52.17 | 8.046 | |||||
2MASS J03343284+1212290 | 03:34:32.872 | +12:12:28.55 | 12.302 | ||||||
Gaia DR2 40541334474313728 | 03:34:33.106 | +12:12:29.76 | 19.087 |
Note. — See section 4.5 for more details.
5 CORRECTING EXTINCTION IN GAIA DR2 PHOTOMETRY
The MUTA association is distant enough that some of its members appear slightly reddened by interstellar dust. We used STILISM (Lallement et al., 2014; Capitanio et al., 2017; Lallement et al., 2018)101010Available at https://stilism.obspm.fr to determine the individual extinction values for individual MUTA objects based on their sky position and Gaia DR2 distance. The resulting individual extinction values are displayed in Figure 10.



We corrected the color-magnitude diagram position of MUTA members and candidates with an iterative method to account for the wide Gaia DR2 photometric bandpasses. As shown in Figure 11, even the bandpass spans a significant region over which both the extinction curve of Fitzpatrick (1999) and the spectral energy density of an M-type star vary significantly. As a consequence, the reddening vectors in Gaia DR2 color-magnitude sequences will differ significantly across spectral types.
The flux of a star with a spectral energy density observed through an instrument with a bandpass is given by:
(1) |
In the presence of interstellar extinction , the observed flux is:
(2) |
and therefore the correction factor that remains valid for wide bandpasses is:
(3) |

In effect, this correction is a weighted average of the extinction curve, where the weight is given by the product of the stellar spectral energy density with the instrumental bandpass. In general, the spectral energy densities of MUTA members and candidates have not been measured, and their spectral types are unknown. We therefore used an iterative method where the photometric spectral type of each star is first estimated from its color. The versus spectral type relation for stars with spectral types B0 to L0 is shown in Figure 12. These data were drawn from the list of nearby young association members of Gagné et al. (2018) and the List of Ultracool Dwarfs111111Available at http://astro.umontreal.ca/~gagne/ultracool_dwarfs.php that includes data from previous lists of brown dwarfs (Dupuy & Liu, 2012; Mace, 2014; Gagné et al., 2015; Liu et al., 2016; Faherty et al., 2016). A polynomial relation was fitted to the data and is also displayed in the figure; the coefficients to this polynomial sequence are available as online-only material. We preferred using a Gaia DR2 color to spectral type relation rather than a Gaia DR2 absolute magnitude to spectral type relation, because unresolved multiples would bias the latter more significantly.
We used the Pickles Atlas of spectral energy distributions for B0–M9 stars (Pickles, 1998) and interpolated the Gaia DR2 instrumental bandpasses and the extinction curve of Fitzpatrick (1999; with a nominal total to selective extinction value ) on the Pickles wavelength vector to determine an appropriate extinction correction.
The resulting extinction-corrected color was then used to obtain a better photometric spectral type estimate, which we used in turn to correct the raw color anew. This step was repeated until the photometric spectral type estimate of a star remained unchanged. A total of four iterations were needed for the de-reddening correction to converge for all MUTA stars. The resulting extinction vectors and corrected color-magnitude diagram of MUTA are shown in Figure 13.
In Tables 7 and 8, we provide reddening values and as a function of spectral types or uncorrected Gaia DR2 colors, which can be used to de-redden the Gaia DR2 photometry of main-sequence or young stars with the following relations:
(4) | ||||
(5) |
Spectral | |||
---|---|---|---|
Type | (mag) | (mag) | (mag) |
B3 | |||
B5 | |||
B7 | |||
B9 | |||
A1 | |||
A3 | |||
A5 | |||
A7 | |||
A9 | |||
F1 | |||
F3 | |||
F5 | |||
F7 | |||
F9 | |||
G1 | |||
G3 | |||
G5 | |||
G7 | |||
G9 | |||
K1 | |||
K3 | |||
K5 | |||
K7 | |||
K9 | |||
M1 | |||
M3 | |||
M5 |
Note. — See section 5 for more details.
Uncorrected | |||
---|---|---|---|
(mag) | (mag) | (mag) | |
0.18 | |||
0.08 | |||
0.02 | |||
0.12 | |||
0.22 | |||
0.32 | |||
0.42 | |||
0.52 | |||
0.62 | |||
0.72 | |||
0.82 | |||
0.92 | |||
1.02 | |||
1.12 | |||
1.22 | |||
1.32 | |||
1.42 |
Note. — See section 5 for more details.
6 DISCUSSION
In this section, we discuss various properties of the MUTA members and of their population as a whole. Photometric spectral type estimates and additional substellar candidates are discussed in Sections 6.1 and 6.2. This is followed by an estimation of the isochronal age of MUTA (Section 6.3) and a discussion of the cooling ages of the two hot white dwarf candidate members of MUTA (Section 6.4). We discuss literature lithium absorption measurements for K- to G-type members of MUTA in Section 6.5, and discuss the present-day mass function of MUTA in Section 6.6. The stellar activity of its members is assessed in Section 6.7. MUTA is placed in context with the Galactic kinematic structure recently unveiled by Kounkel & Covey (2019) in Section 6.8.
6.1 Photometric Spectral Type Estimates
The extinction correction method described above directly provides photometric spectral type estimates for MUTA candidates and members with no spectral type information in the literature. We used a slightly different method to estimate the photometric spectral types of objects near the substellar regime with near-infrared 2MASS–WISE colors , corresponding to a spectral types M6 and later (Gagné et al., 2015). For these redder objects, we used the spectral type to relation of Gagné et al. (2015) to determine a more accurate subtype given that the Gaia DR2 colors are more spread and based on lower-quality detections in these cases (e.g., see Smart et al. 2019). All photometric spectral type estimates are shown in Figure 14.

6.2 Substellar Objects
In Figures 15 and 16, we show near-infrared color-magnitude sequences of MUTA candidates based on 2MASS and WISE photometry, compared with those of field-aged and young L-type or later low-mass stars and brown dwarfs. In both cases, the MUTA sequence forms a prolongation of the young substellar sequences at brighter absolute magnitudes, and there is a small overlap indicating that a few MUTA candidates discussed here may have spectral types as late as L0 (although at the age of MUTA the substellar boundary is near spectral type M7; Allard et al., 2012; Baraffe et al., 2015; Filippazzo et al., 2015). Kirkpatrick et al. (2011) devised a rejection criterion based on WISE photometry to distinguish extragalactic sources from brown dwarfs, but our only MUTA candidates with a sufficient -band detection were not red enough in color to apply the rejection criterion.


6.3 Isochronal Age
The locus of MUTA candidates and members compiled in this work forms a sequence in color-magnitude space that sits between those of the Pleiades association ( Myr; Dahm 2015) and the Tucana-Horologium (see Zuckerman et al., 2001b; Torres et al., 2000), Columba and Carina associations ( 45 Myr; Torres et al., 2008; Bell et al., 2015). We coss-matched all bona fide members of these four associations compiled by Gagné et al. (2018) with Gaia DR2 for this comparison, and built an empirical isochrone for each of them by fitting their sequence with a high-order polynomial. The cross matches with Gaia DR2 were all inspected for spurious matches by building finder charts similar to those discussed in Section 4.5. The color-magnitude positions of all members were corrected for extinction by interstellar dust with the method described in Section 5. This procedure only had a noticeable but small effect on the Pleiades members.
All known unresolved binaries were removed from these lists, and their color-magnitude diagrams were visually inspected to remove the obvious sequence of unresolved binaries and triples that were shifted up by 0.75 and 1.19 mag in Gaia DR2 -band magnitude, respectively. The detailed lists of members used to build these isochrones will be presented in an upcoming publication, along with those of other nearby young associations.
Representing a young association’s color-magnitude sequence with a polynomial curve can be complicated by the fact that they contain many more low-mass stars (e.g., Bochanski et al. 2010), which would cause an over-fitting of the data in the red part of the color-magnitude diagram. To avoid this, we first build a moving box average and standard deviation of the members’ absolute Gaia DR2 -band magnitudes in bins of 0.05 mag in colors, and we subsequently fit a 11-order (Tucana-Horologium, Columba and Carina) or 15-order (Pleiades) polynomial, which were found to be appropriate given the number of stars and the range of colors occupied by the members of these associations. Columba, Tucana-Horologium and Carina were combined as a single 45 Myr-old population as they all share the same age (Bell et al., 2015). This allowed us to build a more accurate empirical isochrone given the larger number of resulting members.
We used our initial list of MUTA members (Table 2) to determine an isochronal age for the association, by comparing each member’s absolute -band magnitude with a hybrid isochrone built from a weighted sum of the 45 Myr and 112 Myr empirical isochrones described above. We assumed that the members are spread around the best-fitting hybrid isochrone along a Gaussian likelihood with a standard deviation of 0.35 mag, typical of other young associations. Members that are either known binaries or have a Gaia DR2 RUWE above 1.4 were not used for this isochronal age determination. These latter objects are identified in Figure 17, along with the empirical isochrones built from the Pleiades and the Tucana-Horologium, Columba and Carina associations.




A one-dimensional grid search was performed to identify the linear combination of the 45 Myr and 112 Myr empirical isochrones that best matches the MUTA stars. A thousand values for a linear coefficient were chosen with to build a set of hybrid isochrones built from the 45 Myr isochrone and the 112 Myr isochrone :
(6) |
The goodness-of-fit of each hybrid isochrone for the values of were assessed by calculating the Gaussian likelihood that the Gaia DR2 absolute -band magnitudes of MUTA members and their associated standard deviations match the model in each color bin :
(7) |
The best-fitting linear combination is displayed in Figure 18. The ages corresponding to each hybrid isochrone were taken as a linear combination of the individual empirical isochrones in logarithm space:
(8) |
The resulting probability density function is shown in Figure 19. It is well represented by a Gaussian in logarithm of age, with an average and characteristic width that correspond to , or an age of Myr.
We also calculated a probability density function for the relative age parameter because the age estimates of both our reference populations could change in the future. For example, some recent lithium depletion boundary age estimates for the Pleiades are as old as Myr (Burke et al., 2004), and Kraus et al. (2014) estimated a slightly younger age for Tucana-Horologium based on the lithium depletion boundary: they found ages of Myr or Myr, depending on the evolutionary models that they used. The age of MUTA can thus be refined with the equation above (i.e., a simple interpolation in log age), replacing with a Gaussian probability density function at for . Using the two extreme ends of these age estimates for the Pleiades and Tucana-Horologium would correspond to MUTA ages of Myr, or Myr, placing two conservative boundaries for the possible age of MUTA.
All MUTA candidate members located more than 0.35 mag fainter than the best-fitting hybrid isochrone were marked as problematic candidates because they likely correspond to interloping field-aged M dwarfs or contaminated Gaia DR2 entries. This flagging procedure is displayed in Figure 20. This step has removed 135 objects from our list of good-quality candidates; we note that this number is comparable to the number of contaminants () we have estimated in Section 4.3 based on the number of old white dwarf interlopers.
6.4 White Dwarf Cooling Ages
In Section 4.3, we noted that our search for additional MUTA candidates yielded 12 white dwarfs seemingly co-moving with MUTA, 10 of which are clearly too cold, and therefore too old, to be credible members. The only two exceptions are WD 0340+103 (MUTA 125) and WD 0350+098 (MUTA 190), which seem to be aged about 200-800 Myr from a first comparison with total-age cooling tracks. However, both white dwarfs are so hot that a direct comparison of color-magnitude relations at visible wavelengths is imprecise, as this regime only samples the Rayleigh-Jeans end of their spectral energy distributions. Furthermore, the Gaia DR2 de-reddening procedure developed here cannot be applied to white dwarfs directly. For this reason, we investigated the properties of both white dwarfs in more details.
WD 0340+103 is an extremely hot white dwarf, which properties have been estimated at , K and a mass of 1.03 by Gentile Fusillo et al. (2019). However, these properties were obtained by fitting models to the Gaia DR2 photometry of WD 0340+103, and the visible photometry of hot stars is relatively insensitive to their fundamental properties given that it only samples the Rayleigh-Jeans limit of their spectral energy distribution. For this reason, we obtained more reliable fundamental parameters by making use of spectroscopy instead of photometry.
We first determined the effective temperature and surface gravity of WD 0340+103 by fitting its SDSS optical spectrum (Ahn et al., 2012) with the grid of non-local thermodynamic equilibrium atmosphere models of A. Bédard (2020, in preparation). This yielded a very hot temperature of K, and . Because WD 0340+103 only exhibits hydrogen features given its DA spectral type, we assumed a pure-hydrogen atmospheric composition. We used the fitting procedure described in Bergeron et al. (1992) and Liebert et al. (2005): briefly, the normalized Balmer lines are adjusted with theoretical line profiles using the Levenberg-Marquardt least-squares method. The observed spectrum of WD 0340+103 was well reproduced by this method, including the emission component at the core of the H line, and as illustrated in Figure 21. The positions of the lower Balmer lines (H, H, and H) were used to measure a total redshift of km s-1, due in part to the gravitational redshift and radial velocity of WD 0340+103.
In a second step, we calculated the mass, radius, luminosity, and cooling age that correspond to the effective temperature and surface gravity of WD 0340+103 using the thick-hydrogen layer () cooling tracks of A. Bédard et al. (2020, in preparation), which are appropriate for the study of hot white dwarfs. Following Holberg & Bergeron (2006), we also computed the absolute SDSS -band magnitude, which we combined with the observed (dereddened) SDSS -band magnitude to evaluate its spectroscopic distance. The atmospheric and stellar parameters of WD 0340+103 are summarized in Table 6.4. Our analysis shows that WD 0340+103 is a highly unusual white dwarf: It is extremely hot, young, and massive. Furthermore, we note that the spectroscopic distance is slightly farther than its Gaia DR2 trigonometric distance, but the values are consistent within measurement errors.
We used the MESA Isochrones and Stellar Tracks (MIST; Choi et al. 2016) to estimate a progenitor mass of for WD 0340+103. This corresponds to a spectral type of about B2, just one subclass earlier than the earliest-type members of MUTA (29 Tau, 30 Tau, Tau and Eri are all B3 stars). This is consistent with the extremely young cooling age of only years which we derived for WD 0340+103. Such a progenitor star has a main-sequence lifetime of Myr, corresponding to a total age of Myr, consistent with our isochronal age of Myr. Combining both estimates in an error-weighted average allows us to refine our age estimate for MUTA at Myr. The core composition of this massive white dwarf likely does not consist of carbon and oxygen, but rather oxygen and neon (Lauffer et al., 2018; Camisassa et al., 2019). This is expected to have a significant effect on the calculated cooling age of about 20% (e.g., see Gagné et al., 2018b; Simon et al., 2015; Simon, 2018), however, in the present scenario the age estimate of WD 0340+103 is completely dominated by its main-sequence lifetime, and its core composition will therefore not have any significant effect on our total age estimation.
The detailed properties of WD 0350+098 are harder to determine because of its lack of spectral lines, likely due to extreme Zeeman broadening caused by a strong magnetic field. Much like WD 0340+103, the age estimate based on Gaia DR2 photometry alone may be unreliable given its extremely blue colors and hot temperature. Adding UV photometry from GALEX (Martin et al., 2005) to better constrain its temperature yielded an estimate of K with a radius of , however, these uncertainties are likely underestimated because the models we used do not include magnetic fields. These parameters would correspond to a mass of and a surface gravity of . Using non-magnetic cooling tracks yields a cooling age estimate of Myr. The main-sequence lifetime that corresponds to the progenitor is Myr, making WD 0350+098 too old for MUTA membership if we take our analysis at face value. However, the lack of magnetic fields in our treatment could have introduced a significant bias in the determination of its cooling age and mass (and therefore its main-sequence lifetime), and for this reason we keep it as a candidate member of MUTA.

Property | Value | Ref. |
---|---|---|
Position and Kinematics | ||
Gaia DR2 Source ID | 36321786805002880 | 1 |
R.A. ep. 2015.5aaJ2000 position at epoch 2015.5 from the Gaia DR2 catalog. Measurement errors are given in units of milliarcseconds. | 03:43:14.370 | 1 |
Decl. ep. 2015.5aaJ2000 position at epoch 2015.5 from the Gaia DR2 catalog. Measurement errors are given in units of milliarcseconds. | +10:29:38.15 | 1 |
() | 1 | |
() | 1 | |
Parallax (mas) | 1 | |
Trigonometric distance (pc) | 1 | |
Spectroscopic distance (pc) | 2 | |
RVoptbbOptimal radial velocity predicted by BANYAN that assumes membership in MUTA. (km s-1) | 2 | |
RVmes (km s-1) | 2 | |
Photometric Properties | ||
(Gaia DR2) | 1 | |
(Gaia DR2) | 1 | |
(Gaia DR2) | 1 | |
(SDSS DR12) | 3 | |
(SDSS DR12) | 3 | |
(SDSS DR12) | 3 | |
(SDSS DR12) | 3 | |
(SDSS DR12) | 3 | |
Fundamental Properties | ||
Spectral type | DA | 4 |
(K) | 2 | |
2 | ||
Mass () | 2 | |
Radius () | 2 | |
2 | ||
Cooling age (Myr) | 2 | |
Progenitor mass () | 2 | |
Progenitor spectral type | B2 | 2 |
Total age (Myr) | 2 |
6.5 Lithium
The equivalent width of the Li I 6708 Å spectral line is a well-established age indicator. Because lithium burns at lower temperatures than hydrogen, it is relatively fragile and will disappear over time if it is allowed to be transported in layers deep enough in a star to reach the threshold temperature for lithium burning. The temperature profile of a star, combined with the location of its convective layers, will determine whether lithium gets burned at all, and how fast it does so. Lower-mass stars (late-K or early-M spectral types) have deep convective layers that allow them to burn through all lithium within only 30 Myr (Randich, 2001), whereas higher-mass stars, with their shallower convective layers, burn lithium more gradually. It takes more than a billion years for stars with spectral types G0 and earlier to burn lithium in their photospheres such that the Li I 6708 Å absorption line disappears completely (Jones et al., 1999). As a result, the sequence in temperature versus Li I absorption line for K-type or earlier stars evolves slowly with time, and makes it possible to place weak constraints on the ages of such early-type stars (e.g., Barrado y Navascués et al., 2001; Soderblom et al., 1993). Similarly, the K-type lithium depletion boundary, where stars below a given temperature stop displaying the lithium absorption line, can be used to place constraints on the age of a stellar population. The location of this boundary is, however, not very sensitive to age for populations 10 Myr and older (Kraus et al., 2014).
Brown dwarfs with masses below 60 do not burn lithium despite their fully convective structure, because they do not reach temperatures sufficient to do so even at their core (e.g., Baraffe et al. 2015). Low-mass stars and brown dwarfs with masses above 60 burn their photosphere lithium slowly, causing the appearance of a second, age-dependent boundary where the lithium absorption line begins appearing again below a threshold in effective temperature. The effective temperatures, spectral types and bolometric luminosities at which this second, M-type lithium depletion boundary occurs, is a strong function of age over the first hundreds of millions of years that follow stellar formation. The lithium depletion boundary has therefore become a popular diagnostic tool to determine precise ages for stellar populations with known M-type stars (e.g., Kraus et al., 2014; Malo et al., 2014b; Shkolnik et al., 2017).
Measuring the equivalent width of the lithium absorption line accurately requires high-resolution spectroscopy, ideally with a resolving power 10,000 to avoid contamination from otherwise blended spectral lines such as Fe I (Xing, 2010). Such measurements require long exposure times and they have thus typically only been obtained for known populations of nearby associations or open clusters. However, a literature search revealed that Li I equivalent width measurements have been obtained by Magazzù et al. (1997) for nine members or candidate members (and one low-likelihood candidate) of MUTA in a follow-up of ROSAT X-ray bright sources (Neuhaeuser et al., 1995) in the vicinity of Taurus-Auriga. These measurements were obtained at a relatively low resolving power ( 8,400),121212Magazzù et al. (1997) also obtained measurements at 4200, but inspecting the Isaac Newton Group Archive at http://casu.ast.cam.ac.uk/casuadc/ingarch/query indicated that none of these lower-resolution observations have been obtained for MUTA objects. meaning that the equivalent widths may be slightly overestimated because of line blending. We obtained effective temperatures for these ten stars from Xing (2010), Gaia Collaboration et al. (2018b) and Bai et al. (2019), where available, listed in Table 6.5 along with the lithium equivalent width measurements of Magazzù et al. (1997).
In Figure 22, we compare these available MUTA temperature versus lithium measurements with other literature data for stellar populations across a range of ages. The 20–25 Myr sequence was built from the Pictoris moving group (PMG, e.g., see Zuckerman et al., 2001a; Zuckerman & Song, 2004; Bell et al., 2015, measurements are from Mentuch et al., 2008; Malo et al., 2014b; Shkolnik et al., 2017). The 40–50 Myr sequence was built from the stellar populations of the Tucana-Horologium association discussed earlier (lithium equivalent width measurements are by Kraus et al. 2014) and the IC 2602 and IC 2391 open clusters (Randich, 2001; Barrado y Navascués et al., 2004; Dobbie et al., 2010). The 110–125 Myr sequence was built from the Pleiades association (Soderblom et al., 1993; Jones et al., 1996; Bouvier et al., 2018), and the 150–175 Myr was built from the M35 open cluster (Barrado y Navascués et al., 2001; Bouy et al., 2015).
MUTA | Common | ROSAT | EW(Li) | ||
---|---|---|---|---|---|
ID | Name | Name | (mÅ) | (K) | Ref. |
24 | RX J0348.5+0832 | RX J0348.5+0832 | 260 | 5409 | 2 |
27 | RX J0338.3+1020 | RX J0338.3+1020 | 250 | 5250 | 2 |
29 | RX J0358.2+0932 | RX J0358.1+0932 | 200 | 4855 | 1 |
94 | V1267 Tau | RX J0333.1+1036 | 320 | 4967 | 1 |
159 | TYC 71–542–1 | RX J0347.9+0616 | 200 | 5794 | 2 |
195 | 2MASS J03545074+1232061 | RX J0354.8+1232 | 0 | 4028 | 3 |
318 A | 2MASS J04341953+0226260 | RX J0434.3+0226 | 300 | 4714 | 1 |
350 | TYC 91–702–1 | RX J0442.9+0400 | 220 | 5247 | 2 |
362 | V1831 Ori | RX J0450.0+0151 | 350 | 5247 | 1 |
376 | TYC 665–150–1 | RX J0357.3+1258 | 250 | 5943 | 2 |
Although the available MUTA measurements do not span either of the lithium depletion boundaries, they seem consistent with an age in the range 20–125 Myr, with the caveat that our comparison sequences were built from higher-resolution spectra compared with MUTA measurements. This likely biases our range slightly towards young ages, but this result seems consistent with our previous age assessments based on empirical isochrones and white dwarf cooling ages. Obtaining higher-resolution optical spectra for MUTA members, as well as extending the range of spectral types over which lithium equivalent widths are measured, will allow us to further constrain the age of MUTA.




6.6 Present-Day Mass Function
We used the empirically corrected MIST solar-metallicity model isochrones of Choi et al. (2016) as described by Gagné et al. (2018a)131313We used the models based on the revised Gaia DR2 photometric zero points of Evans et al. (2018a) available at http://waps.cfa.harvard.edu/MIST/model_grids.html with a nominal stellar rotation of to estimate the masses of MUTA members and candidates based on their position in a Gaia DR2 absolute versus color-magnitude diagram. This method uses the differences between the empirical Pleiades sequence and the 112 Myr MIST isochrone to correct for systematic effects such as the increased stellar activity and strong magnetic fields of low-mass stars.
The masses for MUTA candidates with very red colors () were estimated with the method of Gagné et al. (2014), which is more reliable than extrapolating MIST isochrones or using lower quality Gaia DR2 photometry, but potentially suffers from different systematics. The method is based on a comparison of the absolute 2MASS , , and WISE and photometry of MUTA candidates with BT-Settl models (Allard et al., 2012) in the same respective bandpasses, and combining the individual estimates in a likelihood analysis. These model-dependent mass estimates range from 35 to 0.2 , covering the substellar-to-stellar transition and overlapping slightly with the range of masses (0.1–6.0 ) obtained with MIST isochrones for bluer targets.
The resulting present-day mass function of MUTA members and candidates is displayed in Figure 23 along with a fiducial log-normal mass function ( dex, ). We fitted its amplitude to our MUTA members with masses above 1 , but the width and central position were not fitted. This particular mass function was shown to be a good fit to other nearby young associations by Jeffries (2012). The log-normal mass function is a good match to our distribution of MUTA members and candidates down to 0.1 , indicating that its present-day mass function may be similar to other young associations of the Solar neighborhood. Assuming that the population of MUTA is complete above 0.2 indicates that about 65 brown dwarf members would remain to be found, for a total stellar and substellar population of 450 members.

6.7 Stellar Rotation and Activity
Young stars lose angular momentum as they age, and their rotation periods consequently slow down with time. Because the rate of angular momentum loss depends on the rotation period, members of stellar associations with a wide range of rotation periods will eventually converge to a tight sequence as a function of their mass (Barnes, 2003; van Saders et al., 2016). The timescale for this convergence for Sun-like stars is Myr and decreases with increasing stellar mass (Delorme et al., 2011; Douglas et al., 2016; Curtis et al., 2019), but a partial sequence is apparent even at 112 Myr for higher-mass stars (Rebull et al., 2016).
Depending on the mass, this trend of longer rotation periods for older ages reverses for the youngest (pre-main-sequence) stars, as they spin up while contracting onto the main sequence. The youngest stars therefore also have longer rotation periods. The scatter at these younger ages is also larger because of a large spread in the initial rotation periods. Thus, the rotation period versus color sequence of MUTA can still be used as an additional test of our assigned age by comparing with similarly-aged groups.
As bounds for the expected age of MUTA, we used members the Pleiades (112 Myr; Dahm, 2015) and Praesepe clusters ( 800 Myr; Brandt & Huang 2015), in addition to members of the Columba, Carina, and Tucana-Horologium associations discussed earlier (45 Myr). We included the older Praesepe cluster as an example of a clearly older population in the color-rotation period diagram, because the differences between MUTA and the Pleiades are subtle. We collected the rotation period measurements of the Pleiades and Praesepe members from Rebull et al. (2016) and Douglas et al. (2017), respectively. We obtained light curves for each member of the younger three associations from the TESS or K2 missions, where available. We restricted our sample to targets with Gaia DR2 , as the variability period in bluer stars may be impacted by pulsations as much as rotation. For those observed by K2 (16 stars), we used K2SFF processed light curves (Vanderburg & Johnson, 2014). For TESS targets with short-cadence data, we used light curves from the Science Processing Operations Center (SPOC, Jenkins et al., 2016) and for others we extracted light curves from the full-frame images using Eleanor141414https://github.com/afeinstein20/eleanor (Feinstein et al., 2019). We excluded targets with flux contamination ratios above 1, even when rotation consistent with youth was present in the curve.
R.A. | Decl. | Period 1 | Period 2aaSecond rotation period candidate. | Young | ||
---|---|---|---|---|---|---|
Name | (hh:mm:ss.sss) | (dd:mm:ss.ss) | (days) | (days) | AssociationbbThe full names of young associations are: Carina (CAR), Columba (COL), the Tucana-Horologium association (THA) and the Tau Association (MUTA). | Source |
2MASS J03303685+1610599 | 03:30:36.887 | +16:10:59.58 | 1.70 | MUTA | 2 | |
2MASS J03350134+1418016 | 03:35:01.376 | +14:18:01.14 | 4.38 | MUTA | 2 | |
2MASS J03361762+2153391 | 03:36:17.665 | +21:53:38.50 | 4.38 | MUTA | 2 | |
2MASS J03371337+1307315 | 03:37:13.411 | +13:07:30.93 | 0.66 | MUTA | 2 | |
2MASS J03373508+1705162 | 03:37:35.111 | +17:05:15.93 | 6.19 | MUTA | 2 | |
RX J0338.3+1020 | 03:38:18.266 | +10:20:16.32 | 3.24 | MUTA | 1 | |
2MASS J03385230+1635406 | 03:38:52.328 | +16:35:40.21 | 0.34 | MUTA | 2 | |
TYC 1235–156–1 | 03:39:39.516 | +15:29:54.47 | 4.43 | MUTA | 2 | |
TYC 663–362–1 | 03:40:57.781 | +13:09:03.06 | 2.59 | MUTA | 1 | |
TYC 660–135–1 | 03:41:45.000 | +10:54:27.46 | 5.12 | MUTA | 1 | |
2MASS J03420359+1631392 | 03:42:03.617 | +16:31:38.80 | 4.92 | MUTA | 2 | |
HD 23376 | 03:44:58.957 | +08:19:10.09 | 0.81 | MUTA | 1 | |
BD+04 589 | 03:47:13.551 | +05:26:23.49 | 4.75 | MUTA | 1 | |
TYC 1252–301–1 | 03:47:23.901 | +18:43:17.68 | 4.09 | MUTA | 2 | |
BD+07 543 | 03:47:31.345 | +07:57:26.39 | 3.57 | MUTA | 1 | |
TYC 661–560–1 | 03:47:53.694 | +11:48:57.98 | 1.55 | MUTA | 1 | |
RX J0348.5+0832 | 03:48:31.461 | +08:31:36.43 | 0.41 | MUTA | 1 | |
EPIC 210811401 | 03:48:50.333 | +20:02:27.56 | 5.10 | MUTA | 2 | |
2MASS J03495031+1440552 | 03:49:50.345 | +14:40:54.73 | 1.02 | MUTA | 2 | |
PPM 119410 | 03:50:50.558 | +11:00:05.12 | 1.80 | MUTA | 1 | |
2MASS J03511041+1302467 | 03:51:10.454 | +13:02:46.16 | 2.54 | MUTA | 1 | |
EPIC 210361663 | 03:54:50.776 | +12:32:05.61 | 3.26 | MUTA | 2 | |
HD 286374 | 03:56:19.224 | +11:25:10.84 | 1.57 | MUTA | 2 | |
HD 286380 | 03:56:20.741 | +10:47:47.24 | 2.51 | MUTA | 1 | |
TYC 665–150–1 | 03:57:21.412 | +12:58:16.37 | 0.86 | MUTA | 2 | |
2MASS J03573875+1142322 | 03:57:38.786 | +11:42:31.85 | 3.92 | MUTA | 2 | |
RX J0358.2+0932 | 03:58:12.749 | +09:32:21.97 | 1.44 | MUTA | 1 | |
TYC 662–217–1 | 03:59:42.158 | +12:10:08.14 | 4.80 | MUTA | 2 | |
2MASS J04072953–0115000 | 04:07:29.559 | –01:15:00.13 | 1.04 | MUTA | 1 | |
TYC 74–1393–1 | 04:12:18.449 | +00:01:31.28 | 2.94 | MUTA | 1 | |
2MASS J04210781–0111328 | 04:21:07.848 | –01:11:33.15 | 4.29 | MUTA | 1 | |
TYC 668–737–1 | 04:21:24.386 | +08:53:54.34 | 5.31 | MUTA | 1 | |
BD–03 753 | 04:22:23.528 | –02:40:04.13 | 0.90 | MUTA | 1 | |
HD 27687 | 04:22:24.213 | +06:31:45.14 | 0.53 | 0.39 | MUTA | 1 |
BD+05 638 | 04:22:33.022 | +05:41:38.82 | 3.37 | 6.32 | MUTA | 1 |
HD 28356 | 04:28:32.733 | +06:05:52.07 | 0.81 | MUTA | 1 | |
BD–03 789 | 04:28:37.716 | –03:15:44.58 | 1.72 | MUTA | 1 | |
2MASS J04372578–0210117 | 04:37:25.800 | –02:10:12.12 | 1.13 | MUTA | 1 | |
2MASS J04372971–0051241 | 04:37:29.730 | –00:51:24.47 | 3.59 | MUTA | 1 | |
2MASS J04391308–0045039 | 04:39:13.102 | –00:45:04.39 | 0.42 | MUTA | 1 | |
BD+06 731 | 04:39:15.500 | +07:01:43.92 | 6.08 | 8.66 | MUTA | 1 |
TYC 4739–1225–1 | 04:39:20.251 | –03:14:21.79 | 3.61 | MUTA | 1 | |
BD–02 1047 | 04:52:07.364 | –01:58:57.43 | 1.47 | 0.69 | MUTA | 1 |
TYC 4741–307–1 | 04:56:18.287 | –01:53:33.04 | 2.44 | MUTA | 1 | |
HD 37402 | 05:34:26.201 | –60:06:14.58 | 1.93 | CAR | 1 | |
HD 42270 | 05:53:29.503 | –81:56:52.20 | 1.87 | CAR | 1 | |
HD 43199 | 06:10:52.922 | –61:29:58.79 | 0.52 | CAR | 1 | |
AL 442 | 06:11:30.043 | –72:13:37.79 | 0.85 | CAR | 1 | |
AB Pic | 06:19:12.941 | –58:03:14.83 | 3.81 | CAR | 1 | |
HIP 32235 | 06:43:46.270 | –71:58:34.45 | 3.94 | CAR | 1 | |
HIP 33737 | 07:00:30.501 | –79:41:45.06 | 5.21 | CAR | 1 | |
2MASS J07013884–6236059 | 07:01:38.844 | –62:36:05.98 | 3.93 | 5.58 | CAR | 1 |
2MASS J07065772–5353463 | 07:06:57.714 | –53:53:45.75 | 2.87 | CAR | 1 | |
2MASS J08040534–6316396 | 08:04:05.300 | –63:16:39.11 | 2.01 | CAR | 1 | |
2MASS J08194309–7401232 | 08:19:43.099 | –74:01:23.22 | 0.42 | CAR | 1 | |
2MASS J09032434–6348330 | 09:03:24.265 | –63:48:32.65 | 4.42 | CAR | 1 | |
2MASS J09180165–5452332 | 09:18:01.547 | –54:52:32.85 | 0.37 | CAR | 1 | |
HIP 46063 | 09:23:34.921 | –61:11:35.61 | 3.92 | CAR | 1 | |
2MASS J09315840–6209258 | 09:31:58.328 | –62:09:25.46 | 1.93 | CAR | 1 | |
TWA 21 | 10:13:14.666 | –52:30:53.85 | 4.43 | CAR | 1 | |
HD 14691 | 02:22:01.693 | –10:46:40.40 | 0.46 | COL | 1 | |
2MASS J03083950–3844363 | 03:08:39.597 | –38:44:36.32 | 0.69 | COL | 1 | |
2MASS J03320347–5139550 | 03:32:03.559 | –51:39:54.87 | 5.56 | COL | 1 | |
HIP 17248 | 03:41:37.453 | +55:13:05.02 | 4.70 | COL | 1 | |
2MASS J04091413–4008019 | 04:09:14.199 | –40:08:01.98 | 3.28 | COL | 1 | |
HIP 19775 | 04:14:22.624 | –38:19:01.54 | 1.74 | COL | 1 | |
CD–36 1785 | 04:34:50.821 | –35:47:21.13 | 2.31 | COL | 1 | |
HD 29329 | 04:46:00.914 | +76:36:37.66 | 0.92 | COL | 1 | |
HIP 22226 | 04:46:49.568 | –26:18:08.93 | 0.89 | COL | 1 | |
HD 31242 | 04:51:53.585 | –46:47:13.11 | 3.01 | COL | 1 | |
HD 272836 | 04:53:05.246 | –48:44:38.49 | 4.60 | COL | 1 | |
HIP 23316 | 05:00:51.910 | –41:01:06.56 | 2.29 | COL | 1 | |
2MASS J05195695–1124440 | 05:19:56.985 | –11:24:44.48 | 4.38 | COL | 1 | |
2MASS J05241317–2104427 | 05:24:13.213 | –21:04:43.14 | 4.17 | COL | 1 | |
HIP 25709 | 05:29:24.132 | –34:30:55.43 | 6.14 | 2.75 | COL | 1 |
AH Lep | 05:34:09.189 | –15:17:03.54 | 2.10 | COL | 1 | |
HD 37484 | 05:37:39.655 | –28:37:34.70 | 0.82 | COL | 1 | |
2MASS J05395494–1307598 | 05:39:54.968 | –13:08:00.11 | 1.89 | COL | 1 | |
AI Lep | 05:40:20.753 | –19:40:11.12 | 1.69 | COL | 1 | |
HD 38397 | 05:43:35.843 | –39:55:24.50 | 2.27 | COL | 1 | |
HIP 28036 | 05:55:43.189 | –38:06:16.10 | 0.95 | COL | 1 | |
HD 41071 | 06:00:41.325 | –44:53:49.75 | 5.46 | COL | 1 | |
HIP 30030 | 06:19:08.069 | –03:26:21.01 | 1.36 | COL | 1 | |
CD–40 2458 | 06:26:06.918 | –41:02:53.59 | 4.21 | COL | 1 | |
HIP 490 | 00:05:52.680 | –41:45:12.23 | 3.00 | THA | 1 | |
2MASS J00125703–7952073 | 00:12:57.525 | –79:52:08.03 | 0.99 | THA | 1 | |
HIP 1113 | 00:13:53.335 | –74:41:18.61 | 3.62 | THA | 1 | |
2MASS J00144767–6003477 | 00:14:47.860 | –60:03:48.67 | 0.49 | THA | 1 | |
2MASS J00152752–6414545 | 00:15:27.705 | –64:14:55.61 | 3.69 | THA | 1 | |
GJ 3017 | 00:15:36.842 | –29:46:01.77 | 0.84 | THA | 1 | |
HIP 1481 | 00:18:26.332 | –63:28:39.90 | 2.31 | 2.59 | THA | 1 |
2MASS J00235732–5531435 | 00:23:57.506 | –55:31:44.58 | 2.44 | 2.99 | THA | 1 |
HIP 1993 | 00:25:14.853 | –61:30:49.12 | 4.37 | THA | 1 | |
UPM J0027–6157 | 00:27:33.500 | –61:57:17.79 | 0.55 | THA | 1 | |
2MASS J00284683–6751446 | 00:28:47.106 | –67:51:45.46 | 0.33 | THA | 1 | |
2MASS J00332438–5116433 | 00:33:24.551 | –51:16:44.33 | 0.35 | THA | 1 | |
HIP 2729 | 00:34:51.397 | –61:54:58.95 | 0.38 | THA | 1 | |
2MASS J00393579–3816584 | 00:39:35.930 | –38:16:59.55 | 6.41 | THA | 1 | |
2MASS J00394063–6224125 | 00:39:40.905 | –62:24:13.39 | 0.38 | THA | 1 | |
UPM J0042–5444 | 00:42:10.272 | –54:44:44.09 | 1.78 | THA | 1 | |
CD–78 24 | 00:42:20.705 | –77:47:40.20 | 2.59 | THA | 1 | |
2MASS J00425349–6117384 | 00:42:53.702 | –61:17:39.23 | 1.04 | THA | 1 | |
HIP 3556 | 00:45:28.320 | –51:37:34.85 | 5.97 | 9.13 | THA | 1 |
2MASS J00485254–6526330 | 00:48:52.746 | –65:26:33.71 | 1.01 | THA | 1 | |
2MASS J00493566–6347416 | 00:49:35.887 | –63:47:42.33 | 4.95 | THA | 1 | |
UPM J0113–5939 | 01:13:40.523 | –59:39:35.06 | 0.32 | THA | 1 | |
2MASS J01180670–6258591 | 01:18:06.926 | –62:58:59.85 | 0.35 | THA | 1 | |
2MASS J01211297–6117281 | 01:21:13.152 | –61:17:28.86 | 0.43 | THA | 1 | |
CD–34 521 | 01:22:04.571 | –33:37:04.47 | 9.61 | THA | 1 | |
UPM J0122–6318 | 01:22:45.334 | –63:18:45.24 | 0.46 | THA | 1 | |
HIP 6485 | 01:23:21.433 | –57:28:51.25 | 3.47 | THA | 1 | |
2MASS J01233280–4113110 | 01:23:32.961 | –41:13:11.76 | 0.74 | THA | 1 | |
2MASS J01275875–6032243 | 01:27:58.956 | –60:32:24.76 | 0.34 | THA | 1 | |
HIP 6856 | 01:28:08.842 | –52:38:19.81 | 6.36 | THA | 1 | |
2MASS J01375879–5645447 | 01:37:58.967 | –56:45:45.33 | 0.71 | THA | 1 | |
HD 10863 | 01:46:01.170 | –27:20:56.49 | 0.44 | THA | 1 | |
2MASS J01504543–5716488 | 01:50:45.620 | –57:16:49.23 | 0.71 | THA | 1 | |
2MASS J01505688–5844032 | 01:50:57.087 | –58:44:03.63 | 1.65 | THA | 1 | |
2MASS J01532494–6833226 | 01:53:25.212 | –68:33:22.92 | 0.60 | THA | 1 | |
HIP 9141 | 01:57:49.093 | –21:54:06.12 | 3.04 | THA | 1 | |
2MASS J02001992–6614017 | 02:00:20.178 | –66:14:02.14 | 0.63 | THA | 1 | |
HIP 9685 | 02:04:35.299 | –54:52:54.45 | 0.44 | THA | 1 | |
2MASS J02045317–5346162 | 02:04:53.332 | –53:46:16.75 | 0.70 | THA | 1 | |
UCAC3 92–4597 | 02:07:01.904 | –44:06:38.51 | 0.39 | 3.00 | THA | 1 |
HIP 9892 | 02:07:18.209 | –53:11:56.88 | 2.39 | THA | 1 | |
HIP 9902 | 02:07:26.315 | –59:40:46.23 | 1.71 | THA | 1 | |
2MASS J02125819–5851182 | 02:12:58.366 | –58:51:18.42 | 1.60 | THA | 1 | |
2MASS J02205139–5823411 | 02:20:51.580 | –58:23:41.37 | 1.28 | THA | 1 | |
2MASS J02242453–7033211 | 02:24:24.829 | –70:33:21.25 | 0.52 | THA | 1 | |
2MASS J02294869–6906044 | 02:29:48.952 | –69:06:04.36 | 0.46 | THA | 1 | |
2MASS J02321934–5746117 | 02:32:19.520 | –57:46:11.93 | 0.86 | THA | 1 | |
UPM J0234–5128 | 02:34:18.835 | –51:28:46.44 | 0.46 | THA | 1 | |
2MASS J02383255–7528065 | 02:38:32.880 | –75:28:06.41 | 0.63 | THA | 1 | |
CD–53 544 | 02:41:47.002 | –52:59:52.61 | 0.52 | THA | 1 | |
2MASS J02420204–5359147 | 02:42:02.231 | –53:59:14.88 | 0.57 | 2.47 | THA | 1 |
2MASS J02420404–5359000 | 02:42:04.237 | –53:59:00.22 | 0.57 | THA | 1 | |
CD–58 553 | 02:42:33.187 | –57:39:36.95 | 7.40 | THA | 1 | |
HD 17250 | 02:46:14.687 | +05:35:32.64 | 1.21 | THA | 1 | |
2MASS J02474639–5804272 | 02:47:46.569 | –58:04:27.47 | 9.45 | THA | 1 | |
2MASS J02502222–6545552 | 02:50:22.440 | –65:45:55.27 | 1.29 | THA | 1 | |
2MASS J02523550–7831183 | 02:52:35.919 | –78:31:18.08 | 0.71 | THA | 1 | |
2MASS J02553178–5702522 | 02:55:31.954 | –57:02:52.41 | 0.49 | THA | 1 | |
2MASS J03050556–5317182 | 03:05:05.712 | –53:17:18.46 | 0.44 | THA | 1 | |
2MASS J03104941–3616471 | 03:10:49.532 | –36:16:47.39 | 0.66 | THA | 1 | |
2MASS J03114544–4719501 | 03:11:45.581 | –47:19:50.27 | 4.81 | THA | 1 | |
HIP 15247 | 03:16:40.753 | –03:31:49.69 | 1.03 | THA | 1 | |
2MASS J03244056–3904227 | 03:24:40.680 | –39:04:22.95 | 0.34 | 8.05 | THA | 1 |
2MASS J03291649–3702502 | 03:29:16.628 | –37:02:50.37 | 0.54 | THA | 1 | |
CD–46 1064 | 03:30:49.233 | –45:55:57.44 | 3.92 | THA | 1 | |
CD–44 1173 | 03:31:55.768 | –43:59:13.61 | 2.93 | THA | 1 | |
2MASS J03454058–7509121 | 03:45:40.854 | –75:09:11.91 | 0.70 | THA | 1 | |
HD 24636 | 03:48:11.720 | –74:41:38.44 | 5.72 | 0.84 | THA | 1 |
2MASS J03512287–5154582 | 03:51:23.001 | –51:54:58.01 | 0.43 | THA | 1 | |
HD 25284 | 04:00:03.918 | –29:02:16.64 | 0.31 | 2.27 | THA | 1 |
HD 25402 | 04:00:32.079 | –41:44:54.40 | 3.56 | THA | 1 | |
2MASS J04013874–3127472 | 04:01:38.846 | –31:27:47.35 | 0.46 | THA | 1 | |
BD–15 705 | 04:02:16.556 | –15:21:30.22 | 3.85 | THA | 1 | |
2MASS J04074372–6825111 | 04:07:43.905 | –68:25:10.85 | 1.02 | THA | 1 | |
2MASS J04133609–4413325 | 04:13:36.194 | –44:13:32.40 | 0.78 | THA | 1 | |
WOH S 6 | 04:21:39.275 | –72:33:55.53 | 4.55 | THA | 1 | |
2MASS J04274963–3327010 | 04:27:49.718 | –33:27:01.17 | 0.67 | THA | 1 | |
HIP 21632 | 04:38:44.007 | –27:02:01.97 | 2.40 | THA | 1 | |
2MASS J04435860–3643188 | 04:43:58.683 | –36:43:18.81 | 1.61 | THA | 1 | |
2MASS J04440099–6624036 | 04:44:01.138 | –66:24:03.15 | 7.94 | THA | 1 | |
2MASS J04470041–5134405 | 04:47:00.509 | –51:34:40.23 | 6.25 | THA | 1 | |
TYC 8083–45–5 | 04:48:00.760 | –50:41:25.40 | 8.13 | THA | 1 | |
HIP 22295 | 04:48:05.485 | –80:46:44.64 | 1.24 | THA | 1 | |
CD–30 2310 | 05:18:29.092 | –30:01:32.16 | 1.70 | THA | 1 | |
TYC 8098–414–1 | 05:33:25.647 | –51:17:12.77 | 5.21 | THA | 1 | |
HIP 32435 | 06:46:13.720 | –83:59:28.55 | 1.59 | THA | 1 | |
HIP 84642 | 17:18:14.645 | –60:27:27.57 | 4.17 | THA | 1 | |
2MASS J19225071–6310581 | 19:22:50.700 | –63:10:59.23 | 0.86 | THA | 1 | |
2MASS J20291446–5456116 | 20:29:14.491 | –54:56:13.29 | 0.88 | THA | 1 | |
2MASS J21100614–5811483 | 21:10:06.195 | –58:11:49.78 | 0.56 | THA | 1 | |
2MASS J21163528–6005124 | 21:16:35.368 | –60:05:14.13 | 0.99 | THA | 1 | |
HIP 105388 | 21:20:50.012 | –53:02:04.64 | 3.45 | THA | 1 | |
UPM J2127–6841 | 21:27:50.634 | –68:41:04.64 | 0.34 | THA | 1 | |
2MASS J21370885–6036054 | 21:37:08.927 | –60:36:07.04 | 2.00 | THA | 1 | |
2MASS J21380269–5744583 | 21:38:02.765 | –57:44:59.89 | 0.68 | THA | 1 | |
HIP 107345 | 21:44:30.211 | –60:58:40.34 | 4.53 | THA | 1 | |
2MASS J21504048–5113380 | 21:50:40.563 | –51:13:39.59 | 1.05 | THA | 1 | |
HIP 107947 | 21:52:09.822 | –62:03:09.92 | 0.96 | THA | 1 | |
2MASS J22021626–4210329 | 22:02:16.331 | –42:10:34.73 | 4.51 | THA | 1 | |
2MASS J22025453–6440441 | 22:02:54.624 | –64:40:45.70 | 0.43 | THA | 1 | |
UPM J2222–6303 | 22:22:39.816 | –63:03:27.22 | 1.11 | THA | 1 | |
2MASS J22244102–7724036 | 22:24:41.287 | –77:24:04.82 | 0.67 | THA | 1 | |
2MASS J22444835–6650032 | 22:44:48.534 | –66:50:04.47 | 0.73 | THA | 1 | |
2MASS J22463471–7353504 | 22:46:34.912 | –73:53:51.52 | 1.65 | THA | 1 | |
2MASS J23131671–4933154 | 23:13:16.833 | –49:33:16.85 | 1.23 | THA | 1 | |
2MASS J23170011–7432095 | 23:17:00.401 | –74:32:10.53 | 0.83 | THA | 1 | |
TYC 9344–293–1 | 23:26:10.958 | –73:23:50.88 | 0.57 | THA | 1 | |
2MASS J23273447–8512364 | 23:27:35.285 | –85:12:37.17 | 0.90 | THA | 1 | |
CD–86 147 | 23:27:50.213 | –86:13:19.36 | 0.70 | THA | 1 | |
2MASS J23285763–6802338 | 23:28:57.841 | –68:02:35.08 | 0.37 | THA | 1 | |
2MASS J23291752–6749598 | 23:29:17.728 | –67:50:01.14 | 1.02 | THA | 1 | |
2MASS J23382851–6749025 | 23:38:28.714 | –67:49:03.52 | 0.44 | THA | 1 | |
HIP 116748 | 23:39:39.712 | –69:11:45.75 | 2.86 | THA | 1 | |
2MASS J23424333–6224564 | 23:42:43.528 | –62:24:57.60 | 0.52 | THA | 1 | |
2MASS J23452225–7126505 | 23:45:22.521 | –71:26:51.46 | 1.61 | THA | 1 | |
2MASS J23474694–6517249 | 23:47:47.152 | –65:17:25.79 | 4.84 | THA | 1 | |
2MASS J23524562–5229593 | 23:52:45.779 | –52:30:00.51 | 0.91 | THA | 1 |
Note. — Rotation periods are accurate to approximately 2%. Only a portion of the table is shown here. The full table is available as online-only additional material. See Section 6.7 for more details.
We estimated the rotation periods for each star using two methods: a modified version of the Lomb-Scargle periodogram as described in Horne & Baliunas (1986), and the autocorrelation function as described in McQuillan et al. (2013). In both cases, we searched for periodic signals down to twice the Nyquist-sampling limit, and as long as a third of the total data coverage. Below the lower limit, we found that both algorithms are biased by the data sampling, particularly for long-cadence (30 min) data. We set the lower limit for a significant detection at three full rotations. We then flagged the peak in the periodogram and the second peak in the autocorrelation function as the likely period (see Figure 24 for an example). We only considered periodic signals with false-alarm probabilities % and for which autocorrelation and Lomb-Scargle periods agreed within 10%. For six stars, the autocorrelation and Lomb-Scargle disagreed by an integer factor (alias), which we retained, provided the true rotation period was clear. Across all clusters, 14 out of 201 stars showed evidence of a second period, which we excluded from our sample as they are likely binaries (Douglas et al., 2017). As a final check, we visually inspected all phased light curves.
We created synthetic data sets, with random subsamples of half the data and each point perturbed by a random number following the measurement errors, to investigate the accuracy of our period determinations. We found that, when the correct period is identified, our assigned periods are accurate within 2%, with a fail rate of 5% where the measured period is wrong by 20% or more (usually off by an integer multiple). This assumes that all detected periods are associated with stellar rotation and not other phenomena. Periodic signals caused by binary systems, pulsations or flares could cause further false positives, if they passed our visual inspection.

The resulting rotation periods are shown in Figure 25 and listed in Table 6.7. While there is significant scatter in the sequence, Praesepe and Pleiades members have the longest typical rotation period at , while members of young moving groups have the shortest periods, and MUTA members are located in between. On the cool end (), Pleiades rotations are the fastest, as the 45 Myr stars are still contracting, although we have fewer period measurements in MUTA in this regime. The overall trend is consistent with our assigned Myr age of MUTA based on empirical isochrones and the total age of the white dwarf WD 0340+103, though additional rotation period measurements would be useful to better map out its sequence.

Stellar rotation serves as a driver of magnetic activity through the dynamo effect (Reiners et al., 2012), and causes young stars to display enhanced UV and X-ray emission among other effects associated with an enhanced stellar activity (Kastner et al., 2003; Rodriguez et al., 2013; Malo et al., 2014a). We used data from the ROSAT all-sky survey (Boller et al., 2016) and the GALEX catalog (Martin et al., 2005) to verify that our population of MUTA members and candidates display this expected enhanced activity in a way that is consistent with other young asociations of similar ages ( 10–150 Myr) in the Solar neighborood, including PMG and the AB Doradus moving group (ABDMG, Zuckerman et al. 2004; see Gagné et al. 2018 for a discussion of these associations). The resulting distributions are shown in Figures 26 and 27, and provide more evidence that MUTA consists of a coeval and young association.


6.8 Tau in the Context of the Galactic Structure
An unprecedented view of the local spatial and kinematic structure of the Galaxy was enabled with the advent of Gaia DR2. Using these new data, Kounkel & Covey (2019) identified 1,901 groups of stars that appear co-moving and coeval, located within 30° of the Galactic plane and 1 kpc of the Sun. Their method used the HDBSCAN unsupervised clustering algorithm151515See https://hdbscan.readthedocs.io. directly in the 5-dimensional parameter space of Gaia DR2 observables (sky position, proper motion and parallax) to identify over-densities; this did not allow them to efficiently recover the structure within about 70 pc of the Sun because the large spread of nearby associations on the sky introduces strong variation and correlations in the Gaia DR2 5-dimensional kinematic space of the members within a specific young association. Kounkel & Covey (2019) separated the over-densities among clusters and strings, the latter consisting of much larger structures with typical physical sizes of about 200 pc and some of which also have extended kinematic distributions.
We cross-matched our sample of MUTA candidates and members with the full Kounkel & Covey (2019) catalog of clustered sources to determine whether MUTA had been recovered by their study. We found a total of 72 matches with our list, all with a single Kounkel & Covey (2019) string named Theia 160 that contains a total of 300 stars. Only 4 of these stars are matches to our initial list of MUTA members (HD 28715, HD 27687, HD 28356, and TYC 668–737–1; respectively, MUTA 11, 17, 18, and 30 A). One likely explanation for the partial overlap is the ° cut-off in Galactic latitude that they imposed, as approximately half of MUTA falls at °. We show a comparison of Theia 160, MUTA and Taurus in Figure 28. Theia 160 is spatially more extended, but also shows a much larger spread in space velocities compared with MUTA, although they are centered at similar average velocities; MUTA members have a spread of (2.8, 2.1, 1.6) km s-1 in space, whereas the spread of Theia 160 members is (21.1, 1.7, 8.9) km s-1. This indicates that some interlopers may contaminate the sample of Theia 160 stars, and further investigation will be required to confirm this.
In addition to the similar kinematics between MUTA and Theia 160, Kounkel & Covey (2019) determined a model-dependent isochronal age of 80 Myr for Theia 160, which is close to our estimated age of Myr. It seems likely that MUTA and Theia 160 are related to each other; perhaps Theia 160 represents a stream or tidal tail around the more closely packed core of MUTA (analoguous to the tidal tail around the Hyades cluster although the latter is much older; Röser et al. 2019), or it is simply a fragment of MUTA with some contaminating field stars that have more spread-out space velocities. Investigating this further will require a spectroscopic follow-up of candidates in both MUTA and Theia 160 to complete the measurements of all members in both groups–although the next data release of the Gaia DR2 mission will likely allow to complete the velocities of most MUTA members,–and determine spectroscopic signs of young ages. It is possible that our method did not recover the full spatial structure of MUTA, especially regions that would lack massive stars, because BANYAN requires an initial kinematic model to work with, which we obtained from the initial collection of young or active stars described in Section 2. In addition to this, Kounkel & Covey (2019) uncovered a large kinematic structure (Theia 133) that encompasses the Persei cluster, likely related to Cas-Tau and MUTA, as discussed in Section 2. This structure is also shown in Figure 28.
Liu et al. (2020) recently published the discovery of two new associations physically nearby (but unrelated to) the Taurus-Auriga star-forming region; e Tau and u Tau. The group that they identified as e Tau has significant overlap with our definition of MUTA; 104 of their 119 members are in also in our list (18 in our initial members, 79 in our candidate members, 6 in our low-likelihood candidate members, and 1 in our list of rejected members). The 15 remaining objects not in our catalogs that they list as e Tau members either have a Bayesian membership probability below 90% or a best-case scenario separation above 5 km s-1 with our kinematic model, which explains why we have not recovered them. We identified in this paper a total of 444 candidate members that Liu et al. (2020) did not discuss: 18 in our initial members, 277 candidate members and 149 in our low-likelihood candidate members. An additional 12 objects in our MUTA lists (4 initial members, 6 candidate members and 2 low-likelihood candidates) are listed as u Tau members by Liu et al. (2020). The isochrone age of 50 Myr determined by Liu et al. (2020) is similar to our Myr, but is based on model isochrones rather than empirical ones.
The fact that Kounkel & Covey (2019) and Liu et al. (2020) may have uncovered spatial extensions of MUTA, and the presence of a large structure of additional stars coeval with MUTA and Persei hints that it would be valuable to parse the local Solar neighborood with an overdensity detection algorithm that is not hindered by the lack of radial velocity measurements or the large spread and correlations of sky positions, proper motions and parallaxes of nearby cluster members. Such a study would have the potential to uncover extended structures and connections between the Kounkel & Covey (2019) groups and the known nearby young associations in the Solar neighborhood, as well as new nearby associations entirely.
7 CONCLUSIONS
We presented and characterized the Tau Association, a young stellar population consisting of hundreds of members at about 150 pc from the Sun. We built a BANYAN spatial-kinematic model for this association to identify additional candidate members with Gaia DR2 and to allow other teams to search for new members. The Gaia DR2 photometry and parallaxes of MUTA members allowed us to make a comparison with empirical sequences of the Pleiades, Tucana-Horologium, Carina and Columba members to determine an isochronal age relative to these other young associations. This resulted in an age estimate of Myr for MUTA. We identified a white dwarf (WD 0340+103) that is the remnant of a B2 MUTA member that left its planetary nebula phase 270,000 years ago, and used its total age to further constrain the age of MUTA at Myr. We found literature measurements of the lithium equivalent width for K-type to G-type members of MUTA and showed that they are consistent with our age determination. The members of this new association have a Gaia DR2 colors versus TESS rotation periods sequence consistent with a young age, and display an enhanced level of stellar activity compared with the field population based on UV and X-ray, consistent with a young coeval population. We also showed that its present-day mass function is similar to other known young associations. MUTA is likely part of an extended network of stars coeval and co-moving with the Persei cluster that are currently dissolving. A master table with all candidates and members of the MUTA association is also provided here (Table 12).
The MUTA association is a new laboratory to study stellar and exoplanet evolution at an age which was not well sampled by other associations within the Solar neighborhood. Its distance of 150 pc will make it harder to identify its substellar population, but upcoming wide area surveys such as Pan-STARRS 3 (Magnier et al., 2010) and CatWISE (Eisenhardt et al., 2019) may be able to do so in the near future. The extended ROentgen Survey with an Imaging Telescope Array (eROSITA; Predehl et al. 2014) on the Spektrum-Roentgen-Gamma (SRG) space telescope will also likely allow us to better study the activity of the low-mass stars in MUTA.
Name | Units | Type | Format | Description |
---|---|---|---|---|
muta_id | char | a6 | Tau Association (MUTA) identification number. | |
main_name | char | a25 | Main target name. SIMBAD-resolvable names are preferred; short names in the format J0236+2026 are given otherwise. | |
gaiadr2_id | char | a25 | Gaia DR2 identification number. | |
tm_name | char | a25 | 2MASS designation. | |
aw_name | char | a25 | AllWISE designation. | |
rosat_name | char | a25 | ROSAT designation. | |
tyc_name | char | a25 | Tycho catalog designation. | |
hip_name | char | a25 | Hipparcos catalog designation. | |
simbad_id | char | a25 | Principal SIMBAD identifier. | |
spt | char | a10 |
Literature spectral type. Spectral type estimates based on Gaia DR2 colors are given between parentheses.
(WD) indicates likely white dwarfs. |
|
spt_ref | char | a25 | Reference for literature spectral type. | |
member_type | char | a2 |
Membership type. IM: Member from our initial list. CM: Candidate member. LM: Low-priority candidate member.
R: Rejected candidate member. |
|
source | char | a6 | Source from which the target was obtained. INIT: Initial list described in Section 2. GAIA: Originates from our Gaia DR2-based search for additional candidate members described in Section 4. COM: Originates from our comover search described in Section 4.1. VIS: Originates from our visual identification of comover candidates described in Section 4.5. OH2017: Originates from a Oh et al. (2017) group with a partial match to our MUTA members and candidates. | |
mem_prob | % | R*4 | f7.1 | BANYAN probability for membership in MUTA. |
uvw_sep | km s-1 | R*4 | f7.1 | Smallest possible separation from the center of the BANYAN model in space. |
xyz_sep | km s-1 | R*4 | f7.1 | Smallest possible separation from the center of the BANYAN model in space. |
ra | deg | R*8 | f21.16 | Gaia DR2 right ascension (J2000) at epoch 2015.5 in the ICRS reference frame. |
dec | deg | R*8 | f21.16 | Gaia DR2 declination (J2000) at epoch 2015.5 in the ICRS reference frame. |
pmra | R*4 | f10.5 | Gaia DR2 proper motion in right ascension, including the jacobian term. | |
pmdec | R*4 | f10.5 | Gaia DR2 proper motion in declination. | |
epmra | R*4 | f10.5 | Measurement error for Gaia DR2 proper motion in right ascension. | |
epmdec | R*4 | f10.5 | Measurement error for Gaia DR2 proper motion in declination. | |
plx | pc | R*4 | f10.5 | Gaia DR2 parallax. |
eplx | pc | R*4 | f10.5 | Measurement error for Gaia DR2 parallax. |
ruwe | R*4 | f7.1 | Re-normalised unit weight error of the Gaia DR2 astrometric solution. See Section 4.4 for more details. | |
rv | km s-1 | R*4 | f7.1 | Radial velocity measurement from the literature. |
erv | km s-1 | R*4 | f7.1 | Measurement error for radial velocity measurement. |
rv_ref | char | a25 | Reference for literature radial velocity measurement. | |
pred_rv | km s-1 | R*4 | f7.1 | Predicted radial velocity that maximizes MUTA membership probability obtained from BANYAN , only listed for targets without a radial velocity measurement. |
epred_rv | km s-1 | R*4 | f7.1 | confidence range on predicted radial velocity that maximizes MUTA membership probability. |
gaia_g | mag | R*8 | f12.5 | Gaia DR2 -band magnitude. |
egaia_g | mag | R*8 | f12.5 | Measurement error for Gaia DR2 -band magnitude. |
gaia_grp | mag | R*4 | f12.5 | Gaia DR2 -band magnitude. |
egaia_grp | mag | R*4 | f12.5 | Measurement error for Gaia DR2 -band magnitude. |
gaia_brp | mag | R*4 | f12.5 | Gaia DR2 -band magnitude. |
egaia_brp | mag | R*4 | f12.5 | Measurement error for Gaia DR2 -band magnitude. |
tmass_j | mag | R*4 | f10.3 | 2MASS -band magnitude. |
etmass_j | mag | R*4 | f10.3 | Measurement error for 2MASS -band magnitude. |
tmass_h | mag | R*4 | f10.3 | 2MASS -band magnitude. |
etmass_h | mag | R*4 | f10.3 | Measurement error for 2MASS -band magnitude. |
tmass_k | mag | R*4 | f10.3 | 2MASS -band magnitude. |
etmass_k | mag | R*4 | f10.3 | Measurement error for 2MASS -band magnitude. |
aw_w1 | mag | R*4 | f10.3 | AllWISE -band magnitude, W1MPRO entry in the original catalog. |
eaw_w1 | mag | R*4 | f10.3 | Measurement error for AllWISE -band magnitude, W1SIGMPRO entry in the original catalog. |
aw_w2 | mag | R*4 | f10.3 | AllWISE -band magnitude, W2MPRO entry in the original catalog. |
eaw_w2 | mag | R*4 | f10.3 | Measurement error for AllWISE -band magnitude, W2SIGMPRO entry in the original catalog. |
aw_w3 | mag | R*4 | f10.3 | AllWISE -band magnitude, W3MPRO entry in the original catalog. |
eaw_w3 | mag | R*4 | f10.3 | Measurement error for AllWISE -band magnitude, W3SIGMPRO entry in the original catalog. |
ebv | mag | R*4 | f7.1 | reddening based on the STILISM reddening map combined with Gaia DR2 distance and sky position. See Section 5 for more details. |
eebv | mag | R*4 | f7.1 | Measurement error for reddening. |
galex_nuv | mag | R*4 | f7.1 | GALEX -band magnitude. |
egalex_nuv | mag | R*4 | f7.1 | Measurement error for GALEX -band magnitude. |
galex_fuv | mag | R*4 | f7.1 | GALEX -band magnitude. |
egalex_fuv | mag | R*4 | f7.1 | Measurement error for GALEX -band magnitude. |
rosat_hr1 | R*4 | f10.3 | ROSAT hardness ratio HR1. | |
rosat_hr2 | R*4 | f10.3 | ROSAT hardness ratio HR2. | |
rosat_counts | ct/s | R*4 | f10.3 | ROSAT X-ray counts. |
erosat_counts | ct/s | R*4 | f10.3 | Measurement error for ROSAT X-ray counts. |
rosat_lx | R*4 | f10.3 | Absolute X-ray luminosity calculated from ROSAT X-ray data and Gaia DR2 trigonometric distance. | |
erosat_lx | R*4 | f10.3 | Measurement error for absolute X-ray luminosity. | |
li_ew | mÅ | R*4 | f7.1 | Lithium absorption line equivalent width. |
spt_ref | char | a25 | Reference for lithium absorption line equivalent width. | |
teff | K | R*4 | f7.1 | Effective temperature. |
teff_ref | char | a25 | Reference for effective temperature. | |
is_primary | int | i3 | 1: Single stars or primary (brightest) star in a multiple system. 0: Companion star in a multiple system. | |
mult_letter | char | a3 | Identifier letter for multiple system components. | |
sep_parent | asec | R*8 | f12.5 | Separation from parent star calculated from Gaia DR2 positions. |
esep_parent | asec | R*8 | f12.5 | Measurement error for separation. |
pa_parent | deg | R*8 | f12.5 | Position angle with respect to parent star calculated from Gaia DR2 positions. |
epa_parent | deg | R*8 | f12.5 | Measurement error for position angle. |
comover_gaiadr2_id | char | a40 | Gaia DR2 identification number for comoving star (parent or companion). Multiple entries are separated by a semicolon. | |
oh2017_group_id | char | a4 | Comoving group identification number from Oh et al. (2017). |
Note. — The full table data are available as online-only additional material.
JG wrote the codes, manuscript, generated figures and led the analysis; TJD compiled an initial list of new candidates and generated Figure 1; EEM first identified the over-density associated with MUTA, led the turnoff age analysis, the investigation of HD 27860 and provided the initial members list; AWM led the rotation periods analysis, wrote part o f Section 6.7 and built Figures 24 and 25, JKF provided help with parsing the Gaia DR2 data and general comments, and AB provided the atmosphere analysis of WD 0340+103 and Figure 21.




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