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Identifying the population of T-Tauri stars in Taurus: UV–optical synergy

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Abstract

With the third data release of the Gaia mission, Gaia DR3 with its precise photometry and astrometry, it is now possible to study the behavior of stars at a scale never seen before. In this paper, we developed new criteria to identify T-Tauri stars (TTS) candidates using UV and optical color-magnitude diagrams (CMDs) by combining the GALEX and Gaia surveys. We found 19 TTS candidates and five of them are newly identified TTS in the Taurus molecular cloud (TMC), not cataloged before as TMC members. For some of the TTS candidates, we also obtained optical spectra from several Indian telescopes. We also present the analysis of distance and proper motion of young stars in the Taurus using data from Gaia DR3. We found that the stars in Taurus show a bimodal distribution with distance, having peaks at \(130.17_{-1.24}^{1.31}\) pc and \(156.25_{-5.00}^{1.86}\) pc. The reason for this bimodality, we think, is due to the fact that different clouds in the TMC region are at different distances. We further showed that the two populations have similar ages and proper motion distribution. Using the Gaia DR3 CMD, we showed that the age of Taurus is consistent with 1 Myr.

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Notes

  1. https://www.iiap.res.in/iao/hfosc.html.

  2. http://onlinestatbook.com/Online_Statistics_Education.pdf.

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Acknowledgements

We thank all the people, who have made this possible. We thank the staff of DOT, IAO, Hanle and CREST (Hosakote), who have made spectroscopic observations possible. The facilities at DOT are operated by ARIES, Nainital. The facilities at IAO and CREST are operated by the Indian Institute of Astrophysics, Bangalore. PKN acknowledges TIFR’s post-doctoral fellowship. PKN also acknowledges support from the Centro de Astrofisica y Tecnologias Afines (CATA) fellowship via grant Agencia Nacional de Investigacion y Desarrollo (ANID), BASAL FB210003. This research has also made use of NASA’s Astrophysics Data System Abstract Service and of the SIMBAD database, operated at CDS, Strasbourg, France. This work presents results from the European Space Agency (ESA) space mission, Gaia. Gaia data are being processed by the Gaia Data Processing and Analysis Consortium (DPAC). Funding for the DPAC is provided by national institutions, in particular, the institutions participating in the Gaia MultiLateral Agreement (MLA). The Gaia mission website is https://www.cosmos.esa.int/gaia. The Gaia archive website is https://archives.esac.esa.int/gaia.

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Correspondence to Prasanta K. Nayak.

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This article is part of the Special Issue on “Star formation studies in the context of NIR instruments on 3.6 m DOT”.

Appendices

Appendix A. Sturges’ rule

Sturges’ rule (Sturges 1926) provides a simple method of binning the data based on the number of data points, n. Sturges’ rule makes the assumption that the histogram consists of normally distributed data points, approximated as a binomial distribution. The optical number of bins, k, using the Sturges’ rule (Sturges 1926) is given as:

$$\begin{aligned} k= 1 + \log _2(n). \end{aligned}$$
(A.1)

Appendix B. Rice rule and the rule of square roots

Other methods based on the number of data points in the sample are Rice ruleFootnote 2 and the rule of square roots. The number of bins, k, as given by Rice rule is \(k=\root 3 \of {n}\times 2\) and from the rule of square roots is \(k=\sqrt{n}\). The issue with these methods is that they do not consider the inherent skewness of the data.

Appendix C. Doane’s rule

If the data points are not normally distributed, we can use a modification of the Sturges’ rule, known as Doane’s rule (Doane 1976). Doane’s rule tries to account for the skewness of the data. The number of bins, k, is given as:

$$\begin{aligned} k = 1 + \log _2( n ) + \log _2 \left( 1 + \frac{ |g_1| }{\sigma _{g_1}} \right) , \end{aligned}$$
(C.1)

where \(g_{1}\) is the estimated 3rd-moment-skewness of the distribution and is given as:

$$\begin{aligned} g_{1}=\frac{\Sigma _{i=1}^{n} (X_i - \bar{X})^3}{[\Sigma _{i=1}^{n} (X_i - \bar{X})^2]^{3/2}}. \end{aligned}$$
(C.2)

Here, \(X_i\) are the data points and \(\bar{X}\) is the mean of the sample. \(\sigma _{g_{1}}\) is given as:

$$\begin{aligned} { \sigma _{g_{1}}={\sqrt{\frac{6(n-2)}{(n+1)(n+3)}}}}. \end{aligned}$$
(C.3)

Appendix D. Scott’s rule

Scott’s rule (Scott 1979) is based on the standard deviation, \(\sigma \), of the data. Unlike previous methods, Scott’s rule gives us the optimal bin width, h, and not the number of bins, k. The bin width, w, is correlated with the number of bins by \(k={R}/{w}\), where R is the range in the distribution. The bin width is given as follows:

$$\begin{aligned} h = \frac{3.49 \sigma }{\root 3 \of {n}}. \end{aligned}$$
(D.1)

Appendix E. Freedman–Diaconis rule

The Freedman–Diaconis rule (hereafter FDR; Freedman & Diaconis 1981) has a similar approach as that of Scott’s rule, wherein the optimal bin width is considered instead of the number of bins. The optimal number of bins in the FDR rule depends on the interquartile range \({\text {IQR}}(x)\). The \({\text {IQR}}(x)\) is less sensitive to deviant outlier points than the usual standard deviation estimations. Standard deviation calculation depends on the mean of the data, where outlier data points are included. This may affect the accuracy of the result, and hence \({\text {IQR}}(x)\) will be the best way to estimate the bin size. The optical bin width is estimated as:

$$\begin{aligned} h=2{{\text {IQR}}(x) \over {\root 3 \of {n}}}. \end{aligned}$$
(E.1)

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Nayak, P.K., Narang, M., Puravankara, M. et al. Identifying the population of T-Tauri stars in Taurus: UV–optical synergy. J Astrophys Astron 44, 83 (2023). https://doi.org/10.1007/s12036-023-09972-6

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