LAMOST OBSERVATIONS IN THE KEPLER FIELD: SPECTRAL CLASSIFICATION WITH THE MKCLASS CODE

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Published 2015 December 21 © 2016. The American Astronomical Society. All rights reserved.
, , Citation R. O. Gray et al 2016 AJ 151 13 DOI 10.3847/0004-6256/151/1/13

1538-3881/151/1/13

ABSTRACT

The LAMOST-Kepler project was designed to obtain high-quality, low-resolution spectra of many of the stars in the Kepler field with the Large Sky Area Multi Object Fiber Spectroscopic Telescope (LAMOST) spectroscopic telescope. To date 101,086 spectra of 80,447 objects over the entire Kepler field have been acquired. Physical parameters, radial velocities, and rotational velocities of these stars will be reported in other papers. In this paper we present MK spectral classifications for these spectra determined with the automatic classification code MKCLASS. We discuss the quality and reliability of the spectral types and present histograms showing the frequency of the spectral types in the main table organized according to luminosity class. Finally, as examples of the use of this spectral database, we compute the proportion of A-type stars that are Am stars, and identify 32 new barium dwarf candidates.

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1. INTRODUCTION

The Kepler space mission was designed to detect Earth-like and larger planets around solar-type stars using the transit method (Koch et al. 2010). The Kepler observatory is in a solar orbit, and began collecting data in a fixed field of view consisting of 105 square degrees in the constellations of Lyra and Cygnus on 2009 April 8. Data collection continued in that field until 2013 May 11, when the second of four reaction wheels failed. Kepler data consist of ultrahigh-precision photometry in a single wide wavelength band. While its primary purpose is the detection of transiting exoplanets, these data are also ideal for asteroseismic studies, and for the study and characterization of various types of variable stars, such as eclipsing binaries, pulsating variables, and stars showing variability arising from stellar activity. Most of these applications require accurate spectral types and stellar parameters, such as the effective temperature (${T}_{{\rm{eff}}}$), surface gravity ($\mathrm{log}g$), metallicity ([M/H]), and the projected rotation velocity ($v\mathrm{sin}i$). These parameters are best provided through the analysis of spectroscopic data. To acquire those data, and to carry out the analysis, the international LAMOST-Kepler project was initiated in 2010 (De Cat et al. 2015).

2. THE LAMOST-KEPLER PROJECT

The data for the LAMOST-Kepler project are supplied by the Large Sky Area Multi Object Fiber Spectroscopic Telescope (LAMOST, also known as the Guo Shou Jing Telescope). This unique astronomical instrument is located at the Xinglong observatory in China, and combines a large aperture (4 m) telescope with a 5° circular field of view (Wang et al. 1996). The focal surface is covered with 4000 optical fibers connected to 16 multi-object optical spectrometers with 250 optical fibers each (Xing et al. 1998). Each spectrometer has two arms, a blue and a red, which collect low-resolution spectra ($R\approx 1800$) covering 370–590 nm and 570–900 nm respectively. LAMOST is thus a powerful instrument capable of collecting thousands of spectra simultaneously down to magnitude 17.8. For more information on LAMOST and the LAMOST data release, see Cui et al. (2012), Zhao et al. (2012), and Luo et al. (2012).

The main goals of the LAMOST-Kepler project are to acquire spectra of as many stellar objects in the Kepler field of view as possible, and then to use those spectra to determine the stellar parameters and spectral types of the observed objects in a homogeneous way. These spectra will also be used to determine ${v}_{{\rm{rad}}}$ and $v\mathrm{sin}i$.

Fourteen LAMOST-Kepler fields were selected to cover the Kepler field of view (Figure 1). Each LAMOST-Kepler field contains a bright central star ($V\lt 8$) for the active optics and four fainter ($V\lt 17$) stars in the off-center holes for the guide CCDs. A detailed description of these observations and the selection of the targets can be found in De Cat et al. (2015). To date, 101,086 individual spectra have been obtained of 80,447 separate targets. Table 4 of De Cat et al. (2015) contains details for each of these separate observations, including stellar identifications, the R.A. and decl. of the fiber in question, the date and time of observation, the magnitude of the object, and the signal-to-noise obtained in the Sloan r-band.

Figure 1.

Figure 1. The location of the 14 circular LAMOST-Kepler fields in the Kepler field of view. The small black dots indicate the locations of the LAMOST-Kepler project targets.

Standard image High-resolution image

Our role in this project is to supply accurate two-dimensional spectral types for the observed targets. The large number of spectra obtained for this project (101,086) makes traditional visual classification techniques impractical, so we have utilized the MKCLASS code, as described in Section 3.2 below, to perform these classifications. Other teams are working on other goals of the LAMOST-Kepler project. The "Asian" team (A. B. Ren et al. 2015, in preparation) is preparing a statistical analysis of the stellar parameters resulting from the LAMOST reduction procedure. The "European" team (A. Frasca et al. 2015, in preparation) is determining the stellar parameters with an adapted version of the code ROTFIT (Frasca et al. 2003, 2006). This team is also determining radial velocities as well as rough estimates for the projected rotational velocity, $v\mathrm{sin}i$.

3. CLASSIFICATION OF THE LAMOST-KEPLER SPECTRA

3.1. The Role of Spectral Classification in Large-scale Spectroscopic Surveys

Spectral classification can play important roles in large-scale spectroscopic surveys, such as the current LAMOST-Kepler survey, the Sloan Digital Sky Survey, and others. Those roles are closely tied to the two main goals of spectral classification. The first of those goals is to place a star within the broad population of stars—that is, to locate the star in the Hertzsprung–Russell diagram. This yields, via calibrations, first estimates for the physical parameters of the star, and thus classification is an important first step in the spectroscopic analysis of a star. The second goal of spectral classification is to identify astrophysically interesting stars. Spectral classification is a powerful tool specifically designed to accomplish that task with minimal effort. A catalog containing two-dimensional spectral types augmented with peculiarity codes constitutes a rich database that may be mined to find, for example, candidate solar twins, solar analogs, chemically peculiar A-type stars, barium dwarfs and giants, white dwarfs, or many other desired stellar categories.

3.2. The MKCLASS Code

The MKCLASS code (Gray & Corbally 2014, v1.07)7 , an expert system designed to classify blue–violet spectra on the MK Classification system, was employed to produce the spectral classifications reported in this paper. MKCLASS was designed to reproduce the steps skilled human classifiers employ in the classification process. Central to this process is the direct comparison of the program star with the MK standard stars which define the system. A unique feature of MKCLASS is its ability to recognize many of the common spectral peculiarities, such as chemically peculiar A-type stars (both Ap and Am stars), metal-weak stars, carbon anomalies (such as strong or weak CN and CH bands), stars with enhanced s-process abundances (the barium dwarfs and giants) and others. MKCLASS also has rudimentary code for recognizing non-MK spectral types, such as white dwarfs, carbon stars, Wolf Rayet stars, and various other emission-line stars. A description of the MK Classification System, and the various types of spectral peculiarities can be found in Gray & Corbally (2009).

MKCLASS is distributed with two standard libraries, one based on rectified blue–violet (3800–4600 Å) spectra with $R\sim 2200$, obtained with the Dark Sky Observatory (Appalachian State University) 0.8-m telescope using the GM spectrograph with a 1200 g mm−1 grating. The second library is based on spectra obtained with the 600 g mm−1 grating on the same instrument. Those spectra have a spectral range from 3800–5600 Å, a spectral resolution $R\sim 1100$, and are flux calibrated. Since the LAMOST spectra are flux calibrated, we chose to use the second library for this classification project. A list of MK standard stars that this library is based on may be found on the MKCLASS website. This required degrading the resolution of the LAMOST spectra to R = 1100, and truncating those spectra to the 3800–5600 Å spectral range. A preprocessor was written to accomplish those tasks utilizing the auxiliary programs distributed with MKCLASS.

For "normal" stars, MKCLASS outputs not only a spectral type on the MK system, but also a quality evaluation, of "excellent," "vgood," "good," "fair" and "poor." These ratings are based on ${\chi }^{2}$ differences between the program spectrum and the best matched interpolated MK standard. Very few classifications are given a rating of "excellent"; this requires almost exact correspondence between the program spectrum and the interpolated spectral standard. Spectral types with a "vgood" quality rating will have, typically, an uncertainty (one standard deviation) similar to that reported in Gray & Corbally (2014), that is ±0.6 spectral subtype in the temperature dimension where 1 spectral subtype is the difference between, for instance, F5 and F6. In the luminosity dimension, the uncertainty is about 0.5 luminosity class, where one luminosity class is the difference between, for instance, "V" and "IV." This uncertainty is somewhat dependent on spectral type. Luminosity classification is particularly difficult in the mid A-type stars, where the uncertainty might rise to ±1.0 luminosity class. For spectra with a "good" quality rating, the errors are typically twice those for the "vgood" category. Spectral types with "fair" are much more uncertain, and those with "poor" are unreliable. The last two quality categories can usually be traced to either low signal-to-noise ratio (S/N) spectra, or spectra with obvious defects. Bear in mind that classifications with certain spectral peculiarities, such as strong or weak CN or CH bands might be assigned a lower quality because of significant differences between the program spectrum and the best-matched standard.

Peculiar stars that are so peculiar that a match with a single MK standard is not possible are not given a quality rating. The most common example is an Am star, or "metallic-line" A-type star where the Ca ii K-line, the hydrogen lines, and the metallic-line spectrum are each given separate spectral types. The spectral type of such stars is written in the following way: kA2hF0mF2, where, in this example, A2 represents the K-line spectral type, F0 the hydrogen-line type, and F2 the metallic-line type.

Further comments on the reliability of the spectral types can be found in Section 4.

MKCLASS is a work in progress, and many improvements have been made to the code in the course of the LAMOST-Kepler project. These improvements have resulted in version 1.07 of this code, which may be obtained online at  http://www.appstate.edu/~grayro/mkclass/.

4. THE CLASSIFICATION TABLE

4.1. Description of the Table

The main results of this paper are presented in the form of stellar classifications on the MK system in Table 1. That table consists of 81,171 entries giving MK classifications for the objects in the LAMOST-Kepler database that have plausibly classifiable spectra. The table is ordered in terms of the Kepler ID, except for those objects that do not have a Kepler designation; those objects are appended to the end of the table. The table consists of seven columns. The first column is the name of the original LAMOST fits file; many of these fits files are already in the public domain and may be downloaded from the LAMOST spectral archive (http://www.lamost.org). The unreleased spectra may be obtained upon request after becoming an external collaborator of the LAMOST-Kepler project.8 The second column is the Kepler Input Catalog designation expressed in the form KICNNNNNNNN. For those objects without a KIC designation, this column is blank. The third column is the stellar designation recorded in the header of the fits file. The fourth column is the S/N of the spectrum in the Sloan g-band (${\lambda }_{{\rm{eff}}}=4686$ Å), also taken from the fits header. The effective wavelength of this band coincides approximately with the center of the spectral range utilized for classification by MKCLASS with the libnor36 library (3800–5600 Å). The fifth column is the classification itself in the traditional format of an MK spectral type, with the temperature type first, the luminosity type second, followed by a list of detected peculiarities. For stellar types that are not on the MK system (such as white dwarfs), Table 2 lists the codes that MKCLASS uses for those types; not all of those codes can be found in Table 1. The sixth column of Table 1 is the quality, discussed in Section 3.2 above. The seventh column contains further notes on the quality (see below). Some example rows of Table 1 are reproduced in this paper. The remainder of that table (81,171 lines in total) may be obtained online.

Table 1.  LAMOST-Kepler MKCLASS Spectral Types (Sample Lines)

LAMOST Spectrum Fits File KIC Number Header ID g-band S/N Spectral Type Quality Notes
spec-56094-kepler05B56094_2_sp01-167 KIC01865567 SDSS 278 B8 IV Si vgood ...
spec-56094-kepler05B56094_sp01-167 KIC01865567 SDSS 319 B8 IV-V Si vgood ...
spec-56094-kepler05B56094_2_sp07-213 KIC01873552 SDSS 104 A6 V Sr vgood ...
spec-56094-kepler05B56094_sp07-213 KIC01873552 SDSS 125 A5 V Sr vgood ...
spec-56811-KP190339N395439V01_sp01-180 KIC02284009 1275-10742685 21 F7 IV-V Fe-0.6 good ...
spec-56811-KP190339N395439V02_sp01-180 KIC02284009 kplr002284009 20 F7 IV Fe-0.6 good ...
spec-56811-KP190339N395439V01_sp01-181 KIC02142733 (3) 1275-10780735 31 G0 IV-V vgood ...
spec-56811-KP190339N395439V02_sp01-181 KIC02142733 extra00015199 24 G1 V vgood ...
spec-56811-KP190339N395439V02_sp01-189 KIC02284278 1275-10750999 62 K5 III good ...
spec-56811-KP190339N395439V01_sp01-189 KIC02284278 kplr002284278 60 K5 III vgood ...
spec-56094-kepler05B56094_2_sp14-028 KIC04145645 1275-10950670 20 M3 III vgood ...
spec-56811-KP190339N395439V02_sp06-186 KIC04145645 1275-10950670 32 M2.5 III vgood ...

Only a portion of this table is shown here to demonstrate its form and content. Machine-readable and Virtual Observatory (VOT) versions of the full table are available.

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Table 2.  MKCLASS Codes for Non-MK Spectral Types

White dwarfs
DO(0),DB(1),DA(141),DQ(0),DZ(178)
Carbon stars
Carbon star(5)
Emission-line stars
WN(1), WC(0), Helium nova(0),
emission-line?(609)

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4.2. Further Notes on Spectral Quality

While many of the LAMOST spectra are of excellent quality, there are some problems with the data set. Some of the spectra are too noisy to classify. We have written the preprocessor to reject those spectra with essentially no signal in the 3800–5600 Å range. Some of the spectra have gaps or are truncated, and since those gaps would interfere with the operation of MKCLASS, most of those spectra are also rejected by the preprocessor. Another problem with the LAMOST spectra that has been largely addressed with the latest LAMOST pipeline (v2.7.5) concerns sky, background, or scattered light subtraction (below referred to as "background subtraction"). In earlier pipelines, it was clear that this subtraction was not always properly executed, as the cores of strong lines (such as the Ca ii H & K lines) in some spectra, even those with high S/N, had negative fluxes. In other spectra too little background light was subtracted. In both cases the spectral type (and other types of analysis) could be badly affected.

This problem has been addressed, mostly successfully, with the latest pipeline, but some spectra still exhibit these problems. Spectra with consistently negative fluxes at the violet end, or negative fluxes in the cores of strong lines (such as the Ca ii K & H lines)—both indicative of excessive background subtraction—have been labelled as "unclassifiable" in Table 1. Spectra with some negative points (which may arise either from too much background subtraction, or from noise) are indicated with a "?" in the notes column. Spectra with too little background subtraction are very difficult to detect by machine, but as it turns out, the spectral types assigned to those spectra by MKCLASS are frequently given quality ratings of "fair" or "poor," and/or are assigned unlikely spectral types, such as hypergiants or extreme metal deficiency. Those types have not been removed from the Table 1, simply because it is too time consuming to scan visually through 81,000 spectra to accomplish that task. We estimate that the percentage of spectra that are badly affected by incorrect background subtraction amounts to about 3%, with another 10% somewhat affected. To be safe, all those spectral types with "?" in the Notes column, and/or those with quality ratings of "fair" or "poor" should be regarded with some suspicion. When quoting any of the spectral types in Table 1 in other studies, the spectral type should always be accompanied by the quality rating and the comments in the notes column.

The quality of the spectrum and the resulting spectral type may also be judged from the Sloan g-band S/N listed in the tables. The actual S/N of the spectra submitted to MKCLASS is slightly higher (by a factor of ∼1.6) than those listed because of the filtering procedure used to reduce the resolution of the LAMOST spectrum to that of the MKCLASS spectral library. Even taking that into consideration, many of the tabulated values of the S/N seem somewhat low compared to the actual appearance of the spectra. The S/N is correlated with the MKCLASS quality assignments. For spectral types rated as "excellent," the average S/N = 180; for "vgood," S/N = 73; "good," S/N = 42; "fair," S/N = 11, and "poor," S/N = 14. Spectral types rated "poor" have a slightly higher average S/N than those rated "fair" because of the greater proportion of faulty spectra (incorrect zeropoints, truncations, and gaps) as well as including spectra that are obviously overexposed, but which are assigned a very high S/N by the pipeline.

Yet another way of judging the quality and consistency of the MKCLASS spectral types is by comparing spectral types derived from two or more spectra taken of the same star. Some examples for spectral types from B–M are illustrated in Table 1. For spectra with reasonable S/N ($\gtrapprox 20$), the agreement is excellent and usually well within the errors expected for the different quality ratings. Some further examples are noted in Table 3.

Table 3.  Candidate Ba Dwarfs

Star ID Sp Type Notes
KIC01720728 F5 V Sr
KIC01724355 F9 V Sr
KIC03538912 G0 V Sr
KIC04284190 F6 V Sr
KIC05459339 F8 IV-V Sr
KIC05466012 F5 IV-V Sr 1
KIC05638409 F4 V Sr
KIC06434982 G0 V Sr
KIC06859619 F5 V Sr
KIC06871863 F8 V Sr
KIC07964784 G5 V Sr
KIC08010149 F6 V Sr
KIC08363089 F5 V Sr
KIC08458741 G0 V Sr 2
KIC08642542 G0 V Sr
KIC08775099 F6 V Sr
KIC08905804 F6 V Sr
KIC09087611 F7 V Sr
KIC09095849 F6 III-IV Sr 3
KIC09156222 F6 V Sr
KIC09652632 F6 V Sr 4
KIC09690985 F9 V Sr 1
KIC09711291 G0 V Sr
KIC09786617 F6 V Sr 4
KIC09805523 F9 V Sr 1
KIC09970848 G1 V Sr
KIC09972026 F9 V Sr
KIC10124511 F5 V Sr 1
KIC10469565 F9 V Sr
KIC10850911 F6 V Sr
KIC11516943 F6 V Sr
KIC12736952 F9 V Sr

Notes.

1Two spectra exist for this star in the database, and MKCLASS assigns the same or very similar spectral types to both. 2Three spectra are available in the database, and MKCLASS assigns the same spectral type to all three. 3See the note on this star in the text of the paper. 4Metal-weak.

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4.3. Classification Statistics

Figure 2 shows histograms of spectral type frequency in Table 1 organized in panels according to luminosity type. While the stellar sample selected for the LAMOST-Kepler is not strictly a magnitude-limited sample (cf. De Cat et al. 2015), it does show the basic characteristics of such a sample. In a volume-limited sample the frequency of spectral types on the main sequence increases with decreasing luminosity, but in a magnitude-limited sample, as here, late K-type and M-type dwarfs appear with a low frequency because of their intrisically faint luminosity. Giants thus dominate the sample for spectral types later than K2. The most frequent stellar types in Table 1 are F and G dwarfs and subgiants, exactly the stellar types targeted by the Kepler mission.

Figure 2.

Figure 2. The frequency of the spectral types, organized vertically by luminosity class, found in Table 1.

Standard image High-resolution image

As noted in Section 4.1, MKCLASS has a rudimentary ability to identify stars with "non-MK" types, that is stars with spectral classifications that are not contained within the 2D framework of the MK system. These types are listed in Table 2, and the numbers in parentheses in that table give the frequencies with which they appear in Table 1. Note that the category "emission-line?," for which there are 609 entries in Table 1, is meant to be a grab-bag for all types of emission-line stars not accounted for in the other categories in Table 2, such as cataclysmic binaries, novae of various types, B[e] stars, etc. Unfortunately, it appears that many of the stars that fall into that category have spectra that are flawed with "spikes" arising from cosmic rays or, more likely, CCD read errors. In the early data sets from LAMOST (most notably, those taken during 2011), such flawed spectra were very common. It appears that in the newer data sets, which form the basis for this paper, such flaws now appear in less than 1% of the spectra.

Table 1 may be used for interesting statistical studies, provided those studies are not compromised by the selection criteria used in establishing the LAMOST-Kepler sample. A good example is determining the frequency of occurrence of Am stars (A-type metallic line stars—see Section 3.2). Abt (1981) studied the frequency of Am stars in the field and determined that Am stars constitute 32% of the dwarf and subgiant stars with spectral types between A4 and F1. In Table 1 we count a total of 3088 dwarfs and subgiants with spectral types between A4 and F1. That number includes 1067 Am stars with hydrogen-line types between those same limits. This gives a frequency of 34.6%, in excellent agreement with Abt.

The vast majority of Am stars have hydrogen-line and metallic-line types of F2 and earlier, although there is a small sample with hydrogen-line and metallic-line types as late as F5. These are known as the ρ Puppis stars (Gray & Garrison 1989). Some instances of those stars may be found in the database. Interestingly, there are a small number of stars that MKCLASS has classified using the Am notation (see Section 3.2) but which have hydrogen-line and/or metallic-line types beyond F5, some even in the G class. In some instances, these curious spectral types are derived from very noisy spectra. However, in other instances, it is clear that MKCLASS is using the Am notation to classify composite spectra—spectra that arise from the superposition of the spectra of two stars with very different spectral types. A common example (cf. Corbally 1987) is an A dwarf with a G giant.

5. STARS OF ASTROPHYSICAL INTEREST

As an example of how this database may be used, we provide a table of candidate barium dwarfs (Table 3). This table is not exhaustive, as we have considered only spectral types with quality evaluations of "vgood" and better, and S/N $\geqslant \;50$, so many good candidates remain undiscovered in these tables. We have visually inspected all of the spectra in this table and can verify the accuracy of the spectral types.

Barium dwarfs are F, G, and K-type dwarfs which show enhanced abundances of s-process elements (such as strontium and barium), presumably acquired from an asymptotic giant branch companion star, now a white dwarf. The interest in discovering such stars in the Kepler field is that they should show, provided the geometry is correct, eclipses with the putative companion white dwarf. Most barium dwarfs are single-lined spectroscopic binaries, and so far the white dwarf companions have only been directly detected in the ultraviolet, and then only via a statistical argument (cf. Gray et al. 2011). This means that the discovery of eclipses in one or more of these systems and verification that the companion is indeed a white dwarf would be of considerable astrophysical interest.

Of further interest is the star KIC09095849 in the table of barium dwarfs. This star has been classified by MKCLASS (and verified visually) as an F6 III-IV giant, and thus is considerably more evolved than other known barium "dwarfs." We have obtained a spectrum of this star with the spectrograph on the Vatican Advanced Technology Telescope, and that spectrum confirms the MKCLASS spectral type. This star may therefore provide a link between barium dwarfs and barium giants, almost all of which must have been contaminated with s-process elements while on the main sequence (cf. Böhm-Vitense et al. 2000; North et al. 2000).

Gray et al. (2001) derived basic physical parameters for a set of A, F, and G-type dwarfs, giants, and supergiants. Stars of spectral type F6 III-IV in that reference average ${T}_{{\rm{eff}}}=6450\;{\rm{K}}$ and $\mathrm{log}g=3.6$. Via theoretical evolutionary tracks (Lejeune & Schaerer 2001) this yields a mass for KIC09095849 in the range 1.7–2.0 ${M}_{\odot }$, indicating a ZAMS effective temperature between 8000 and 9000 K, corresponding to the mid A-type stars. No known barium dwarf has a spectral type earlier than F4. Indeed, many barium giants also have masses corresponding to A and early F-type stars on the ZAMS, and so this suggests that at least some A-type and early F-dwarfs that show strontium enhancements are in reality barium dwarfs and not Ap or Fp stars.

A caveat for those interested in discovering more examples of barium dwarfs in this dataset: be aware that there are occassional "glitches" at the location of the Sr ii $\lambda 4077$ line (the main spectral criterion used for identifying barium dwarfs, also called "strong $\lambda 4077$ stars" in the literature). A real barium dwarf will also show a strong Sr ii $\lambda 4216$ line, and many of these stars also show a noticeable enhancement in the strength of the Ba ii resonance line at $\lambda 4554$. Without those other criteria, it is not safe to classify a star as a barium dwarf. Indeed, the user should, in general, be aware of "glitches" in the LAMOST spectra which may result in incorrect peculiarity assignments. For instance, upon examination of those stars classified with a barium (Ba) peculiarity, a number showed a "glitch" at the wavelength of the Ba ii $\lambda 4554$ line. A case in point is KIC05853260, classified by MKCLASS from the LAMOST spectrum as K2 III CN1 Ba. We obtained a spectrum of this star with the Vatican Advanced Technology Telescope spectrograph. That spectrum agrees with the K2 III classification, but with no sign of a barium peculiarity. This suggests that some LAMOST spectra have "glitches" at random wavelengths, and those that correspond to lines involved in common spectral peculiarities (such as strong strontium and barium) are flagged as such by MKCLASS.

A further caution is necessary with regard to those stars classified as λ Bootis in Table 1. Definitive classification of a star as a λ Boo star requires an experienced classifier supplied with a high S/N ($\geqslant 100$) spectrum. It is preferable to use spectra with resolutions better than 2 Å as well. Hence, the 132 λ Boo classifications in Table 1 should be regarded as preliminary. They constitute an excellent source of λ Boo candidates for further investigation, but they are not definitive classifications.

Guoshoujing Telescope (the Large Sky Area Multi-Object Fiber Spectroscopic Telescope LAMOST) is a National Major Scientific Project built by the Chinese Academy of Sciences. Funding for the project has been provided by the National Development and Reform Commission. LAMOST is operated and managed by the National Astronomical Observatories, Chinese Academy of Sciences. J.N.F. acknowledges the support from the Joint Fund of Astronomy of National Natural Science Foundation of China (NSFC) and Chinese Academy of Sciences through the Grant U1231202, and the support from the National Basic Research Program of China (973 Program 2014CB845700 and 2013CB834900).

Footnotes

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10.3847/0004-6256/151/1/13