Multiplicity of M-dwarfs

The AstraLux Large M-dwarf Multiplicity Survey**affiliation: Based on observations collected at the European Southern Observatory, Chile, under observing programs 081.C-0314(A), 082.C-0053(A), and 084.C-0812(A), and on observations collected at the Centro Astronómico Hispano Alemán (CAHA) at Calar Alto, operated jointly by the Max-Planck Institute for Astronomy and the Instituto de Astrofísica de Andalucía (CSIC).

Markus Janson11affiliation: Princeton University, Princeton, USA 22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany 55affiliation: Hubble fellow; janson@astro.princeton.edu , Felix Hormuth22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany , Carolina Bergfors22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany , Wolfgang Brandner22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany , Stefan Hippler22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany , Sebastian Daemgen33affiliation: European Southern Observatories, Garching, Germany , Natalia Kudryavtseva22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany , Eva Schmalzl44affiliation: Leiden Observatory, Leiden, Netherlands , Carolin Schnupp22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany , Thomas Henning22affiliation: Max Planck Institute for Astronomy, Heidelberg, Germany
Abstract

We present the results of an extensive high-resolution imaging survey of M-dwarf multiplicity using the Lucky Imaging technique. The survey made use of the AstraLux Norte camera at the Calar Alto 2.2m telescope and the AstraLux Sur camera at the ESO New Technology Telescope in order to cover nearly the full sky. In total, 761 stars were observed (701 M-type and 60 late K-type), among which 182 new and 37 previously known companions were detected in 205 systems. Most of the targets have been observed during two or more epochs, and could be confirmed as physical companions through common proper motion, often with orbital motion being confirmed in addition. After accounting for various bias effects, we find a total M-dwarf multiplicity fraction of % within the AstraLux detection range of 0.08–6″(semi-major axes of 3–227 AU at a median distance of 30 pc). We examine various statistical multiplicity properties within the sample, such as the trend of multiplicity fraction with stellar mass and the semi-major axis distribution. The results indicate that M-dwarfs are largely consistent with constituting an intermediate step in a continuous distribution from higher-mass stars down to brown dwarfs. Along with other observational results in the literature, this provides further indications that stars and brown dwarfs may share a common formation mechanism, rather than being distinct populations.

binaries: general — techniques: high angular resolution — stars: late-type
slugcomment: Submitted to the Astrophysical Journal

1 Introduction

The multiplicity of stars is an important characteristic for understanding how they form and evolve. The fraction of multiple stars has implications for typical architecture of stellar and planetary systems, monitoring their orbital characteristics yields information that would otherwise be unavailable, and their distribution in orbits and masses can yield insights into the formation process (e.g. Burgasser et al., 2007; Goodwin et al., 2007). One clear observational trend that has gradually emerged is that the fraction of stars that have stellar companions depends on the masses of those stars. For instance, within the population of Sun-like stars (FGK-type), less than half (46%; Raghavan et al., 2010) are multiple (although a previous well-known survey gave a larger value of up to 67%, see Duquennoy & Mayor, 1991). By contrast, for more massive stars in the AB-type range, upwards of 80% appear to be in multiples (Shatsky & Tokovinin, 2002; Kouwenhoven et al., 2007; Peter et al., 2012). The trend of decreasing multiplicity from massive stars to Solar-mass stars also continues down to lower masses. In the M0–M6 spectral type range, multiplicity fractions of 26–42% have been found (e.g. Fischer & Marcy, 1992; Delfosse et al., 2004). For even later-type objects in the VLM range (Very Low-Mass stars and brown dwarfs), the multiplicity frequencies are as low as 10–30% (e.g. Bouy et al., 2003; Close et al., 2003; Gizis et al., 2003; Joergens, 2008).

A challenging factor in previous surveys for multiplicity in low-mass stars has been limited sample sizes of 100 stars or less. Part of the reason for this is that M-stars are altogether more poorly characterized than higher-mass stars – for instance, due to their low brightnesses, they are generally not included in the Hipparcos catalog (Perryman et al., 1997). Hence, well-characterized samples of M-dwarfs that are appropriate for statistical studies have been hard to come by. However, recently a number of efforts have been made in identifying and characterizing nearby M-dwarfs (e.g. Riaz et al., 2006; Reid et al., 2007; Lépine & Gaidos, 2011), which has mitigated this situation. Following the publications of these studies, we have undertaken an extensive effort to study the multiplicity properties of nearby M-stars with high-resolution imaging. An intermediate study of 124 of these targets has been previously published (Bergfors et al., 2010). Here, we summarize the full sample of 761 individual stars and perform studies of statistical properties of various sub-samples.

A large sample of stars and a catalog of their binarity properties are relevant for a wide range of scientific purposes. For instance, the formation of VLM objects remains less well understood than for Sun-like stars. Although there are many indications that they may form as the low-mass tail of regular star formation (e.g. Luhman et al., 2005; Bourke et al., 2006), there have also been alternative mechanisms proposed for the formation of some or all of these objects (e.g. Reipurth & Clarke, 2001; Goodwin & Whitworth, 2007; Basu & Vorobyov, 2012). For instance, Thies & Kroupa (2007) argue that the different binarity properties of stars and VLM objects is an indication for separate formation mechanisms of the two populations. Sun-like stars have separations that peak broadly at 30 AU, and a rather uniform distribution of mass ratios (e.g. Duquennoy & Mayor, 1991; Raghavan et al., 2010), whereas VLM objects have separations that peak narrowly at smaller separations (3–10 AU), and show a preference to nearly equal masses of the components (e.g. Burgasser et al., 2007). A key question, then, is whether the transition in binary properties from Sun-like stars to VLM objects proceeds smoothly over the intermediate range. A large M-dwarf sample is ideal for addressing this question. If any break or bimodality occurs over this range, this would imply that there are indeed two separate formation scenarios at play, whereas if the progression is fully continuous and monotonous, the opposite would be the natural conclusion.

Besides statistical issues, the individual detections, confirmations, and observational parameters of binaries are highly useful. For instance, continued orbital monitoring can yield simultaneous brightnesses and masses of the components (e.g. Delfosse et al., 2000; Zapatero Osorio et al., 2004; Bouy et al., 2004; Liu et al., 2008). Since our main sample from Riaz et al. (2006) is young, one of the implications of this is that the ages of individual systems can be inferred through isochronal analysis (e.g. Janson et al., 2007). Conversely, for the youngest systems and lowest masses, the theoretical mass-luminosity relationships (e.g. Burrows et al., 1997; Chabrier et al., 2000), which are increasingly uncertain under such conditions, can be better constrained (e.g. Hillenbrand & White, 2004; Konopacky et al., 2010).

The paper will be structured as follows: In Sect. 2, we will describe the observations and data reduction procedure used for the survey. In Sect. 3 the determination of the photometric and astrometric properties of each detected binary pair is described, along with the determination of the corresponding underlying physical parameters of the individual components. This is followed by a discussion of sub-sample selection for statistical purposes in Sect. 4. Most of the binaries have been observed over two or more epochs, and the astrometric analysis of those cases is discussed in Sect. 5. The statistical analysis is described in Sect. 6 for the multiplicity fraction, and Sect. 7 for the distribution of physical parameters. Finally, we summarize our results in Sect. 8. Furthermore, individual notes for targets in the survey as well as a summary of background contaminants are provided in the Appendix.

2 Observations and Data Reduction

For all observations in this survey, we have used AstraLux Norte (Hormuth et al., 2008) at the Calar Alto 2.2m telescope in Spain, and AstraLux Sur (Hippler et al., 2009) at the ESO/NTT 3.5m telescope on La Silla in Chile. The two AstraLux cameras are a near-identical twin pair of high-speed electron multiplying cameras developed for a wide range of high-resolution imaging purposes (e.g. Hormuth et al., 2007; Sicilia-Aguilar et al., 2008; Daemgen et al., 2009). This is achieved through a technique known as ”Lucky Imaging” (Tubbs et al., 2002; Law et al., 2006), where a very large number of frames (10000) of very short integration time (10 ms) are collected during an observation. In such a short time as 10 ms, each frame can be seen as capturing a frozen state of the wavefront distortion pattern imposed by the atmosphere. These states will be statistically distributed over a wide range of distortion severity, where in some cases, the wavefront will be particularly well preserved, so that the Strehl ratio will be high in these frames. By rejecting the majority of frames and using only the few percent of highest Strehl ratio, we can gain substantially in spatial resolution in this way, and achieve almost diffraction-limited images, at the cost of image depth.

Our total sample consists of 761 unique stars, of which 124 were presented in Bergfors et al. (2010). In this study, we present results for the full sample. In most cases where a companion candidate was found, multiple observations of the same system have been taken over a baseline that is useful for common proper motion tests, so that physical companionship can be stringently tested in those cases. The targets were chosen primarily from the Riaz et al. (2006) sample (569 stars) and additionally from the Reid et al. (2007) sample (198 stars), and are summarized in Table 1. The spectroscopic distances in the table were adopted from Riaz et al. (2006) (but corrected for binarity for binaries detected with AstraLux, see Sect. 4). The targets were selected directly from the above samples without additional constraints imposed, except for the AstraLux Sur targets, where only M-stars within 52 pc were observed. For statistical purposes, we have constructed homogenized sub-samples within the existing data. We will discuss various sub-samples that were selected for specific statistical investigations in Sect. 4. With most stars being observed in two filters (SDSS and ) and many of the binaries being observed twice or more, our survey encompasses more than 1600 individual observations, each of 10–12 minute extent in telescope time. In total, this corresponds to approximately 300 hours of observations, which have been performed between January 2007 and February 2010.

The raw frames produced by the camera were reduced with the dedicated AstraLux pipeline (Hormuth et al., 2008), which makes the frame selection and recombination of frames, with a Drizzle algorithm to oversample the image and produce an output pixel scale of 23.3 mas/pixel for AstraLux Norte and 15.4 mas/pixel for AstraLux Sur. Flat field and bias corrections are applied prior to the drizzling. Individual frames were aligned based on the brightest pixel in the oversampled frames, and the 10% best frames were selected for producing the final image. The pixel scale as well as the orientation of true North were monitored by observing astrometric references during the nights, in particular the Trapezium (Köhler et al., 2008) whenever it was visible, and M15 (van der Marel et al., 2002) at any other time. The representative uncertainties for these quantities, determined using the IRAF geomap procedure, are as/pixel in pixel scale, which typically does not dominate the error in astrometric separation since the separations of the binaries in our survey are small, and 0.3 in orientation angle, which often does dominate the error in position angle for the binary astrometry.

A sample of reduced images are shown in Fig. 1. The separation and brightness contrast of each binary (as discussed in the following section) along with the AstraLux detection limit is shown in Fig. 2.

Figure 1: Four examples of multiple systems imaged in the AstraLux survey. Top left: A high-contrast binary. Top right: A low-contrast binary. Bottom left: A triple system. Bottom right: A binary displaying the fake triple effect, common for close low-contrast binaries. All images are in , and in each case North is up and East is to the left.

3 Photometry and Astrometry

The procedure for determining photometric and astrometric quantities was already described in Bergfors et al. (2010), here we summarize that procedure. The relevant quantities to be determined are the magnitude differences between primary and secondary within each pair in each detected multiple system in and for photometry, and the projected separation and position angle of the components in each pair for astrometry. For close binaries (1″ or less), this was done with PSF fitting, using the reference PSF of a single star to iteratively create binary configurations that minimize the squared residuals of the fit. For wider binaries, we used Gaussian centroid fitting of the primary and secondary in order to yield the photometric and astrometric parameters.

As is normally the case in Lucky Imaging data, some close and near-equal component binaries display the ”fake triple” effect, where a ghost tertiary appears at the same separation from the primary as the real secondary, but on the opposite side of it. In these cases, we use the procedure of Law (2006) to ”de-triple” the system, determining the true flux ratio of the binary components as

(1)

where and . When a fake triple occurs, or indeed more generally in any case of a close binary of nearly equal brightness, it is relevant to note that there can be a 180 phase ambiguity, given the difficulty to determine which star is actually the primary. This is especially true for such late-type stars as these, which are sometimes quite variable, such that the binary components alternate between which is the brightest. On this topic, it should be noted that because the brightness difference between the two components is taken as the apparently brighter component minus the apparently fainter one, it is a positive definite quantity. Hence, the measured brightness difference on (e.g.) two equally bright components will not converge toward zero for a large number of measurements, since no measurement will be negative. This leads to a bias which exaggerates the brightness difference of close companions, and which most likely explains the apparent avoidance in the zone of very close binaries with almost equal-mass components (see Fig. 2). The final photometry and astrometry values of each detected binary are listed in Table 2, and in Table 5 for the suspected or confirmed background contaminants..

Figure 2: The separation and brightness difference in for all binary pairs detected with AstraLux, plotted along with the typical AstraLux detection limit. The small zone in the upper left that shows a lack of objects is likely due to a bias that tends to systematically over-estimate the brightness difference for close pairs of nearly equal brightness.

In order to translate the integrated spectral type and relative photometry of each binary pair into individual spectral types and masses, we again follow the procedure in Bergfors et al. (2010), which was developed in Daemgen et al. (2007) and is based on the magnitude-spectral type relationship in Kraus & Hillenbrand (2007). We base our final individual spectral types on the -band, but we also make the same estimations on the basis of the -band, which gives consistent spectral types to within 0.5 sub-classes (except in those cases that have been identified as background objects). The translation of individual spectral types to component masses also follows the relations given in Kraus & Hillenbrand (2007). The resulting physical quantities for the pairs are listed in Table 3.

4 Statistical Samples

Out of our total sample we construct two main sub-samples for the purpose of statistical analysis. This is done in order to remove statistical bias from selection effects and provide samples that are optimally suited for specific statistical studies. The first sample will be referred to as the Inclusive Sample (IS). This sample includes most of the stars observed, with some special cases excluded that are discussed toward the end of this section. However, this also includes 60 stars with estimated spectral types earlier than M-type (K7 and K5) which are additionally excluded in many of the statistical investigations.

The second sample is a sub-sample of the first and is called the Constrained Sample (CS). This sample is constructed to provide a multiplicity fraction that is well-defined and bias free, following similar criteria to those in Bergfors et al. (2010). In CS, we make a cut for significant X-ray flux. This provides a sample that is young (less than 1 Gyr, see Bergfors et al., 2010) and provides further confirmation that the selected targets are indeed nearby M-dwarfs rather than mis-classified distant objects, as can otherwise happen for these kinds of targets where a parallax is generally lacking. As in Bergfors et al. (2010), we use X-ray counts and errors from ROSAT111Both the Bright Source Catalog IX/10A and the Faint Source extension IX/29 (Voges et al., 1999) with 3.3 as the relevant significance criterion. In the case of binaries, this can lead to a selection effect due to the fact that the flux of the primary and secondary may add up to just above the significance criterion in cases where a single star would not have reached the criterion and thus not have been selected. We account for this in the same way as in Bergfors et al. (2010), by noting that is roughly constant as a function of spectral type, and calculating what the significance would have been for the primary component alone, had it been single. In those cases where the significance drops below the 3.3 criterion, the binary is removed from the CS. These cases are laballed ‘S’ in the X-ray column of Table 1.

We also adopt a 52 pc maximum distance cut-off for the CS, again analogously to Bergfors et al. (2010). However, in addition, we also take into account a further bias that favors selection of binaries. Since most of the distances are determined spectroscopically under the assumption that the primary is single, a system that is in reality a binary will appear artificially too bright for the primary spectral type, and thus appear closer than it really is. We correct for this by adjusting all the distances for binaries that do not have parallax measurements and are not resolved in the 2MASS catalog (Skrutskie et al., 2006), which provided the brightness that the spectroscopic distance estimate was originally based on. Any binary that passes the 52 pc cut-off with the new distance estimate is removed from the CS. In the cases of both X-rays and distance, there can be stellar components inside of the resolution limit of AstraLux which could have similar effects as those corrected for here. To first order, one might expect that such effects should affect singles and multiples within the AstraLux range of 0.08″–6.0″ equally and thus not introduce any significant bias in the multiplicity fraction, although it should also be noted that some bias could be introduced if there is a strong correlation between the presence of a close companion and the presence of wider companions.

The CS also only contains primary stars in the spectral type range of M0–M5. In contrast to the analysis in Bergfors et al. (2010), in this study we do not remove targets that are 6″ companions to stars of earlier spectral type than M0. The reason for this is that we are concerned with multiplicity in the range of 0.08″–6.0″, and so any companions or lack of companions beyond these limits should not be allowed to have an impact on the multiplicity statistics.

In total, 761 targets observed by AstraLux are presented here, of which 205 are multiple within 0.08″–6.0″. The IS sample contains 751 targets with K-stars (693 without K-stars), of which 203 (191 without K-stars) are multiple. The CS sample contains 337 targets, where 85 are multiple. The majority of the multiple systems are binary, but there are 12 triple systems and 1 quadruple system in the IS, and 6 triple systems in the CS (all within 0.08″–6.0″). These numbers include only those detected candidates that are consistent with common proper motion with the primary and/or the expected color-magnitude relationship of a physical companion, and not those that have been rejected in this regard (see Sect. 5 for details on the companionship analysis).

There are also 10 targets that are not included in either statistical sample. Seven of these were excluded because their multiplicity status is unclear: Since the resolution and contrast limits are not sharp cut-offs and since there is some variability in data quality, there inevitably exist limit-case tentative detections where binarity is plausible, but cannot be firmly established, for instance because the binary fitting does not converge, or there is a deemed risk of mix-up with some temporary PSF extension of non-astronomical origin. In our sample, these cases are J05323611-0523010, J15403153+1736554, J15530484+4457446, J21375368-0444383, J22581643-1104170, J23353509-0613302 and J23385413-1246184. Data under better conditions or with larger apertures are needed to confirm or reject those potential companions as astronomical objects. The remaining three cases that are not included in any of our sub-samples are binaries that contain a white dwarf. These systems, J03324345-0855391, J10162867-0520320 and J16291031+7804399, are discussed further in the individual notes.

5 Multi-epoch Analysis

Most of the multiples observed with AstraLux have been detected in multiple epochs. Systems that were first discovered with AstraLux were generally observed over more than one epoch, and in addition, literature astrometry exists for some systems that had been previously discovered. In each case where multi-epoch astrometry exists, it becomes possible to stringently test physical companionship through common proper motion, as well as to examine whether significant orbital motion is taking place. Hence, we perform such analysis for all systems observed in more than one epoch. For each system, we acquire a proper motion for the primary from the literature, either from Hipparcos (where available), or otherwise from the PPMXL (Röser et al., 2010) or NOMAD 222Available from http://www.nofs.navy.mil/nomad/ or VizieR I/297 catalogs. Likewise, whenever parallax values are available (see Table 1), they are used in the analysis, in the remaining cases a parallax is calculated based on the spectroscopic distance estimate. Two epochs of astrometry are then chosen for each star, and the change in position is compared to the change that would be expected for an unrelated static background object. If the relative motion deviates by more than 3 from the background hypothesis, the binary is considered as a confirmed physical binary. If in addition there is a more than 3 deviation from exact co-motion, the binary is considered to display significant orbital motion, with some exceptions. These are the cases for which the estimated period is very large relative to the observed motion over the observational baseline. Although there can be a signficant excess of orbital motion over expectation if the orbit is close to periastron or if the distance to the system is considerably smaller than the mean value, there is also good reason for caution in the event that the astrometric errors have been underestimated in those cases. Hence, we regard such cases as unconfirmed with respect to orbital motion.

The alternative case where there is a less than 3 deviation from the background hypothesis is somewhat more complicated, because in that case there is an ambiguity between orbital motion and non-common proper motion – in principle, there can be orbital motion that happens to bring the companion in the same direction as it would have moved relative to the primary, if it had been a static background source. There are a few cases in our sample where this issue is genuinely very complicated; these are discussed in the individual notes. However, in most cases, there are two clear groups of objects with non-significant common proper motion: those for which the expected motion is simply small compared to the astrometric errors, which we treat as unconfirmed with regards to companionship, and those that display a clear motion consistent with the background hypothesis, which we regard as being cases of background alignment. We summarize these results in table 4.

The vast majority of the systems examined do exhibit a common proper motion, which confirms that background contamination is rare and that most binaries in the total sample (including most of those that have only been observed in a single epoch) are real physically bound systems, as can also be statistically inferred simply from the fact that the frequency of detected companions increases rapidly with decreasing projected separation, rather than the other way around, as would be expected if background contaminants were dominant (Bergfors et al., 2010). Furthermore, the group of systems for which the color of the secondary is inconsistent with expectations for a physical companion provide an excellent match to the group of systems that are best consistent with the background hypothesis in the proper motion analysis. Hence, we conclude that false positives can be distinguished from real physical systems in our data with a high accuracy. All cases for which no common proper motion could be established (either due to only a single epoch being available, or due to insufficient motion with respect to the astrometric errors between the epochs) are listed in the individual notes in the Appendix. In order to quantify the risk of biasing the multiplicity statistics through mis-classification of background targets as physical companions and vice versa, we can note that only two of the systems that were classified through both their colors and their proper motion give conflicting conclusions between these two measurements (J03050976-3725058 and J06583980-2021526, see individual notes). Since 134 of the systems have been doubly tested in this regard, this means that 1.5% of the systems are problematic, such that in the remaining 85 system that have not yet been doubly tested, we can expect one additional such system, giving three in total. Assuming that all these three systems are mis-classified gives, for instance, a potential impact on the multiplicity fraction among the 337 targets in the CS sample of approximately 1%. Aside from being generous in this context given the fact that the two targets listed above are not even included in the CS, this is in any case smaller than the statistical error, as shown in Sect. 6, and we can thus assume that the impact of this potential bias is negligible.

We do not make any attempts at more detailed orbital modeling even for systems with several epochs of observations – additional AstraLux epochs are still being acquired, and a detailed orbital analysis based on those results will be the subject of a future publication.

6 Multiplicity Fraction

6.1 Total Multiplicity Fraction

We calculate the total multiplicity fraction of M0–M5-stars between 0.08″ and 6.0″ based on our CS sample. The fraction of detected multiples in the CS is %. However, in order to get the actual multiplicity fraction in the range of 0.08″–6.0″, we have to account for the fact that the detectability is incomplete for faint companions at small separations. We do this by noting that detectability is essentially complete for all separations as long as  mag is fulfilled, and that it is complete for the full contrast range as long as ″ is fulfilled (see Fig. 2). We then assume that the distribution of is independent of separation, such that would hold true under full completeness, where is the number of binary pairs with  mag and ″, is the number with  mag and ″, and and are the corresponding cases with  mag. In other words, we assume that in the narrow-separation range of 0.08″–1.0″, the fraction of low-contrast companions ( mag) to high-contrast companions ( mag) is the same as is measured outside of 1″. Hence, the number of missed companions is the difference between the ideal that fulfills the equality and the actual measured number. In this context, it should be noted that the assumption of being independent of separation should be taken with some caution, as discussed in Sect. 7.

In this way, we find that 7.4 companions are missing in the data, such that the actual multiplicity fraction is %, where the error is based on Poissonian statistics. There is a remaining incompleteness to low-mass brown dwarfs; although we are sensitive to L0-type companions out to 52 pc, later-type companions fall below the sensitivity limits for the distant part of the sample. However, given that such companions are rare even for closer systems (only three L0 companions exist in the entire observed sample, see Table 3), this is most likely a marginal effect. Hence, in summary, we conclude that the multiplicity fraction of M0–M5-stars within 0.08″–6.0″ is %.

As mentioned above, our observations and statistical studies are focused on acquiring multiplicity statistics within the separation range covered by AstraLux of 0.08″–6.0″. However, in order to put this discussion in a broader context, we will briefly discuss the implications for the total multiplicity fraction, irrespective of separation. We do this by comparing the result to the multiplicity study by Fischer & Marcy (1992) (abbreviated as FM92), which studies the full separation range by combining radial velocity and imaging data. Our limits in angular separation at the median distance of the sample of 30 pc correspond to projected separations of 2.4 AU to 180 AU. We translate this into statistically relevant physical separations by applying the FM92 correction factor of 1.26, yielding physical limits of 3 AU to 227 AU. Out of the 37 companions detected in FM92, 14 are either inside of 3 AU or outside of 227 AU. Henceforth, we will assume that the completeness within 3–227 AU is approximately the same as outside of this range in FM92; the estimated completeness values in FM92 largely support such an assumption, although the values for very large separation are highly uncertain. Under this assumption, we can hypothesize that in addition to the 85 companions that we detect within 3–227 AU in our CS sample, there additionally exist companions outside of these limits. Some of these will exist in systems that appear single in the AstraLux images, and thus form an additional multiple system, whereas others will exist in systems the are already binary within 3–227 AU, and thus not affect the total multiplicity fraction (but only the higher-order fraction). To which extent these additional companions affect the multiplicity statistics thus depends on to which extent close or wide companions are correlated or anti-correlated with companions in the intermediate separation range. For the purpose of this discussion, we assume that there is no correlation, such that exactly 27.4% of the additional components occur in systems that had already been identified as multiple. This leaves 23.4 companions that contribute to the total multiplicity fraction over all separations, which consequently comes out to 34.4%. By comparison, the total multiplicity fraction in FM92 is given as %. Alternatively, we may recalculate the FM92 multiplicity within 3–227 AU under the same assumptions, by removing multiplicity components that are outside of these ranges. This gives a fraction of 28% within 3–227 AU in FM92. Hence, our data implies a slightly lower multiplicity fraction than FM92, but the values are consistent within the errors (under the given assumptions).

6.2 Multiplicity Dependence on Spectral Type

After having examined the multiplicity fraction of the full population of M0–M5-stars, we turn to studying the dependence of multiplicity fraction on spectral type within the sample. It is already well known that this fraction increases globally with increasing primary mass, since the multiplicity fraction is higher for Sun-like stars at 46–67% (Duquennoy & Mayor, 1991; Raghavan et al., 2010), yet higher for yet more massive stars at 70% (e.g. Shatsky & Tokovinin, 2002; Mason et al., 2009), and lower for brown dwarfs at 10–30% (e.g. Burgasser et al., 2003; Joergens, 2008). Given our large sample and relatively large range in stellar masses, we can check how the multiplicity fraction evolves as function of primary mass self-consistently within the sample. In other words, if there are any discontinuities along the range as opposed to a smooth decline toward smaller masses, these could potentially be noticeable in the data. We use the IS M-dwarf sample for this purpose.

A plot of the multiplicity fraction as function of spectral type is shown in Fig. 3. The distribution is consistent with a uniform trend, and with random scatter from Poisson errors around the trend. For instance, although the fraction at spectral type M0 is lower than the fraction at M2, this is not statistically significant. We show this by making a linear fit to the data. The best fit (shown in Fig. 3) gives a of 10.1, corresponding to a probability that it matches the underlying distribution of 52.6%. Hence, a monotonous trend is fully plausible given the data, and there is no valid motivation to infer any sub-structure in the general trend. Furthermore, the slope of the line is negative with increasing sub-class (i.e., decreasing mass), with a coefficient of . Thus, at a marginal significance of 1.9, we can confirm the trend of multiplicity function with stellar mass, even within just the M-star spectral type range.

Figure 3: Multiplicity fraction as a function of primary spectral type. The data are consistent with a uniformly increasing trend with stellar mass.

7 Physical Distributions

7.1 Distribution in Mass Ratio

The mass ratios of binaries among Sun-like stars and brown dwarfs have quite different distributions (e.g. Burgasser et al., 2007; Raghavan et al., 2010), where the mass ratios among Sun-like stars are quite uniformly distributed, while the components of brown dwarf binaries appear to be preferentially nearly equal in mass. It is thus interesting to study to whether M-dwarfs constitute a transitional regime between these two distributions, and if so, whether the transition is continuous or discrete. In order to demonstrate that this is a more complicated issue to address than it might seem at first, we first discuss the case of the IS sample.

A histogram of the mass ratios in the IS sample is shown in Fig. 4. Here the mass ratio is defined as , where is the primary mass and is the secondary mass. The sample shown in the figure only includes binaries with separations larger than 1″, since smaller separations are subject both to bias due to the limited detectability of high-contrast systems in that range, as well as the high uncertainty in determining flux ratios of close binaries. The histogram shows a very pronounced peak at mass ratios near unity, in addition to a population with a more homogenous distribution. However, the peak is not physically real, as we can see if we plot the same distribution for the CS sample, shown in Fig. 5. Again, this analysis contains only binaries with separations greater than 1″. For the CS sample, the distribution is much more homogenous, with no sharp peak near equal masses. The stark difference between the two samples can be easily understood by considering the biases that are involved. As we mentioned in Sect. 4, in the CS sample we have de-selected binaries that were positively selected for during observation preparations by appearing to be closer or brighter in X-rays than they would have been if they had been single. This effect is by far the strongest in binaries where the components have about equal brightness, and thus about equal mass. Hence, even though this is globally a subtle effect, in that the number of binaries that are positively selected for is rather small compared to the total number of binaries and single stars in the survey, it is the case that in every event where it happens, the contaminating binary has a near-unity mass ratio and thus the effect becomes significant in the particular case of mass ratio investigations.

Figure 4: Histogram of mass ratios for the IS sample. The peak at near-equal masses is due to an observational bias, as explained in the text.

For this reason, we will concern ourselves only with the CS distribution for the rest of the mass ratio discussion. In order to examine this distribution in a bias-free manner, we need to take some observational effects into account. As a first step, we select only pairs with 1″ separations, as described above. In addition, we need to take into account the fact that the mass ratio in systems containing a brown dwarf candidate is highly uncertain, since brown dwarfs cool continuously after formation. Thus, the mass-luminosity relation depends on the highly uncertain age in those cases. We therefore remove all systems containing any component with a spectral type of L0 or later from our further analysis on the mass ratio distribution. However, this also introduces a bias (by preferentially removing systems with low mass ratios) that needs to be accounted for. We do this by generating simulated populations and subjecting them to the same process, as described in the following.

As mentioned above, the most interesting scientific question regarding the mass ratio distribution concerns whether this distribution is best described as uniform, as for the Sun-like primary population, or as rising toward near-equal masses, as in the case of the brown dwarf population and as some star formation simulations predict should be the case also for low-mass stars (Bate, 2012). We therefore generate simulated populations that follow these types of distribution. For each primary mass in our sample, 100 random mass ratios are generated. These are either uniformly distributed between 0 and 1 (to represent the uniform case), or distributed between 0 and 1 in such a way that the probability is directly proportional to the mass ratio (to represent the rising case). In every case where  , the system is removed from the analysis. The full population of all mass ratios for all stars is then compared to our observed sample using a Kolmogorov-Smirnov test (K-S test). Furthermore, this process is repeated 100 times performing the same test, in order to ensure that the result is statistically relevant. When assessing the probability that the two compared samples are drawn from the same distribution, we use the mean probability from the 100 tests. We find that the probability that our observed sample is consistent with a uniform distribution is 63.7%, but the probability for the rising distribution is only 8.9%. The simulated distributions are shown in Fig. 5.

Figure 5: Histogram of mass ratios for the CS sample. Also plotted are the bias-corrected simulated distributions for the uniform and rising cases, normalized to the same number of total systems. The sample is better consistent with uniform distribution than a rising one.

We also make the same comparison of a uniform and rising sample to the Bate (2012) sample of simulated star formation. In this case, we do not remove brown dwarfs since all samples are simulated and have no observational bias. As expected, the Bate (2012) sample provides a better match to the rising distribution with a probability of 39.4%, compared to the uniform distribution which has a probability of 11.1%. Hence, it follows that the mass distribution of our sample of M-stars is better described by a Sun-like uniform distribution, than by a distribution that moderately favors near-equal masses as in the Bate (2012) simulations, which one might have expected for an intermediate continuous population between Sun-like stars and brown dwarfs. This could imply that a sharp gradient or discontinuity occurs somewhere near the star/BD boundary, which would be difficult to consolidate with a common formation mechanism across this mass range. However, this issue should be considered with some caution, given the uncertainties in determining masses for brown dwarfs, as mentioned above. Also, it could for instance be the case that the mass ratio distribution depends on semi-major axis (e.g. Delfosse et al., 2004; Bate, 2009). Here we have studied a relatively wide population of binaries, since we removed ″ binaries from the comparison. The mass ratio distribution of Sun-like stars is similarly dominated by wide binaries since their semi-major axis distribution peaks at such separations. By contrast, the brown dwarf population is dominated by small semi-major axes. A future specific study of M-dwarf multiplicity at small separations would be interesting in this regard (as well as an extensive survey of BD binarity at wide separations).

7.2 Distribution in Semi-Major Axis

Since our survey has a typical inner semi-major axis cut-off at 3 AU which is somewhat comparable to the most interesting region of distinction between the stellar and brown dwarf multiplicity populations at 10 AU, there is reason to proceed with care when determining this distribution in our sample. First of all, we use the CS sample for this purpose, in order to avoid distant targets that might skew the distribution. Also, we make a cut in flux ratio, keeping only binaries with  mag, since there is a gradual loss of sensitivity to fainter companions inside of 1″, which could affect the apparent distribution. Furthermore, we include only stars with primary mass  , since lower-mass stars are not fully complete out to 52 pc and thus have smaller average distances than the full sample, which again could skew the distribution. These cuts leaves a sub-sample of a rather modest size, whose semi-major axis distribution is plotted in Fig. 6.

Figure 6: Histogram of semi-major axes for the CS sample. Also plotted is the bias-corrected simulated distribution for Sun-like stars, as well as a narrower distribution peaking at smaller separations. The sample is inconsistent with a Sun-like distribution, but better consistent with the narrower one.

The distribution appears to peak at smaller semi-major axes and be narrower than the corresponding distribution for Sun-like stars. In order to test this, we simulate binary populations with a Gaussian distribution in logarithmic semi-major axis space, with and from Raghavan et al. (2010). For each star in our statistical sub-sample with a distance , we generate 100 random semi-major axis values following the above Gaussian distribution. In every case where ″ or ″, the simulated pair is removed from the analysis, in order to reproduce the existing bias in the observed population. The simulated population is then compared with the observed population using a K-S test, and this test is repeated 100 times in the same way as described in the previous section. This gives a 5.8% probability that the populations are drawn from the same distribution. As a reference case, we also repeat the same procedure for an example distribution with a lower mean and a narrower width ( and ), which gives a significantly higher probability of 55.5%. Hence, the results imply that M-dwarfs indeed have a semi-major axis distribution that is narrower and peaks at smaller values than for Sun-like stars. At the same time, the distribution seems to peak at larger separations than brown dwarfs, since it starts to drop already at 10 AU, which is probably not a bias-dominated trend, given that the median inner limit of detectability is 3 AU in our sample. This apparently intermediate distribution between Sun-like stars and brown dwarfs could be interpreted as another piece of evidence in favor of a common formation mechanism.

8 Summary and Conclusions

In this article, we have presented results for a high-resolution imaging survey of 761 low-mass stars with the AstraLux Norte and AstraLux Sur cameras, using the Lucky Imaging technique. We have detected 219 companions in 205 multiple systems, of which 182 companions in 171 systems were previously undiscovered. Our census of multiplicity in these young nearby M-stars is potentially useful for a wide range of future applications, such as calibration of theoretical isochrones for low-mass stars and determination of orbital distributions through continued orbital monitoring. The sample should also be useful for future planet-search projects, such as high-contrast imaging surveys, which typically seek to avoid close binaries as targets, or astrometry surveys with planned instruments such as GRAVITY (Eisenhauer et al., 2011), for which close binarity is highly desirable for astrometric referencing purposes.

Our sample also allows us to study the population statistics of M-dwarf binarity. We find that the multiplicity fraction of M0–M5-type stars between separations of 0.08″ and 6″ is %. If we assume that close and wide binarity is uncorrelated with intermediate-range binarity, this implies a total multiplicity fraction in the range of 34%, slightly lower than reported by (Fischer & Marcy, 1992) but consistent within the errors. Furthermore, we find that the multiplicity fraction as function of primary mass in our sample is consistent with a smooth increase in multiplicity with increasing mass across the sample, as might be expected from the fact that the multiplicity is known to be higher for Sun-like stars and yet higher for high-mass stars, and lower for brown dwarfs. The mass ratios of the binary components in our sample on the other hand appear to be fully consistent with a uniform distribution and no preference toward near-equal masses. This is consistent with an equal distribution to Sun-like stars, which is distinct from the distribution of the brown dwarf population and may indicate a rather abrupt change in properties in the vicinity of the star-BD boundary. The semi-major axis distribution is however again consistent with a smooth intermediate stage between stars and brown dwarfs. Hence, the different multiplicity properties give conflicting information about whether or not the transition from stars to brown dwarfs is smooth, and thus whether or not they are best interpreted as sharing a common formation mechanism. On balance, given the two pieces of evidence in favor and the single one against, we consider a common mechanism to be more likely. We emphasize that no final conclusions can be based on these distributions alone, but that they should be interpreted as pieces of evidence in a larger picture, along with other lines of evidence from observations and simulations. Of course, it could also be the case that several different mechanisms are involved in the formation of brown dwarfs and very low-mass stars in overlapping mass ranges (e.g. Dupuy & Liu, 2011; Riaz et al., 2012).

Most of the binaries and higher-order multiples in our sample have been observed at two or more epochs, which allows to confirm common proper motion (as is expected for physical pairs but not for background contaminants) and to get a first handle on orbital motion. The vast majority of point-sources in the AstraLux images are real physical companions, and the large difference in colors between companions and typical background stars allow us to distinguish between these two cases even for the targets that have only been observed in one epoch. Many of the targets show highly significant orbital motion, and could have their complete orbital characteristics determined through further monitoring over a longer baseline.

An even more stringent and fully encompassing census of the multiplicity characteristics of this sample could be acquired through monitoring with radial velocity. This would allow to discover binaries on smaller orbits, as well as to determine accurate mass ratios and various orbital elements of the binaries. In this way, many biases could be removed and a much larger fraction of the sample used for a wider range of statistical applications. We are already studying a subset of targets with this technique, and future spectrographs that are well suited for radial velocity at near-infrared wavelengths, such as CARMENES (Quirrenbach et al., 2010) should be able to further enhance such studies.

We thank all the staff at the Calar Alto and La Silla observatories for their support, and the referee, V.J.S. Béjar, for his useful report. This study made use of the CDS services SIMBAD and VizieR, as well as the SAO/NASA ADS service. Support for this work was provided by NASA through Hubble Fellowship grant HF-51290.01 awarded by the Space Telescope Science Institute, which is operated by the Association of Universities for Research in Astronomy, Inc., for NASA, under contract NAS 5-26555.

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Appendix A Notes on individual binaries and multiple systems

Special remarks on individual systems are summarized below.

J00080642+4757025 In addition to the companion detected with AstraLux, J00080642+4757025 is a close spectroscopic binary with a 4.4 day period (Shkolnik et al., 2010), hence the system is actually a triple.

J00150240-7250326 The AstraLux PSF was strongly asymmetric for this target, hence in addition to the usual PSF fitting, we also performed a customized aperture photometry scheme in order to ensure that the PSF fitting did not provide a biased result. We chose a circular aperture with a 3 pixel radius centered on the primary and the companion respectively. In order to estimate the influence of the primary PSF at the location of the secondary, we adopted the mean of aperture fluxes in two locations at the same separation as the secondary, azimuthally separated from it by 15 pixels in each direction. This mean value was subtracted from the aperture flux of the secondary, thus removing the influence of the stellar PSF. The results are well consistent with the PSF fitting values and the method seems more sensible for this particular type of application, hence we adopt the aperture photometry values for the differential photometry, and let the errors be represented by the scatter between PSF fitting results and the aperture photometry. Note that the photometry values presented here should replace those in Bergfors et al. (2010).

J00193931+1951050 J00193931+1951050 and J00194303+1951117 are separated by only 53″, have very similar proper motions (e.g. Röser et al., 2010) and have similar estimated spectroscopic distances (23 and 21 pc, respectively) in Riaz et al. (2006), hence it is highly likely that they form a physical pair.

J00250428-3646176 Like J00150240-7250326, this stellar binary also had an asymmetric PSF, and we therefore calculated the photometry in the same way as for that case, see the individual note for J00150240-7250326. Note that the photometry values presented here should replace those in Bergfors et al. (2010).

J00424820+3532554 This system is noted as being triple in Tokovinin et al. (2006), including a close spectroscopic binary pair with approximately 1.3 mas separation and a likely wider companion at 11″ separation. Due to these separations however, it is counted as single for our purposes.

J00560596+4153282 The star has a likely companion at 13″ with similar proper motion (e.g. Röser et al., 2010) seen in 2MASS, but appears single closer in, in the AstraLux field of view.

J01034210+4051158 Aside from the companion seen in the AstraLux images, there is an additional possible wide companion at 26″ separation, as noted in the Washington Double Star (WDS) catalog (Mason et al., 2001). The wide components have very similar proper motions (e.g. Röser et al., 2010), so actual companionship seems probable.

J01093874-0710497 This binary displays clear common proper motion, but the residual astrometry does not seem to follow a simple trajectory consistent with only orbital motion of the two visible components. In addition, the brightness difference is larger than the spectral type difference would imply at a common distance. This could indicate that the A component is itself an unresolved binary.

J01132817-3821024 The primary star in the system is a known eclipsing binary with a period of 0.4455 days (Parihar et al., 2009). Since the angular separation is inside of our inner cut-off, we count the system as a binary here for the purpose of multiplicity statistics, although it is really a triple system. To estimate the mass of the primary for the purpose of deriving the mass ratio to the tertiary component detected in our images, we use the sum of the masses corresponding to the individual spectral types, M1 and M3, derived for the eclipsing binary.

J01154885+4702259 In addition to the companion detected with AstraLux, it can be noted that J01154885+4702259 has a very similar proper motion to the star J01155017+4702023 at just 27″ separation (Röser et al., 2010), which is itself a close binary (Law et al., 2008). Thus, this is a very likely quadruple system.

J01452133-3957204 J01452133-3957204 has only been observed in one epoch, but the color and brightness of the detected companion are consistent with expectation, hence we count it as an unconfirmed binary.

J01473248+3453528 This star has a possible wide brown dwarf companion at 43″ separation, according to Casewell et al. (2008).

J01564714-0021127 This is an eclipsing binary with a 0.5 day period (Chen et al., 2006), but it is single in the AstraLux images.

J02002975-0239579 The companion to J02002975-0239579 has yet to be tested for common proper motion, but since its color and brightness are consistent with expectation and its separation is small (0.32″), it is counted as a physical companion here.

J02070176-4406380 J02070176-4406380 and J02070198-4406444 are separated by only 7″ and have similar estimated spectroscopic distances (13 and 21 pc, respectively) in Riaz et al. (2006), hence it is likely that they form a physical pair.

J02155892-0929121 This likely triple system has only been observed in one epoch, hence it remains unconfirmed. The brightnesses and colors of all components are however consistent with expectation for a physical triple.

J02165488-2322133 The companion to J02165488-2322133 has not yet been confirmed to share a common proper motion, but the color and brightness of it are well consistent with a physical companion, hence it is counted as such in the statistics.

J02335984-1811525 There is insufficient motion between the two epochs of observation of J02335984-1811525 to establish common proper motion of the binary, but the components are nearly equal brightness and color, and reside at a relatively small separation of 0.85″  hence it is almost certainly a physical pair.

J02411909-5725185 J02411909-5725185 is yet to be confirmed as a common proper motion binary, but the color and brightness of the companion are well consistent with it being physically bound, hence it is counted as a binary in the statistics.

J02411510-0432177 This star has been classified as a possible T Tau star in the Taurus-Auriga region by Li & Hu (1998).

J02451431-4344102 J02451431-4344102 is a member of an approximately equal-brightness binary with 50″ separation (Mason et al., 2001), in addition to being a close binary discovered with AstraLux.

J02490228-1029220 The system is precisely at the 3 threshold for statistically significant exclusion of the background star hypothesis. By chance, the AB astrometry is just below the criterion (2.7) and BC is just above (3.1), so in principle the BC pair is inconsistent with chance alignment, if the pair does share a common proper motion with A. However, the proper motion of the system has of course been determined based on A, so until the AB physical connection has been demonstrated to the required accuracy, the 3.1 confidence of the BC pair is irrelevant. Hence, we label the entire system as undetermined for now, although it is obviously very likely that the whole system is indeed bound.

J02545247-0709255 The primary is an SB2 binary with an 11.8 day period (Torres et al., 2002). Since the angular separation is inside of our inner cut-off, we count the system as a binary here (unconfirmed, since it has not yet been confirmed to share a common proper motion) for the purpose of multiplicity statistics, although it is really a triple system. To estimate the mass of the primary for the purpose of deriving the mass ratio to the tertiary component detected in our images, we adopt the mass ratio of 0.58 derived from the spectroscopic orbit and use the mass corresponding to an M3 spectral type for the primary.

J03032132-0805153 A possible wide companion to J03032132-0805153 at 172″ with similar proper motion is noted in WDS (Mason et al., 2001).

J03033668-2535329 One or both of the stars in this system must be highly variable. The magnitude differences between the primary and secondary vary from 5.14 mag to 1.72 mag between different observations in Bergfors et al. (2010) and here. In contrast to the individual note on this system in Bergfors et al. (2010), we assume here that the designation LTT 1453 refers to the primary star.

J03042184+2118154 The close (0.40″) companion to J03042184+2118154 is counted as an unconfirmed binary companion, since it has not yet been tested for common proper motion.

J03050976-3725058 This target, like J06583980-2021526, gives conflicting information about whether the AB pair is physically bound. The brightness and color are fully consistent with B being an M3.5 companion to the M2.0 primary. Furthermore, the separation is only 0.2″, and the whole field is otherwise empty. This indicates physical companionship. However, the deviation from the expectation of a background source is only 1.1, and the companion has moved 3.6 times closer to the background expectation than its original position where the motion has a 14 confidence. This, by contrast, suggests a chance alignment. Since the magnitude of motion is not inconsistent with what could be expected for orbital motion of a real physical pair, we keep it as binary in our analysis, but we note that further observations will be necessary in order to resolve this issue satisfactorily.

J03283893-1537171 Also known as GJ 3228A, this star has a wide binary companion at 16″ separation (e.g. Weis, 1991).

J03323578+2843554 This is a close triple system discovered with AstraLux, where in particular the tertiary component is difficult to fit for. Since the relative positions of the BC pair components are therefore clearly dominated by noise scatter in both separation and position angle, we set the error of each epoch to the scatter among the data points and make no assessment of orbital motion for the BC pair (although by contrast, clear orbital motion is seen of the pair with respect to the A component).

J03324345-0855391 J03324345-0855391 is a component in a system with a rather complex history, as it is a spectroscopic binary with a DA white dwarf with a 0.2 day period and has undergone a common envelope phase in the past (e.g. Davis et al., 2010). Hence, it cannot count as a regular M-star, and is not included in the statistical analysis.

J03360868+3118398 This star has been classified as a possible T Tau star in the Taurus-Auriga region by Li & Hu (1998).

J03394784+3328306 Also known as GJ 9119 B, this star is a wide companion to GJ 9119 A at about 14″ as noted in e.g. the WDS catalog (Mason et al., 2001). It is however single in the separation range covered by the AstraLux data.

J03415581-5542287 J03415581-5542287 and J03415608-5542408 are separated by only 12″ and have similar estimated spectroscopic distances (14 and 20 pc, respectively) in Riaz et al. (2006), hence it is likely that they form a physical pair. J03415581-5542287 is a close (0.61″) binary in our data, so the system is likely triple in reality, although common proper motion of all components has yet to be proven.

J03423180+1216225 Since the two epochs of observation were acquired over a baseline of only a few months, there is not yet sufficient motion to confirm common proper motion of the companion that was detected with AstraLux. However, the separation between the components is rather small (0.86″), and the fact that the companion is clearly detected in but too faint in implies that it must be very red, as expected for a real companion. Hence, we count it as a binary system for statistical purposes.

J03461399+1709176 This star has a possible wide companion at about 8″ as noted in e.g. the Washington Double Star (WDS) catalog (Mason et al., 2001). It is however single in the separation range covered by the AstraLux data.

J03472333-0158195 López-Santiago et al. (2006) classify this star as a member of subgroup B4 (a nearby young moving group), with an estimated age of 100 Myr.

J03591438+8020019 A companion to J03591438+8020019 was detected on two separate occasions with AstraLux, in both cases the detection is rather tentative, but since it is detected twice with consistent properties we count it as a genuine detection. However, due to the poor quality of the fit and the fact that the two epochs of observation are only separated by 3 months, we do not try to acquire two epochs of astrometry, but merely quote the astrometry as the mean (and standard deviation) of the two epochs.

J04143060+2851298 J04143060+2851298 and J04143109+2851518, both from the Riaz et al. (2006) sample, are separated by only 23″  and although the estimated spectroscopic distances of 55 and 72 pc are not fully equal, they are consistent to within the 37% error. In addition, they have very similar proper motions (e.g. Röser et al., 2010) and thus probably form a physical pair.

J04244260-0647313 Although this star appears single in our images, it has been identified as a three-component spectroscopic multiple system in Shkolnik et al. (2010). The largest semi-major axis in the system is constrained as 0.25 AU, which at a distance of 35 pc corresponds to approximately 7 mas, hence we should indeed not expect to see any of these components in the AstraLux images.

J04305203-0849193 A known component of the wide binary Konigstuhl 2AB with a separation of 20″ (Caballero, 2007), J04305203-0849193 is single closer in, in the AstraLux images.

J04373746-0229282 Better known as GJ 3305, this binary is part of the Pic moving group (Zuckerman et al., 2001), and is also bound to 51 Eri in a wide orbit (Feigelson et al., 2006) with a projected separation of 66″. The binarity of GJ 3305 was first reported by Kasper et al. (2007), and has been observed with AstraLux on several occasions.

J04374563-0119118 The X-ray flux of this star is probably due to the fact that it is a symbiotic star, as identified by e.g. Belczynski et al. (2000), hence we consider it as a contaminant to the Riaz et al. (2006) sample.

J04465175-1116476 J04465175-1116476 has a companion that has not yet been tested for common proper motion. Since the brightness and color match expectations, the system counts as an unconfirmed binary.

J05100427-2340407 Both J05100427-2340407 and J05100488-2340148 are binaries in the AstraLux images, so since they are separated by only 27″ on the sky and have very similar proper motions (e.g. Röser et al., 2010), this is likely a quadruple system in reality. Common proper motion remains to be confirmed for both of the close components.

J05130132-7027418 There is a companion to J05130132-7027418 in the AstraLux images which has a brightness and color that is consistent with a physical companion. It counts as an unconfirmed binary here, since it has not yet been tested for common proper motion.

J05195412-0723359 J05195412-0723359 and J05195513-0723399, both from the Riaz et al. (2006) sample, are separated by only 16″ and have comparable estimated distances (59 and 70 pc), as well as quite similar proper motions (e.g. Röser et al., 2010), and thus likely form a physical pair.

J05225705-0850119 This star has been classified as a probable T Tau star in Alcala et al. (1996).

J05243648-0535175 There is a possible companion at 7.8″ noted in WDS (Mason et al., 2001), but inside the AstraLux field of view, the star appears single.

J05301858-5358483 The AstraLux images resolve this system into a likely triple, where all components have brightnesses and colors consistent with a physically bound system. Since it has only been observed in one epoch, common proper motion has not yet been established.

J05320450-0305291 J05320450-0305291 is identified as a Pic member in da Silva et al. (2009). It is also known as V1311 Ori.

J05323611-0523010 Also known as HR Ori, this star has been classified as a probable T Tau star in Alcala et al. (1996).

J05343767-0543044 J05343767-0543044 has been classified as a likely member of the 1 Myr Orion OBIc/d association (Stassun et al., 1999). The companion that was detected with AstraLux has not yet been confirmed to share a common proper motion, but its brightness and color are consistent with what would be expected for a physical companion, hence it is counted as such in the statistical analysis.

J05344858-3239362 All components of this triple system have colors and brightnesses consistent with expectation for physical companions. Common proper motion has however not yet been demonstrated.

J05350429-0508125 This star has been classified as a probable T Tau star in Alcala et al. (1996). It is also known as V1321 Ori.

J05355975-0616065 Also known as V1178 Ori, this star has been classified as a probable T Tau star in Alcala et al. (1996). It has a companion that is as of yet unconfirmed with regards to common proper motion, but since the brightness and color are well consistent with expectations for a real companion, the system is counted as binary in the statistics.

J06002304-4401217 The two components resolved by AstraLux have nearly equal brightnesses and colors. Hence, this counts as an unconfirmed binary, since the system has only been observed in one epoch so far.

J06061742-2754050 This star is likely a binary companion to the nearby K1-type star HD 41842 at 20″ separation, as noted in WDS (Mason et al., 2001).

J06112997-7213388 Since the separation between the components of this system is very small (0.16″), it is almost certainly a physical binary, although common proper motion has yet to be demonstrated.

J06134171-2815173 This binary consists of two components with almost equal brightnesses and colors. Although common proper motion has not yet been demonstrated, it thus counts as binary in the statistical analysis.

J06134539-2352077 The close binary pair which was resolved by AstraLux is likely itself a wide companion to the nearby G5-type star HD 43162 at 25″ separation, as noted in WDS (Mason et al., 2001). Hence the system is likely triple, although common proper motion has not yet been deomnstrated.

J06161032-1320422 In Bergfors et al. (2010), we detected a close binary companion to J06161032-1320422 at 190 mas separation. In a re-observation of the target from February 2010, there is no resolved companion detected but only a slightly extended primary PSF, hence the binary separation probably decreased in the meantime.

J06234024-7504327 Although not yet confirmed to share a common proper motion, the companion to J06234024-7504327 is both relatively close 0.57″ and has consistent brightness and color to what should be expected for a physical companion.

J06262932-0739540 The motion in the J06262932-0739540 system is not yet sufficient to determine whether the two components share a common proper motion, but since the separation is small (0.47″) and the colors and brightnesses of the components are consistent with expectation, it is likely that they form a physical pair. The system counts as binary in the statistical analysis.

J06281861-0110504 The companion that was detected in the AstraLux images has not yet been confirmed as a physical companion through common proper motion. However, the two components have nearly equal brightness and colors, and a relatively small separation of 1.4″  hence it is very likely that it is a real physical binary, and it is counted as such here for statistical purposes.

J06351837+4745366 J06351837+4745366 is an unconfirmed binary with regards to common proper motion. Since the brightness and color of the companion is consistent with expectation, we count it as binary in the statistical analysis.

J06583980-2021526 Out of the targets that have been classified as ’undetermined’ with respect to common proper motion, the J06583980-2021526AB pair is one out of two that have reasonable (or even large) chances of being chance alignments rather than physical pairs. The fainter candidates J06583980-2021526C and D at larger separations reported in Bergfors et al. (2010) are clearly identified as background contaminants here, given both the colors and proper motions. However, J06583980-2021526B gives conflicting information. On one hand, its brightness and color are fully consistent with it being an almost equal-mass companion to the primary, which would be a very unusual coincidence for a background object, especially at a separation of only 1.4″. On the other hand, from an astrometric viewpoint, the B component is fully consistent with the expectation for a background object. The deviation from the background expectation is 0.4, and the B component has moved to a position that is 7.4 times closer to the background expectation than its first-epoch position, with a confidence for the motion of 7.5. This is also unlikely to happen by chance, hence the evidence is divergent. Since the magnitude of motion is not inconsistent with what could be expected for orbital motion of a real physical pair, we keep it as binary in our analysis, but we note that further observations will be necessary in order to resolve this issue satisfactorily.

J07115917-3510157 The two components of J07115917-3510157 have nearly equal brightnesses and colors, hence it is very likely that they form a physical pair. They have yet to be demonstrated to share a common proper motion.

J07210894+6739590 In addition to the close binarity discovered in the AstraLux data, there is a star at 21″ separation (HIP 35628), but due to its very different proper motion, it is likely physically unrelated to the J07210894+6739590 system (Reid et al., 2007).

J07282116+3345127 Although the star counts as single in our AstraLux data, it is in reality a spectroscopic binary with less than 0.55 AU semi-major axis, as noted by Shkolnik et al. (2010).

J07382951+2400088 A 2.4″ possible companion to J07382951+2400088 is noted in WDS (Mason et al., 2001), but our AstraLux images show no such companion.

J07505369+4428181 There is a companion to J07505369+4428181 which has a color and brightness that is consistent with what should be expected if it was physcially bound. Common proper motion has not yet been tested for the system.

J08082487+4347557 Although the star counts as single in our AstraLux data, it is in reality a spectroscopic binary with less than 0.02 AU semi-major axis, as noted by Shkolnik et al. (2010).

J08224744-5726530 As noted in Bergfors et al. (2010), this is a triple system with component C outside of 6″. Hence, we do not include component C in Table 4, but we note that at 8.4290.001″ separation in 2008.88 and 8.3740.003″ in 2010.09, there is statistically significant orbital motion also for this component.

J08310177+4012115 For astrometric analysis of J08310177+4012115, we compare our AstraLux measurement with the data from the original discovery as listed in WDS (Mason et al., 2001). Since there are no error bars quoted, it is difficult to formally establish physical companionship. However, even if we assume that the errors are 0.5″ and 5, which should be very conservative, the background hypothesis can still be firmly excluded with 5 confidence. We therefore count it as a confirmed companion.

J08412528-5736021 The two components of this system have nearly equal colors and brightnesses, hence they very likely form a physical pair, althouhg they have not yet been tested for common proper motion.

J08472279-4047381 This star is a known eclipsing binary with a period of 1.6219 days (Parihar et al., 2009), but has no additional companions in the AstraLux field of view.

J08475676-7854532 More commonly known as EQ Cha, this star appears single in the AstraLux images, but has most likely been partially resolved as a close binary in previous imaging campaigns (Köhler & Petr-Gotzens, 2002; Brandeker et al., 2006). With an angular separation as small as 40 mas in 2003, it is fully plausible that the companion exists but was too close to be resolved by AstraLux in 2010.

J08483696-1353087 J08483696-1353087 and J08483645-1353083 are separated by only 7″, the former is a close binary (as of yet unconfirmed by common proper motion) and the latter is single, so this is likely a triple system in reality.

J09053033-4918382 This star has a probably brown dwarf companion, but since only one epoch of data exists, this is still unconfirmed.

J09121259-2555025 J09121259-2555025 has the alternative identifier CD-25 6962B in SIMBAD, implicitly implying companionship with the G2-type star CD-25 6962 at 14″ separation. However, given the apparently very different proper motions of the components (e.g. Röser et al., 2010), we consider such a companionship questionable.

J09164398-2447428 We resolve this star into a close binary (as of yet unconfirmed through common proper motion). It was recently classified as a classical Cepheid based on light curve analysis (Christiansen et al., 2008). We assume that this is a mis-classification, given that the unresolved spectral type is M0.5V.

J09180165-5452332 J09180165-5452332 has a close (0.49″) companion to which it is probably physically bound, although this still needs to be confirmed through common proper motion.

J09365782-2610111 The companion discovered with AstraLux is probably physical given the rather small separation (0.39″), but so far only one epoch of imaging exists.

J09394631-4104029 This star is listed as a Tycho double star in the WDS catalog (Mason et al., 2000) with a separation of 600 mas and equal brightness. However, it appears entirely single in our AstraLux data. Although we cannot strictly rule out that the companion is presently too close to be resolved with AstraLux (e.g. due to a close to edge-on orbit and unfortunate timing of the observation), we consider it relevant to regard the possible companion as unconfirmed at present.

J09423823-6229028 The two components of this binary have almost equal brightnesses and colors, hence they are very likely to form a physical pair. Common proper motion has not yet been tested.

J10023100-2814280 J10023100-2814280 has a relatively close (0.56″) companion which is probably real, although this has yet to be confirmed with a proper motion test.

J09583428-4625300 While the system appears single in the AstraLux images, it is in reality a spectroscopic binary with a 1.88 day period (e.g. Diáz et al., 2007). Such a small orbit is obviously consistent with a non-detection by AstraLux.

J10162867-0520320 In this previously known system, J10162867-0520320 is a spectroscopic binary of two M-dwarfs components, which is in turn a visual companion at 3.2″ separation from a white dwarf (WD). Furthermore, the WD is itself a spectral binary, making the system quadruple, with a demonstrated physical companionship of all four components (Vennes et al., 1999). The 3.2″ pairing is easily distinguished in the AstraLux image, but the spectroscopic pairs remain unresolved. Because the system must primordially have had a pre-WD primary much more massive than J10162867-0520320 (given that the main sequence lifetime of an M0 star is longer than the Hubble time), we do not count it as an M-star binary for any of our statistical purposes. The binary is listed as having confirmed proper motion in Table 4, this is based on the result in Vennes et al. (1999) and not our comparison with the astrometric point in the literature; since no error bars are listed for that point and since we only get rather marginally significant results if we assume reasonable errors of ″ and 1, we do not draw any new conclusions on the basis of such a comparison.

J10181387-2028413 The star is single in the AstraLux images, but has a known wide companion at 32″ separation (Deacon & Hambly, 2007).

J10423011-3340162 The source at 2.4″ separation, first reported in Neuhäuser et al. (2000), is an already known background star (Lowrance et al., 2005), a conclusion which we can confirm at 28 confidence.

J11091380-3001398 This previously known binary (e.g. Webb et al., 1999) is part of the TW Hya association, and is also known as TWA 2.

J11102788-3731520 This previously known binary (e.g. Brandeker et al., 2003) is part of the TW Hya association, and is also known as TWA 3.

J11240434+3808108 There is a possible brown dwarf companion to J11240434+3808108 at 8″ separation noted by Reid et al. (2007), but it is single within the AstraLux field of view.

J11254754-4410267 J11254754-4410267 has a relatively close (0.55″) companion that is likely physically bound, but so far there is only a single epoch of data available.

J11315526-3436272 This system has been identified as a member of the TW Hya association (Kastner et al., 1997) and is known as TWA 5. It contains a previously known brown dwarf TWA 5B, first suggested by Lowrance et al. (1999) and later confirmed by e.g. Brandeker et al. (2003). The latter also reported the presence of a close companion TWA 5Ab at 54 mas from the primary, independently detected by Macintosh et al. (2001). We detect TWA 5B in our AstraLux data, but not TWA 5Ab, which implies that the projected separation was probably smaller in 2010 than it was in 2000. The orbit of TWA 5Aa/Ab has been analyzed in detail by Konopacky et al. (2007). Using the orbital parameters that they determine, we deduce that at epoch 2010.11, the projected separation should be only about 18 mas, which is well consistent with our non-detection of TWA 5Ab. We use the best-fit total mass of 0.71 for TWA 5Aa/Ab from Konopacky et al. (2007).

J12045611+1728119 Common proper motion is shared between J12045611+1728119 and HIP 58919 at 23″ separation, hence they constitute a wide physical pair (Lépine & Bongiorno, 2007).

J12062214-1314559 Due to the small separation (0.42″) of the companion detected in the AstraLux images, it is likely a physical companion, although common proper motion has not yet been tested.

J1206557+700749 Aside from the spatially resolved companion, the primary in the J1206557+700749 system is a known spectroscopic binary with a semi-major axis less than 0.03 AU. This is well consistent with our AstraLux data, where the primary is significantly brighter than the secondary, despite having about equal spectral type. Hence, the system is a triple in reality.

J12134173-1122405 A companion to J12134173-1122405 is detected in the AstraLux images which has not yet been tested for common proper motion, but the color and brightness is consistent with the expectation for a physically bound companion.

J12173945-6409418 The two targets J12173945-6409418 and J12174012-6409389 are physically bound, as shown by common proper motion analysis. However, this means that one of the targets likely has an error in the Riaz et al. (2006) spectral type determination, since J12174012-6409389 is classified as M2 but is fainter than J12174012-6409389, which is classified as M3.5. The fact that J12174012-6409389 is fainter holds true both in 2MASS and in the AstraLux images. Both components are resolved as close binaries with AstraLux, so we consider it a strong candidate for a quadruple system, with J12173945-6409418A as the primary. Concerning which spectral type determination is incorrect, we consider that it is more likely that J12174012-6409389 is mis-classified, as the flux ratio to the close companion is closer to unity than in the J12174012-6409389 case. We thus set the spectral type of J12174012-6409389A to M31, and determine the other spectral types on the basis of flux ratios. Component Bb is not visible in the data, but becomes visible in thanks to the higher Strehl ratio and intrinsic brightness of the component. A fifth object is visible in the field, but its color reveals it to be a likely background star.

J12345629-4538075 J12345629-4538075 is better known as TWA 16. The presence of a close companion to this star was noted in Zuckerman et al. (2001) which seems to be consistent with the companion that we detect. However, since no explicit astrometric information is given in Zuckerman et al. (2001) other than a rough estimation of the separation (0.67″), it is not possible to test whether the companion shares a common proper motion with the primary at this point. The brightness and color are consistent with a physical companion, hence the system counts as binary in the statistics.

J12351726+1318054 The position angle for this system given in Law et al. (2006) is actually 257.0, but since the components are fairly similar in brightness and there is a fake triplet effect, we assume that there can be a 180 phase shift present in the Law et al. (2006) data (or alternatively in both of our epochs). The angular motion in our two AstraLux images is 1.8 in about 0.5 years. If taken at face value, the Law et al. (2006) data point would imply 198.4 angular motion in 4.5 years, corresponding to 22 per half-year, which is an order of magnitude too large. On the other hand, if we subtract 180 from the Law et al. (2006) position angle to get 77.0, then the angular motion is 2.0 per half-year, which is perfectly consistent with our measurements. Hence, we adopt the latter value for our analysis.

J12392104-5337579 The two components of J12392104-5337579 that were detected in the AstraLux images have almost equal brightnesses and color, hence they are very likely physically bound. Common proper motion has not yet been tested.

J12485345+1204326 J12485345+1204326 is a wide (76″) common proper motion companion to HIP 62536 (Lépine & Bongiorno, 2007), but is single in the AstraLux images.

J12533626+2247354 The star shows photometric variability with a 1.9 day periodicity (Norton et al., 2007).

J12565215+2329501 J12565215+2329501 and J12565272+2329506 constitute a known 8″ binary pair in the Reid et al. (2007) sample.

J13013268+6337496 Aside from the binary companion detected in the AstraLux images, the star has a probable wide companion at 119″, as noted in WDS (Mason et al., 2001).

J13015919+4241160 The companion to the J13015919+4241160 is clearly inconsistent with a background contaminant, but the astrometry is also inconsistent with a simple orbital motion of B around A – for instance, the separation decreases from June 2008 to February 2009, but then increases again to June 2009. This could for instance imply that either A or B is a close unresolved binary, where the photo-center shifts on a shorter timescale than that of the AB orbit.

J13022691-5200507 Due to the very compact arrangement of the three components of J13022691-5200507, it is highly probable that this is a physically bound triple system. Futhermore, the system is conspicuously close to the close binary J13025257-5201384 both on the sky and in distance (52 versus 59 pc), hence this is a candidate quintuple system. Only one epoch of imaging exists, so common proper motion has not yet been demonstrated.

J13082484+3019094 Aside from the binary companion detected in the AstraLux images, the star has a possible wide companion at 101″, as noted in WDS (Mason et al., 2001).

J13093495+2859065 Also known as GJ 1167 A, this star has a wide companion at about 190″ according to WDS (Mason et al., 2001).

J13120689+3213179 J13120525+3213332 and J13120689+3213179 constitute a known 26″ binary pair in the Reid et al. (2007) sample, and in addition, each of the components are discovered as close binaries in the AstraLux data. Hence, the system is a very likely quadruple system, although the close pair of J13120689+3213179 has yet to be formally confirmed as physically bound.

J13151846-0249516 Due to the small separation of the companion to J13151846-0249516 it is very likely a physical binary, but common proper motion has not yet been tested for.

J13195689-6831142 J13195689-6831142 has a companion detected in the AstraLux images. Since the companion is relatively close (0.88″) and has a brightness and color that is consistent with expectation, it is probably a physical pair. Only one epoch of images exists so far.

J13293209+5142114 The B component seen in the AstraLux images appears to be a very close binary itself due to a PSF extension visible in five separate epochs. However, we count the system as a regular binary here since we do not get a converging fit for the closer pair.

J13313493+5857171 We count J13313493+5857171 as single close in, although its PSF appears somewhat extended in the 2009.13 epoch. However, it is a likely companion to the nearby G2-star HD 117845 at 11″ separation. HD 117845 has been included in the AstraLux field and appears to be itself a close binary with a 0.5″ separation.

J13345147+3746195 Although the close binarity of J13345147+3746195 was reported in Daemgen et al. (2007) and our AstraLux data have a similar sensitivity, the star appears single in our images. Since the separation was only 82 mas in 2006, it has presumably moved inward since then.

J13493313-6818291 Due to the compact configuration of the three components resolved by AstraLux, the probability is very high for this to constitute a physical triple system. Common proper motion has not yet been tested for.

J13534589+5210298 The secondary detected in the AstraLux images is perhaps itself a close binary, as it appears extended in epochs 2008.64 and 2009.42. However, we count it as a single component of the system here.

J14134677+4618227 J14134677+4618227 is possibly a wide companion to HIP 69518 at 83″ (Reid et al., 2007). It is however single in the AstraLux field of view.

J14201961+2758563 This star is variable, and has been classified as a classical Cepheid based on this variability (Akerlof et al., 2000). We assume that this is a mis-classification, given that the spectral type is K5.

J14204953+6049348 Although the star is single in our AstraLux images, it is known to be a spectroscopic binary with a semi-major axis of 0.01 AU (Shkolnik et al., 2010).

J14402293+1339230 This late-type (M7.5–M8.0) object is classified as a brown dwarf in SIMBAD. It is however unclear what this classification is based on, as our comprehensive search through the full published body of literature available on the object did not turn up any references or justification to such a classification.

J14433804-0414354 The two components resolved by AstraLux have very similar brightnesses and colors, hence physical companionship is probable, although common proper motion has not yet been tested for.

J15090696+5904282 J15090696+5904282 and J15090808+5904258 are separated by only 9″ and have similar estimated spectroscopic distances (30 and 39 pc, respectively) in Riaz et al. (2006), hence it is likely that they form a physical pair.

J15235385+5609320 A probable wide companion to this star at approximately 68″ separation is noted in WDS (Mason et al., 2001).

J15370409+3748275 The star displays photometric variability at a 1.2 day period (Norton et al., 2007).

J15530484+4457446 The close binary that we discovered in the AstraLux images was not seen in the Daemgen et al. (2007) study with a similar spatial resolution, which implies that the projected separation of the system probably increased during the intermediate period.

J15553178+3512028 In addition to the astrometric points listed in Table 4, there is another data point from 2005 in Law et al. (2008). This point is essentially at equal epoch to the Daemgen et al. (2007) point, but the position angle differs by 88 in the two cases. While the Daemgen et al. (2007) data point is fully consistent with all other astrometric points of the target, the Law et al. (2008) point is fully inconsistent in this regard. The close to 90 offset could imply some trivial trigonometric error in Law et al. (2008). Here we simply exclude the point from our analysis.

J16291031+7804399 Like J10162867-0520320, this is a previously known system with a white dwarf component (Farihi et al., 2010). Hence, we do not include this system in the binary fraction statistics.

J16494292+2220037 The star shows photometric variability with a 22.9 day periodicity, which might imply that it is an eclipsing binary (Norton et al., 2007).

J16552880-0820103 Also known as GJ 644, this is a well-known and much studied triple system (e.g. Ségransan et al., 2000), of which we resolve the wider AB pair (the secondary is a spectroscopic binary with a 3 day period). In addition, there are two much wider components known to share a common proper motion with GJ 644, making the system a likely quintuple. Since there are so many existing astrometric points of the AB pair in the literature, we do not give an extensive list in Table 4, but rather refer the reader to (Ségransan et al., 2000), where there is a full orbital analysis of the close triple system.

J16590962+2058160 The star displays photometric variability at a 4.1 day period (Norton et al., 2007).

J17111769+1245408 J17111769+1245408 and J17111841+1245080, both from the Riaz et al. (2006) sample, are separated by only 34″ and have comparable estimated distances (69 and 82 pc), as well as similar proper motions (e.g. Röser et al., 2010), and thus likely form a physical pair.

J17292722+3524048 This star is variable, and has been classified as a classical Cepheid based on this variability (Akerlof et al., 2000). We assume that this is a mis-classification, given that the spectral type is K5.

J17380077+3329457 The B component of the system appears to be a close binary itself in several different epochs of AstraLux imaging, but the suspected Ba/Bb pair is not sufficiently resolved to get a converging binary fit, hence we treat the AB system as a regular binary in this study.

J18153459+1614253 A possible wide companion to J18153459+1614253 at 13″ is noted in WDS (Mason et al., 2001). The star is however single within the AstraLux field of view.

J18351833+4544379 Also known as GJ 720 A, this star has a wide companion with a demonstrated common proper motion at about 112″ according to Lépine & Bongiorno (2007).

J18355276+1659057 J18355276+1659057 is possibly a wide companion to HIP 91159 at 35″ separation, as noted in Reid et al. (2007).

J18464053-0916238 The primary star has two candidate companions in the field of view. The fainter candidate C is most likely a background star, since its color is entirely inconsistent with a late M-type star. The brighter candidate B is more uncertain. It’s colors are fully consistent with the brightness contrast to the primary for a physical companion, implying a spectral type of M5. It is also visible in 2MASS (Skrutskie et al., 2006), which enables to perform a rough CPM test. The test indicates that B is inconsistent with a static background object, again implying physical companionship. However, the motion is also poorly consistent with orbital motion, with a sky-projected speed of order 2 AU per year – highly unlikely for such a wide and low-mass binary. This implies either under-estimated uncertainties in the data, or an unusual astronomical coincidence. With the small separation and relatively high brightness difference of the candidate companion, it is just at the detection limit of 2MASS, and is only reliably detectable in K-band. Perhaps there is a systematic noise component beyond the quoted astrometric 2MASS error in this circumstance. If all the data are taken at face value, another possible interpretation is an unfortunate chance alignment with a local M-dwarf, which has a signficant proper motion of its own. In any case, due to all these uncertainties, we tentatively treat the pair as a candidate binary here, but emphasize that more data is needed to test physical companionship.

J18564143+5014071 J18564143+5014071 and J18564286+5013483 are separated by only 23″ and have similar estimated spectroscopic distances (79 and 77 pc, respectively) in Riaz et al. (2006), as well as very similar proper motions (e.g. Röser et al., 2010), hence it is likely that they form a physical pair.

J19105480+3017476 The AstraLux images reveal three components in the J19105480+3017476 system. Due to their very compact configuration, the triple system is very likely physically bound. Only one epoch of imaging exists so far.

J19213210+4230520 The very close companion resolved by AstraLux is probably physically bound, but this has yet to be tested through proper motion analysis.

J19425324-4406278 A close companion to J19425324-4406278 is detected which is counted as a physical companion for statistical purposes, although this has not yet been demonstrated through common proper motion.

J19432464-3722108 Only one epoch of imaging exists for this binary system, hence common proper motion has not yet been confirmed. It is counted as an unconfirmed binary here.

J20003177+5921289 Aside from the close companion detected in the AstraLux data, J20003177+5921289 possibly has a wide companion at 14″, as noted in WDS (Mason et al., 2001).

J20100002-2801410 Given the relatively small separation (0.62″) and the similar brightnesses of the two components in the J20100002-2801410 system, it is likely that they form a physical pair. However, only one epoch of imaging exists at this point.

J20163382-0711456 Due to the very small separation of the detected companion to J20163382-0711456, this is likely to be a physical binary, although a second epoch to confirm common proper motion has not yet been acquired.

J20500010-1154092 J20500010-1154092 has a close companion detected with AstraLux, but it has not yet been confirmed through common proper motion. However, since the separation is quite small (0.47″) and the brightness and color of the companion is consistent with expectations, the system counts as binary for statistical purposes.

J20564846-0450490 This star has a wide companion at about 14″ as noted in e.g. the WDS catalog (Mason et al., 2001). It is however single in the separation range covered by the AstraLux data.

J20581756+1541315 J20581756+1541315 and J20581836+1541211, both from the Riaz et al. (2006) sample, are separated by only 10″ and have comparable estimated distances (144 and 119 pc), as well as similar proper motions (e.g. Röser et al., 2010) and thus likely form a physical pair.

J21091375-0814041 The binary J21091375-0814041 is as of yet uncomfirmed with regards to common proper motion, but the components have similar colors and brightnesses, and a relatively small separation of 0.97″  hence the pair is probably physically bound, and counts as such in the statistical analysis.

J21154192+1746242 This star possibly has a wide companion at about 9″ as noted in e.g. the WDS catalog (Mason et al., 2001). It is however single in the separation range covered by the AstraLux data.

J21205172-0301545 J21205172-0301545 has a companion with brightness and color that is consistent with expectation, but no common proper motion test has yet been done.

J21295166-0220070 The close companion to J21295166-0220070 has consistent brightness and color with the expectation for a physical companion. Only one epoch of images exists, hence common proper motion has yet to be confirmed.

J21365560-0840313 Due to the small separation (0.24″) of the companion detected in the AstraLux images, physical companionship is very likely, although only one epoch of images exists so far.

J22014336-0925139 The two components of the J22014336-0925139 system that have been resolved with AstraLux have very similar brightnesses and colors, and it is therefore likely that they form a physical binary pair. Common proper motion has not yet been demonstrated.

J22171899-0848122 This system counts as single in our statistics, even though it appears to be a triple system in reality. The reason for this is that the A component was the AstraLux target, and the BC pair at 7.8″ is outside of the completeness cut-off at 6″. Since the BC pair is visible in the AstraLux images, we can nonetheless analyze it astrometrically. This pair was first reported by Beuzit et al. (2004) with ″ and . There are no error bars quoted, but if we assume that the quoted precision in decimal places corresponds to the measurement precision, and adopt errors of 5 mas and 0.5, which should be conservative in that circumstance, we find that common proper motion can be confirmed at a 76 confidence level. Hence, physical companionship can be confidently inferred, even if the errors should be substantially larger than what we have assumed.

J22232904+3227334 Also known as GJ 856, this is a well studied binary with several astrometric data points over a long baseline. In Table 4, we present the AstraLux data as well as one example data point from the literature, and otherwise refer to Seymour et al. (2002) for more information on the astrometric data and a preliminary orbit fit. López-Santiago et al. (2006) classify the system as a member of subgroup B4, with an estimated age of 100 Myr.

J22545501+2414451 This star has a probable wide companion at about 73″ as noted in e.g. the WDS catalog (Mason et al., 2001). It is however single in the separation range covered by the AstraLux data.

J23062378+1236269 In addition to the previously known binary companion seen in the AstraLux images, J23062378+1236269 is also a spectroscopic binary with a semi-major axis smaller than 0.31 AU (Shkolnik et al., 2010), and has the additional wide companion J23062530+1236570 (also in the sample, a single star in the AstraLux images) at 37.6″ with confirmed proper motion (Lépine & Bongiorno, 2007), hence the system is likely quadruple in reality.

J23062928-0502285 The M7.5 spectral type classification of J23062928-0502285 originates from a spectroscopic analysis in Gizis et al. (2000). There is some ambiguity to this classification in that Bouy et al. (2003) find it to be a brown dwarf of type L4. However, the latter estimate is based on a single color, so we consider it less reliable.

J23101857+1447203 The star is classified as T Tau in Li et al. (2000).

J23120603+2655579 As noted in Lépine & Bongiorno (2007), J23120603+2655579 forms a probable wide (14″) pair with HIP 114543, which is itself a 1″ binary. Hence, with the additional component seen in the AstraLux images, the system is likely quadruple.

J23205766-0147373 Although the close binarity of J23205766-0147373 was reported in Daemgen et al. (2007) and our AstraLux data have a similar sensitivity, the star appears single in our images. Since the separation was only 99 mas in 2005, it has presumably moved inward since then.

J23230117-0635436 There is a spectral classification ambiguity for this target, with a K5 classification in Riaz et al. (2006) and a G9III classification in SIMBAD. Regardless of which one is trusted, the star is too early-type to be included in the statistical studies anyway.

J23261707+2752034 A very close (0.15″) companion is detected, which is most likely physically bound, although this has yet to be confirmed with common proper motion.

J23314492-0244395 There is a possible companion at 19″ noted in Lowrance et al. (2005), but it has not been checked for common proper motion.

J23342274+2739556 This star has a possible wide companion at about 63″ as noted in e.g. the WDS catalog (Mason et al., 2001). It is however single in the separation range covered by the AstraLux data.

J23385413-1246184 This late-type (M6.5) object is classified as a brown dwarf in SIMBAD. It is however unclear what this classification is based on, as our comprehensive search through the full published body of literature available on the object did not turn up any references or justification to such a classification.

J23450477+1458573 Due to the compact configuration of the three components resolved by AstraLux, this is almost certainly a physically bound triple system. Only one epoch of images exist so far, hence common proper motion has not yet been demonstrated.

2MASS ID Other name SpT D [pc] J mag Mult. X-ray Sample Norte/Sur
J00053484-0607070 LP 644-34 M2.5 25 9.28 S N IS N
J00063925-0705354 M3.5 14 9.86 M N IS N
J00080642+4757025 M4.0 12 8.55 S Y CS N
J00142956+1331086 K7.0 70 9.34 S Y IS N
J00150240-7250326 M1.0 41 8.62 M Y CS S
J00155808-1636578 M4.0 9 8.74 S Y CS S
J00165001-0710157 M0.0 64 9.58 S Y IS N
J00171443-7032021 M0.5 48 9.00 S Y CS S
J00193931+1951050 M4.0 23 10.93 S N IS N
J00194303+1951117 M4.0 21 10.72 S Y CS N
J00210932+4456560 M3.5 39 9.60 S Y CS N
J00213729-4605331 GJ 3029 M3.0 20 (P97) 8.33 S Y CS S
J00250428-3646176 M2.5 29 8.65 M Y CS S
J00254902+4501315 M3.0 86 11.17 S Y IS N
J00263162+1459223 G 32-18 M4.0 32 10.18 S N IS N
J00275035-3233238 M3.5 28 8.97 S Y CS S
J00281434-3227556 M5.0 12 10.12 S Y CS S
J00325313-0434068 M3.5 12 9.27 M N IS N
J00330109-0342579 M2.5 53 9.97 S Y IS N
J00363616+1725177 M0.5 45 9.55 S N IS N
J00380001+4353454 M0.0 85 10.03 S Y IS N
J00414141+4410530 M2.0 79 10.01 M S IS N
J00424820+3532554 FF And M1.0 24 (P97) 7.16 S Y CS N
J00462185+3522125 M3.0 23 8.93 S N IS N
J00471801-0628378 G 270-70 M3.5 31 10.06 S N IS N
J00485822+4435091 GJ 3058 M3.0 45 9.13 M S IS N
J00501079-0337532 M1.5 77 10.38 S Y IS N
J00503319+2449009 GJ 3060A M3.5 12 (P97) 7.92 M Y CS S
J00535096+2212113 M3.0 75 10.94 S Y IS N
J00544803+2731035 G 69-32 M4.0 19 10.34 S Y CS N
J00551501+3015156 M2.0 58 10.05 S Y IS N
J00560596+4153282 K7.0 81 9.68 S Y IS N
J01025097+1856543 M4.0 13 9.51 S Y CS N,S
J01034210+4051158 G 132-51 K7.0 32 (G04) 9.37 M Y IS N
J01050677+2815049 M3.5 78 11.12 S Y IS N
J01071194-1935359 M1.0 37 8.15 M Y CS S
J01091229+1414096 M0.5 107 10.81 S N IS N
J01093874-0710497 HIP 5443 M1.5 38 (P97) 7.96 M Y CS S
J01105042-4600141 M4.0 20 10.39 S Y CS S
J01112343-0525381 M3.5 35 9.47 S Y CS N,S
J01112542+1526214 GJ 3076 M5.0 9 9.08 M Y CS N
J01123504+1703557 M3.0 54 10.21 S Y IS N
J01132817-3821024 M0.5 50 8.49 M Y CS S
J01132958-0738088 K7.0 65 9.36 M Y IS N
J01154885+4702259 LP 151-21 M4.0 27 10.23 M N IS N
J01192312-0052354 M3.5 26 11.98 S N IS N
J01202841+3302388 M6.0 26 12.21 S N IS N
J01210504-0402082 G 271-42 M0.0 73 9.72 M Y IS N
J01212520+2926143 M3.5 30 9.38 M N IS N
J01225093-2439505 M3.5 45 10.08 S Y CS S
J01231480+2632367 M1.5 47 9.84 S N IS N
J01242767-3355086 GJ 2022 M4.0 15 9.20 M Y CS S
J01244246-1540454 NLTT 4703 M1.5 27 8.11 S Y CS S
J01294256-0823580 M5.0 19 10.65 S N IS N
J01314719+3848032 K5.0 72 9.22 S Y IS N
J01315597-0042237 M4.5 18 12.00 S N IS N
J01345037-0254397 M1.0 74 10.12 S Y IS N
J01351393-0712517 M4.0 10 8.96 S Y CS N
J01362619+4043443 M0.5 65 9.73 S Y IS N
J01365516-0647379 NLTT 5400 M4.0 37 9.70 BG Y CS S
J01365645-0039031 LP 855-20 M3.5 46 11.49 S N IS N
J01385527-0925268 M3.5 30 11.60 S N IS N
J01421511+4845428 LP 648-44 M6.0 29 12.39 S N IS N
J01424628-0309037 LP 152-14 M4.5 24 11.61 S N IS N
J01433150+3904165 M3.5 65 10.12 M S IS N
J01434512-0602400 M3.5 26 8.77 S Y CS N,S
J01452133-3957204 NLTT 5871 M0.0 32 (P97) 8.43 M Y IS S
J01473248+3453528 M3.5 70 10.98 S Y IS N
J01483524-0955226 LP 708-465 M4.0 21 9.53 M N IS N
J01511997+1324525 M1.5 31 8.56 S Y CS N,S
J01535076-1459503 M3.0 25 7.94 M Y CS S
J01555022-0535097 K7.0 71 9.58 S Y IS N
J01564714-0021127 M0.0 81 9.99 S Y IS N
J01583910+4324172 M6.0 29 12.40 S N IS N
J02001277-0840516 M2.5 30 8.77 S Y CS S
J02001278+1303112 M4.5 5 (P97) 7.50 S Y CS N
J02002975-0239579 M3.5 59 10.07 M Y IS S
J02014384-1017295 NLTT 6782 M4.0 17 10.03 S N IS S
J02041831+1318533 K5.0 211 11.33 S Y IS N
J02070176-4406380 M3.5 32 9.27 S Y CS S
J02070198-4406444 M5.5 21 11.36 S Y IS S
J02070786-1810077 M4.0 22 10.70 S Y CS S
J02081218+1508424 NLTT 7084 M4.5 12 9.46 M S IS N
J02132062+3648506 M4.5 12 9.37 M Y CS N
J02133021-4654505 M4.0 15 9.43 M Y CS S
J02155892-0929121 M2.5 27 8.43 M Y CS S
J02164119-3059181 GJ 3148 A M3.5 14 (P97) 7.99 S Y CS S
J02165488-2322133 M3.5 40 9.79 M Y CS S
J02175601+1225266 M3.5 43 9.96 S Y CS N
J02183655+1218579 M2.0 34 8.80 S Y CS N,S
J02224418-6022476 M4.0 10 8.99 S Y CS S
J02255447+1746467 LP 410-22 M4.0 39 10.22 M N IS N
J02271603-2929263 M3.5 57 10.34 M S IS S
J02273726+4710045 M4.0 25 10.34 S N IS N
J02303485-1543248 NLTT 8185 M2.5 39 9.29 S Y CS S
J02313926+4456387 M3.5 24 10.01 S Y CS N
J02333717+2455392 GJ 102 M4.0 8 (J52) 8.44 S Y CS N
J02335984-1811525 M3.0 71 10.09 M S IS S
J02354955-0711214 M5.5 34 12.40 S N IS N
J02365171-5203036 M2.0 28 8.42 S Y CS S
J02411510-0432177 G 75-35 M4.0 11 9.20 S N IS N,S
J02411909-5725185 M3.0 52 9.85 M N IS S
J02414730-5259306 M2.5 27 8.48 S Y CS S
J02451431-4344102 M4.0 9 8.06 M Y CS S
J02461887+4311065 M4.0 22 10.05 S N IS N
J02485260-3404246 M4.0 12 9.31 S Y CS S
J02490228-1029220 M2.0 39 8.82 M Y CS S
J02492136-4416063 M3.0 45 9.88 S N IS S
J02505959-3409050 M4.0 21 10.48 S Y CS S
J02512559+1323125 K7.0 41 8.24 M Y IS N
J02515204+1850218 M3.0 29 9.67 S N IS N
J02515408+2227299 M4.0 10 8.92 S Y CS N
J02543265+3911023 M1.5 34 9.18 S N IS N
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J13062782+4244081 M0.5 90 10.46 S Y IS N
J13082484+3019094 M1.5 64 10.37 M N IS N
J13093495+2859065 GJ 1167 A M3.5 12 (R02) 9.48 S Y CS N
J13101268+4745190 LHS 2686 M4.5 10 (S10) 9.58 S Y CS N
J13101637+2744170 LP 322-879 M4.5 37 12.49 S N IS N
J13102891+2808355 M1.0 203 12.4 S Y IS N
J13120525+3213332 M2.5 44 9.74 M N IS N
J13120689+3213179 M5.0 52 12.48 M N IS N
J13151846-0249516 LP 617-21 M3.5 33 9.80 M N IS N
J13180012+5533121 M0.5 61 9.52 S Y IS N
J13195689-6831142 M1.5 57 9.47 M S IS S
J13233804-2554449 GJ 3780 M3.5 16 (R10) 8.66 S Y CS S
J13283294-3654233 M3.5 43 9.83 S Y CS S
J13293209+5142114 K7.0 100 9.86 M Y IS N
J13313493+5857171 M1.0 56 9.61 S Y IS N
J13322442-0441126 M7.5 19 12.34 S N IS N
J13333371+7029412 M2.5 24 9.20 S N IS N
J13345147+3746195 M3.5 38 9.71 S Y CS N
J13382562-2516466 M3.5 25 8.66 S Y CS S
J13414631+5815197 M3.0 34 8.73 M Y CS N
J13432832+3911404 M0.0 275 12.75 S Y IS N
J13441529+3412299 M1.0 65 10.49 S N IS N
J13454718+8030587 M2.0 162 12.21 S N IS N
J13462649+5304550 M3.5 87 11.38 S Y IS N
J13493313-6818291 M2.0 53 9.50 M+BG Y IS S
J13510548-0519107 LP 678-65 M1.5 42 9.75 S N IS N
J13534190-0045586 M2.5 41 10.65 S N IS N
J13534589+5210298 M3.5 29 9.15 M N IS N
J13584500+3140179 LP 324-42 M4.0 30 10.22 M N IS N
J14071864+6307391 M0.0 107 10.54 S Y IS N
J14095897+1713362 M0.5 59 9.82 S N IS N
J14110874-6155469 M0.5 26 7.78 S Y CS S
J14134677+4618227 M2.0 32 9.41 S N IS N
J14145043+6412442 LP 66-542 M5.0 21 10.82 S N IS N
J14161138+2323297 LP 381-30 M1.0 29 8.67 S N IS N
J14171954+4124239 M3.0 33 10.01 S N IS N
J14190331+6451463 M3.0 61 10.40 BG Y IS N
J14194671+3137037 M4.0 21 9.98 S N IS N
J14201961+2758563 K5.0 62 8.84 S Y IS N
J14204953+6049348 M3.5 45 10.06 S Y CS N
J14252860+6541516 M3.0 22 9.21 S N IS N
J14311348+7526423 M4.0 18 9.77 S N IS N
J14321078+1600494 GJ 3856 M3.0 36 9.29 S N IS N
J14360274+1334484 M2.5 125 11.10 M S IS N
J14372948+4128350 M2.5 54 9.95 S Y IS N
J14402293+1339230 M7.5 19 12.38 S N IS N
J14404355-0058576 LP 620-52 M3.5 26 10.17 S N IS N
J14430789+1720463 K5.0 385 12.66 M Y IS N
J14433804-0414354 M2.0 64 9.51 M S IS N
J14442809-0424078 M2.0 51 9.73 S Y CS N
J14450627+4409393 LP 175-27 M7.5 20 12.44 BG N IS N
J14511044+3106406 G166-49 M3.5 22 8.41 BG Y CS N
J15032251-0040310 M0.5 119 12.29 M N IS N
J15041515-0222573 LP 621-63 M0.5 65 9.88 S N IS N
J15090696+5904282 M4.0 30 11.37 S Y CS N
J15090808+5904258 M2.5 39 9.25 S Y CS N
J15123237+3813362 LP 272-53 M2.0 40 9.75 S N IS N
J15185835+2147521 LP 383-31 M3.0 70 10.82 S N IS N
J15202740+5538502 M5.5 19 11.02 S N IS N
J15210103+5053230 NLTT 40026 M8.0 15 12.00 S N IS N
J15220233+5901172 M3.5 29 9.76 S N IS N
J15235144+5828064 G 224-65 M3.5 42 9.91 S Y CS N
J15235385+5609320 M0.0 44 8.79 S Y CS N
J15271929+4130449 M6.5 26 12.49 S N IS N
J15280061+3431226 M4.5 59 11.19 M N IS N
J15290296+4646240 M4.5 21 9.96 M N IS N
J15312428+1900268 LP 442-66 M2.5 50 10.66 M N IS N
J15323737+4653048 M1.0 33 8.34 S Y CS N
J15370409+3748275 M2.0 66 10.04 M Y IS N
J15403153+1736554 LP 443-39 M3.0 30 9.83 U N N N
J15460540+3749458 M7.5 20 12.44 S N IS N
J15462317+4403148 K7.0 64 9.25 S Y IS N
J15471859+6310599 K5.0 81 9.48 S Y IS N
J15484846+3030388 M3.0 23 8.96 S N IS N
J15492428+4608102 K5.0 88 9.55 S Y IS N
J15530484+4457446 M3.5 47 10.14 U Y N N
J15553178+3512028 GJ 3928 M4.0 11 9.00 M Y CS N
J15565823+3738137 M2.5 42 9.42 S Y CS N
J15584213+3230460 K5.0 70 9.18 S Y IS N
J15594729+4403595 M1.0 35 8.51 M Y CS N
J16151006+3151495 M5.0 16 10.33 S N IS N
J16152207+5230320 M2.5 58 10.97 S N IS N
J16155939+3852102 M0.0 53 9.02 S Y IS N
J16232165+6149149 M2.5 68 10.08 M Y IS N
J16241856+7754086 M2.0 56 9.87 S Y IS N
J16291031+7804399 K7.0 151 11.00 M Y N N
J16363309+6353452 M2.0 64 10.19 M S IS N
J16411543+5344110 M0.0 72 9.34 M S IS N
J16460779+4142057 M2.5 65 10.38 BG Y IS N
J16470576+4117062 LP 225-65 M6.0 25 12.14 S N IS N
J16480454+4522429 M4.0 32 9.38 S Y CS N
J16494292+2220037 K7.0 38 7.89 S Y IS N
J16503028+2319353 K5.0 143 10.59 BG N IS N
J16505199+4928430 K7.0 109 10.47 S N IS N
J16510995+3555071 LP 276-29 M4.0 53 10.30 M Y IS N
J16544298+4654335 V781 Her M3.0 77 10.88 S Y IS N
J16552880-0820103 GJ 644 M2.0 6 (P97) 5.27 M Y CS N
J16575029+5638355 M3.0 67 10.60 S Y IS N
J16581746+1738350 M4.0 34 10.30 S N IS N
J16590404+3822593 M3.0 79 11.06 S Y IS N
J16590962+2058160 M3.0 26 8.34 M Y CS N
J16594764+3657533 M2.5 48 9.72 S Y CS N
J17021204+5103284 M0.5 74 9.35 M Y IS N
J17035283+3211456 LP 331-57 M3.0 21 7.89 M Y CS N
J17111769+1245408 M2.0 69 10.29 S Y IS N
J17111841+1245080 M3.0 82 11.19 S N IS N
J17235678+1338204 M3.5 24 9.52 S Y CS N
J1724591+210838 M2.0 28 9.02 M N IS N
J17250940-0633536 M0.5 63 9.26 M Y IS N
J17261439+1404364 K7.0 86 9.76 BG Y IS N
J17261525-0311308 M4.5 17 10.38 S Y CS N
J17292722+3524048 K5.0 86 9.59 S Y IS N
J17302672+3344522 M3.0 25 9.46 S N IS N
J17363485+4549324 M3.5 32 9.90 S N IS N
J17365925+4859460 M2.5 43 9.50 S Y CS N
J17380077+3329457 K7.0 63 8.52 M Y IS N
J17402734+1616540 M2.0 79 10.59 S Y IS N
J17520294+5636278 M3.5 31 9.23 S Y CS N
J18014229+2758009 M3.5 44 9.90 S Y CS N
J18021660+6415445 G 227-22 M5.0 6 8.54 S Y CS N
J18043871+1354143 M2.5 29 9.47 S N IS N
J18061809+7249162 NLTT 46021 K7.0 43 8.46 S N IS N
J18064367+6822031 M2.0 48 9.69 BG Y CS N
J18083702-0426259 HIP 88871 K5.0 134 (P97) 5.77 S Y IS N
J18095976+5155083 M2.0 43 9.25 S Y CS N
J18110625+3543573 M0.5 62 9.60 M S IS N
J18111491-0101116 M3.5 51 10.19 S Y CS N
J18153459+1614253 M1.5 31 9.02 S N IS N
J18154890+5244006 M2.5 58 10.11 S Y IS N
J18162484+5013570 M0.5 94 9.88 M S IS N
J18172513+4822024 M2.0 21 7.77 S Y CS N
J18184588+3146403 M2.0 75 10.51 S Y IS N
J18200570+6343427 M2.0 68 11.02 S N IS N
J18224710+4434427 K5.0 74 9.34 S Y IS N
J18315610+7730367 LP 24-256 M4.0 16 10.07 S Y CS N
J18323941+4806013 M3.0 63 10.49 S Y IS N
J18351833+4544379 HIP 91128 M0.0 15 (P97) 6.92 S N IS N
J18353790+3259545 M8.5 6 10.27 S N IS N
J18355276+1659057 M3.5 21 9.60 S N IS N
J18361922+1336261 G 141-21 M4.0 19 8.19 S Y CS N
J18373180+2030424 M5.5 18 11.07 S N IS N
J18390173+3459097 M3.0 50 10.06 S Y CS N
J18393839+1623136 M0.0 62 9.35 S Y IS N
J18413741+3942123 GJ 4096 M4.0 30 9.22 S Y CS N
J18421322+1907549 M3.5 35 10.28 S N IS N
J18441139+4814118 M2.5 48 9.86 S Y CS N
J18464053-0916238 M0.0 50 8.93 M+BG Y CS N
J18471129+2212413 M3.5 44 9.63 M+BG Y CS N
J18495543-0134087 M2.5 49 9.78 S Y CS N
J18550451+4259510 M4.0 14 9.78 S Y CS N
J18554528+3720193 K5.0 92 9.72 S N IS N
J18564143+5014071 M2.0 79 10.71 S Y IS N
J18564286+5013483 M1.5 77 10.44 S Y IS N
J18592937-0403042 K5.0 128 9.82 M S IS N
J19051335+3845050 M3.5 23 9.36 S N IS N
J19105480+3017476 M1.5 42 9.58 M N IS N
J19145001-0823400 HD 179944 K5.0 22 6.70 S Y IS N
J19213210+4230520 M2.0 27 8.65 M Y CS N
J19224005-0612076 M2.5 83 10.59 M S IS N
J19224278-0515536 K5.0 103 9.92 S Y IS N
J19425324-4406278 M3.5 51 9.43 M Y CS S
J19430726+4518089 M5.5 21 11.33 S N IS N
J19432464-3722108 M3.5 32 9.20 M Y CS S
J19435432-0546363 M4.0 37 9.75 S Y CS N
J19465050-0157397 M3.0 17 8.55 S N IS N
J19513587-3510375 M4.0 8 8.58 S Y CS S
J20003177+5921289 M4.0 26 9.65 M Y CS N
J20091824-0113377 M5.0 10 9.42 S Y CS N
J20100002-2801410 M3.0 32 8.65 M Y CS S
J20113029+1321373 K5.0 74 9.18 S Y IS N
J20113960-0235257 K5.0 55 8.55 S N IS N
J20163382-0711456 M0.0 50 8.59 M S IS N
J20194981-5816431 M6.0 12 10.66 S Y IS S
J20290922-0526165 M1.5 75 10.44 S N IS N
J20320370-0203181 M4.0 112 12.08 S N IS N
J20343383+1739508 M0.5 23 7.69 S N IS N
J20364367-0019545 K5.0 167 10.93 S Y IS N
J20393534-0402327 K7.0 96 10.22 S Y IS N
J20465795-0259320 M0.0 57 9.12 S Y IS N
J20483385+1952450 M4.0 33 10.15 S N IS N
J20500010-1154092 M3.5 40 9.68 M N IS S
J20523149-0147089 LP 636-16 M4.5 22 10.90 S Y CS N
J20530910-0133039 M5.0 17 10.69 S N IS N
J20531465-0221218 LP 636-19 M3.0 41 9.33 M S IS N
J20564846-0450490 HIP 103393 M4.0 18 (P97) 8.05 S Y CS N
J20581756+1541315 M3.5 144 12.47 S N IS N
J20581836+1541211 M0.0 119 10.80 S N IS N
J20584192-0116316 M3.0 56 10.33 S Y IS N
J21010793-4158536 M0.0 52 8.98 S Y CS S
J21025150-0702487 M3.5 74 11.14 S N IS N
J21032686+1616569 M3.0 80 11.08 S Y IS N
J21035992+1218570 M3.5 142 11.81 M N IS N
J21044799-0418264 M4.0 40 9.88 S Y CS N
J21072409-0958253 M2.5 80 10.81 S Y IS N
J21073678-1304581 M3.0 27 8.73 S Y CS S
J21090888-0940187 K5.0 96 9.69 S N IS N
J21091375-0814041 M1.5 98 10.50 M Y IS N
J21100162-0605112 K5.0 368 12.68 S N IS N
J21103147-2710578 M4.5 16 10.30 S Y CS S
J21141395-0702503 M3.5 13 9.98 S N IS N
J21150531-0949414 M0.0 175 11.70 BG N IS N
J21154192+1746242 M3.0 45 9.90 S Y CS N
J21170412-0706363 M4.0 58 12.80 S N IS N
J21203506+3419476 M3.5 33 9.70 M N IS N
J21205172-0301545 LP 697-26 M4.0 17 10.20 M N IS N
J21235271-3908176 M3.5 32 9.33 S Y CS S
J21295166-0220070 M0.0 101 10.15 M Y IS N
J21365560-0840313 K7.0 86 9.67 M N IS N
J21372900-0555082 M3.0 25 8.80 M N IS N
J21373116-1014250 LP 458-43 M4.0 16 10.28 S N IS N
J21374917-0757145 M3.5 45 10.02 S N IS N
J21375368-0444383 M4.0 59 12.79 U N N N
J21422932+1233175 M1.0 120 11.19 M N IS N
J21490738+1819354 M5.0 33 11.80 S N IS N
J21505366-0553186 M1.0 51 9.38 S Y CS N,S
J21511011-1141181 M7.0 18 12.06 S N IS N
J21525841-0056000 M2.5 86 11.07 S N IS N
J21550017-0722138 M1.5 77 11.25 S N IS N
J21551741-0045478 M4.5 24 11.09 S Y CS N
J21552420-0238247 M4.0 22 10.66 S N IS N
J21574119-5100221 GJ 841 A M2.5 16 (P97) 6.75 S Y CS S
J22012831-0509201 M2.5 139 12.06 S N IS N
J22014336-0925139 M1.5 79 9.89 M S IS N
J22042147+1505517 M5.5 17 10.87 S N IS N
J22114208-2044181 M3.5 39 9.65 S Y CS S
J22145556-0913037 M1.5 48 10.35 S N IS N
J22171899-0848122 GJ 852 A M4.0 10 (H80) 9.02 S Y CS S
J22174316-1546452 M4.0 22 10.79 S N IS S
J22184009-5326405 M2.5 37 9.24 S Y CS S
J22191380+3829594 M0.0 75 9.83 S Y IS N
J22202418-0727341 M1.5 56 9.81 S Y IS N
J22230696-1736250 GJ 4274 M4.0 7 (A95) 8.24 S Y CS S
J22232904+3227334 GJ 856 A M3.0 16 (P97) 6.90 M Y CS N
J22240821+1728466 M4.0 22 10.26 M Y CS N
J22250174+3540079 M2.0 31 8.57 S Y CS N
J22274882-0113527 M3.5 36 9.48 S Y CS N
J22294694-0432036 M0.0 94 10.31 S N IS N
J22332264-0936537 GJ 4282 M2.5 36 8.53 M Y CS S
J22382974-6522423 GJ 865 M3.5 15 (P97) 7.27 M Y CS S
J22401867-4931045 M5.5 10 9.84 M S IS S
J22413577+2602128 M3.0 31 9.04 BG N IS N
J22432021+1413016 K5.0 96 9.83 S Y IS N
J22434378+1916544 M3.0 25 9.30 S N IS N
J22473764+4041253 LP 237-32 M4.0 20 10.36 S Y CS N
J22495622+1744414 M0.0 83 9.74 M N IS N
J22515348+3145153 HIP 112909 M3.0 14 (P97) 7.70 S Y CS N
J22544453+3929017 LP 289-19 M6.5 25 12.47 S N IS N
J22545501+2414451 M2.0 90 10.92 S Y IS N
J22560818-0009597 K7.0 73 9.51 S Y IS N
J22581643-1104170 M2.5 23 9.05 U N N N
J23025250+4338157 M4.0 15 9.31 S Y CS N
J23062378+1236269 HIP 114088 M0.5 37 (P97) 8.36 M Y CS N
J23062530+1236570 G 67-47 M2.5 37 (G04) 11.35 S N IS N
J23062928-0502285 M7.5 12 11.37 S N IS N
J23080940+4514402 M7.0 22 12.47 S N IS N
J23095418-0437284 LP 702-109 M1.5 57 10.61 S N IS N
J23101857+1447203 M4.0 23 10.79 S Y CS N
J23115362-4508004 HD 218860B M3.0 44 9.72 S Y CS S
J23131671-4933154 M4.0 15 9.76 S Y CS S
J23172807+1936469 GJ 4326 M3.0 21 8.02 M Y CS N
J23173353+3700166 M1.0 36 8.52 S Y CS N
J23181817-0239323 M0.5 93 11.25 S N IS N
J23205766-0147373 LP 642-48 M4.0 12 9.36 S Y CS N
J23213759+2944238 M0.0 114 10.67 S Y IS N
J23221088-0301417 K7.0 53 8.73 S Y IS N
J23230117-0635436 HD 220338 K5.0 25 6.87 S Y IS N
J23261069-7323498 M0.0 46 8.84 S Y CS S
J23261182+1700082 M4.5 17 9.30 M N IS N
J23261707+2752034 M3.0 31 8.46 M Y CS N
J23285763-6802338 M2.5 38 9.26 S Y CS S
J23292570-0417338 M2.0 60 10.05 S Y IS N
J23301129-0237227 M6.0 13 10.68 S N IS N
J23314492-0244395 AF Psc M4.5 11 9.51 S Y CS N,S
J23314763-0625502 M4.5 12 9.83 S N IS N
J23320018-3917368 M3.0 29 8.90 S Y CS S
J23321568-0118184 M0.5 117 11.01 S N IS N
J23323085-1215513 M0.0 25 7.45 S Y CS S
J23324655-1645081 Gl 897 M2.5 12 6.71 S Y CS S
J23331860+2714219 G 128-76 M3.0 37 9.35 S Y CS N
J23341101-1531012 M0.0 47 8.91 S Y CS S
J23342274+2739556 M1.5 57 9.75 S Y IS N
J23353509-0613302 M4.0 35 12.00 U N N N
J23385413-1246184 M6.5 26 12.18 U N N N
J23415498+4410407 HH And M5.0 3 (H80) 6.88 S Y CS N
J23430224-0148163 K5.0 68 9.00 S Y IS N
J23443838-0851082 M2.5 151 12.24 S N IS N
J23450477+1458573 G 68-39 M1.0 59 9.41 M N IS N
J23452225-7126505 M3.5 48 10.19 S Y CS S
J23474694-6517249 M1.5 42 9.10 S Y CS S
J23483610-2739385 GJ 4362 M2.5 24 (R10) 8.58 S Y CS S
J23495365+2427493 M3.5 51 9.88 M Y CS N
J23495384+2721406 G 130-14 M3.5 44 9.89 S Y CS N
J23500639+2659519 M3.5 47 10.18 S Y CS N
J23512227+2344207 G 48-46 M4.0 14 9.68 S Y CS N
J23513366+3127229 M2.5 50 9.82 S Y CS N
J23532520-7056410 M3.5 24 8.68 S Y CS S
J23545147+3831363 M4.0 13 8.97 S Y CS N
J23551649-0235417 M4.0 14 9.66 M N IS N
J23555512-1321238 NLTT 58441 M2.5 39 9.26 S Y CS S
J23570417-0337559 M4.0 71 10.90 M N IS N
J23571934-1258406 GJ 4379 B M3.0 32 9.13 S Y CS S
J23572056-1258487 GJ 4378 A M4.0 23 8.64 S Y CS S
J23581366-1724338 NLTT 58589 M2.0 40 8.31 M Y CS S
J23584033-0306535 K7.0 162 11.19 S N IS N
Distance is spectroscopic distance except for cases indicated by an acronym. Parallax distances: J52 (Jenkins et al., 1952),
H80 (Harrington & Dahn, 1980), A95 (van Altena et al., 1995), P97 (Hipparcos; Perryman et al., 1997), R02 (Reid & Cruz, 2002),
G04 (Gould & Chanamé, 2000), R04 (Reid et al., 2004), H06 (Henry et al., 2006), L09 (Lépine et al., 2009), R10 (Reidel et al., 2010),
S10 (Smart et al., 2010). Kinematic distances: M05 (Mamajek, 2005). The uncertainty in the spectroscopic distances is 37%.
Multiplicity status as observed with AstraLux. M: Multiple system. S: Single star. BG: Confirmed or suspected background star.
U: Unclear case.
Flag for whether X-ray emission is detected at 3.3 (Y) or not (N), see Sect. 4 for details.
This column lists membership of IS or CS (members of neither are marked with N). See Sect. 4 for details.
Observed with AstraLux Norte (N) or Sur (S).
Table 1: continued.
2MASS ID (mag) (mag) (″) () Epoch New
J00063925-0705354AB 1.170.05 1.510.01 0.2500.001 5.50.4 2008.88 Y
J00150240-7250326AB 2.650.03 2.720.08 0.2900.009 69.10.3 2008.86 Y
J00250428-3646176AB 3.340.23 3.650.21 0.6050.012 242.40.3 2008.86 Y
J00325313-0434068AB 2.530.06 3.170.02 0.4280.006 179.20.9 2008.88 Y
J00414141+4410530AB 0.360.11 0.240.07 0.5790.001 11.40.3 2008.59 Y
J00485822+4435091AB 0.200.11 0.170.01 1.0530.002 254.20.3 2008.59 N
J00503319+2449009AB 0.820.04 0.900.01 1.3200.001 319.00.3 2008.59 Y
J01034210+4051158AB 0.680.01 0.810.01 2.4770.001 96.80.3 2008.64 N
J01071194-1935359AB 0.630.05 0.510.02 0.4260.002 169.70.3 2010.08 Y
J01093874-0710497AB 1.870.03 2.010.01 2.4850.015 75.90.3 2008.64 Y
J01112542+1526214AB 1.110.11 1.230.10 0.2930.002 205.30.3 2008.88 N
J01132817-3821024AB 0.170.01 0.170.01 1.4150.001 27.20.3 2010.09 Y
J01132958-0738088AB 4.550.08 5.180.12 2.9450.007 227.630.3 2007.85 Y
J01154885+4702259AB 0.930.05 0.890.10 0.2710.001 267.60.4 2008.88 Y
J01210504-0402082AB 2.880.18 3.140.23 4.5390.001 137.20.3 2008.64 Y
J01212520+2926143AB 0.570.15 0.680.10 0.2600.001 310.00.3 2008.87 Y
J01242767-3355086AB 0.100.01 0.070.01 2.0620.002 43.20.3 2010.08 N
J01433150+3904165AB 0.230.83 0.200.77 0.1630.004 273.80.3 2008.88 Y
J01452133-3957204AB 2.000.10 2.390.16 0.9430.009 130.90.3 2008.86 Y
J01483524-0955226AB 0.620.18 0.680.18 0.4850.001 154.20.3 2008.87 Y
J01535076-1459503AB 0.040.01 0.050.01 2.8790.001 291.80.3 2010.08 Y
J02002975-0239579AB 0.750.06 0.890.05 0.3230.001 5.90.3 2008.87 Y
J02081218+1508424AB 0.010.03 0.030.03 3.6170.004 238.30.3 2008.03 N
J02132062+3648506AB 2.130.08 2.400.10 0.1810.002 56.52.2 2007.61 Y
J02133021-4654505AB 0.990.02 0.790.10 0.1380.005 96.40.9 2010.11 Y
J02155892-0929121AB 2.620.05 2.800.05 0.6310.001 292.20.3 2008.87 Y
J02155892-0929121AC 4.990.05 5.520.10 3.5090.002 299.30.3 2008.87 Y
J02165488-2322133AB 0.920.01 0.950.01 4.3740.004 313.60.3 2010.09 Y
J02255447+1746467AB 1.270.05 1.170.24 0.0990.001 278.41.9 2008.87 Y
J02271603-2929263AB 1.490.05 1.730.03 1.8010.012 232.50.3 2010.10 Y
J02335984-1811525AB 0.000.01 0.000.01 0.8390.006 49.00.3 2010.09 Y
J02411909-5725185AB 1.190.02 1.370.01 1.5040.007 286.80.3 2010.11 Y
J02451431-4344102AB 0.750.03 0.840.04 0.3670.001 184.40.3 2010.09 Y
J02490228-1029220AB 1.270.01 1.510.03 0.4930.002 210.50.3 2010.09 Y
J02490228-1029220BC 0.200.04 0.290.07 0.1570.001 217.40.8 2010.09 Y
J02512559+1323125AB 3.850.05 4.340.05 4.0810.004 15.40.3 2008.64 Y
J02545247-0709255AB 2.270.03 2.520.02 4.1650.011 285.30.3 2010.09 Y
J02594789-0913109AB 3.710.10 0.5950.008 319.90.7 2008.88 Y
J03033668-2535329AB 1.720.01 1.830.01 0.8230.003 3.50.3 2010.08 Y
J03042184+2118154AB 3.020.07 2.920.07 0.4010.001 300.00.3 2008.64 Y
J03050976-3725058AB 1.030.01 1.120.05 0.2290.005 47.70.3 2010.09 Y
J03323578+2843554AB 0.680.03 0.790.06 0.5250.001 106.40.3 2008.88 Y
J03323578+2843554AC 2.380.09 2.630.17 0.1580.016 282.42.0 2008.88 Y
J03415581-5542287AB 1.790.05 2.160.16 0.6080.004 262.50.3 2010.10 Y
J03423180+1216225AB 5.200.27 0.8660.008 17.80.4 2008.87 Y
J03591438+8020019AB 2.300.23 0.2000.006 356.73.3 2009.01 Y
J04071148-2918342AB 1.920.04 2.660.13 0.3130.003 45.40.3 2010.10 Y
J04080543-2731349AB 1.090.06 1.400.07 0.2210.003 216.70.7 2010.09 Y
J04132663-0139211AB 1.680.01 2.030.04 0.7590.003 178.20.3 2010.10 N
J04373746-0229282AB 1.340.01 3.730.01 0.2840.003 18.50.6 2010.10 N
J04441107-7019247AB 0.770.01 1.040.01 2.6360.001 156.30.3 2010.11 N
J04465175-1116476AB 0.400.13 0.620.16 1.4970.002 281.00.3 2008.87 Y
J04595855-0333123AB 1.420.05 1.550.07 0.1410.001 302.70.7 2010.08 Y
J05024924+7352143AB 1.270.15 1.220.05 0.3010.001 82.50.3 2008.88 Y
J05100427-2340407AB 0.420.01 0.450.02 0.5220.001 128.30.3 2010.08 Y
J05100488-2340148AB 0.400.01 0.470.01 1.8150.003 307.00.3 2010.08 Y
J05115301-5246286AB 3.570.05 4.520.05 4.8320.012 36.30.3 2010.09 Y
J05130132-7027418AB 1.890.01 1.990.01 1.6650.006 39.70.3 2010.11 Y
J05191382-0059423AB 0.240.15 0.230.15 1.1510.002 211.60.3 2008.87 Y
J05195412-0723359AB 0.580.08 0.710.08 0.7140.002 195.60.3 2008.88 Y
J05195513-0723399AB 2.460.07 2.680.08 0.5100.002 303.90.3 2008.88 Y
J05225705-0850119AB 0.350.06 0.520.07 0.6820.001 112.50.3 2008.88 Y
J05234434-0753375AB 0.420.20 0.360.19 0.4450.005 189.10.3 2008.88 Y
J05241914-1601153AB 0.370.01 0.430.03 0.6130.001 68.50.3 2010.09 Y
J05254166-0909123AB 0.630.01 0.690.02 0.6450.001 54.90.3 2010.09 N
J05301858-5358483AB 0.730.03 0.830.02 0.2320.001 291.90.3 2010.09 Y
J05301858-5358483AC 3.120.02 3.450.01 4.3980.009 327.70.3 2010.09 Y
J05320450-0305291AB 1.050.01 1.280.02 0.2160.003 41.01.1 2010.09 Y
J05343767-0543044AB 1.440.03 1.740.03 1.4370.001 267.40.3 2008.87 Y
J05344858-3239362AB 1.580.01 1.790.01 2.1330.005 161.30.3 2010.09 Y
J05344858-3239362BC 0.670.01 0.800.01 0.4410.001 186.60.3 2010.09 Y
J05350429-0508125AB 5.260.01 5.770.01 4.1310.001 163.90.3 2008.88 Y
J05355975-0616065AB 1.970.01 2.330.01 1.1700.001 17.00.3 2008.88 Y
J05464932-0757427AB 5.550.11 6.200.12 2.8430.020 115.20.3 2009.13 Y
J05494272-1158500AB 1.140.02 1.160.01 3.5030.007 110.20.3 2010.08 Y
J06002304-4401217AB 0.040.01 0.090.01 1.9270.006 285.30.3 2010.08 Y
J06012540-3225168AB 1.010.01 1.110.01 5.2140.005 16.10.3 2010.09 Y
J06112997-7213388AB 1.210.04 1.160.08 0.1640.002 316.60.3 2010.11 Y
J06134171-2815173AB 0.000.01 0.070.01 1.0560.003 359.10.3 2010.11 Y
J06134539-2352077AB 1.370.02 1.490.04 0.1450.002 320.00.5 2010.10 Y
J06161032-1320422AB 1.940.12 1.400.23 0.1940.008 170.60.3 2008.87 Y
J06234024-7504327AB 1.450.04 1.590.06 0.5660.005 97.70.3 2010.11 Y
J06262932-0739540AB 0.480.11 0.490.10 0.4650.002 84.60.3 2008.88 Y
J06281861-0110504AB 0.030.05 0.060.02 1.4320.001 152.80.3 2008.88 Y
J06351837+4745366AB 2.170.06 2.260.07 3.9350.003 264.90.3 2008.88 Y
J06434532-6424396AB 0.940.07 1.130.03 0.2710.008 13.00.6 2010.11 N
J06434532-6424396AC 2.120.01 2.670.01 0.9350.006 295.10.3 2010.11 N
J06583980-2021526AB 0.240.01 0.300.01 1.4450.004 197.20.3 2010.10 Y
J07102991-1637350AB 1.020.01 0.920.05 0.5580.003 355.10.3 2010.09 Y
J07105990-5632596AB 1.880.02 2.110.02 1.1190.002 309.20.3 2010.10 Y
J07115917-3510157AB 0.000.01 0.110.01 1.0290.006 32.90.3 2010.09 Y
J07210894+6739590AB 1.770.07 2.310.03 0.1740.002 58.81.2 2008.87 Y
J07223179+7305048AB 0.690.28 0.920.28 0.2370.002 195.30.6 2008.87 Y
J07285137-3014490AB 1.200.02 1.470.03 0.4640.001 176.40.3 2010.08 N
J07293108+3556003AB 1.150.12 1.280.08 0.1980.001 261.50.3 2008.88 Y
J07313848+4557173AB 1.130.04 1.410.15 0.2060.001 353.02.2 2009.13 Y
J07505369+4428181AB 0.720.33 0.990.23 2.0310.001 141.50.3 2007.84 Y
J08031018+2022154AB 0.730.19 0.880.15 0.2000.002 48.40.8 2009.13 Y
J08125835-1031581AB 1.440.01 1.700.01 2.6690.002 314.20.3 2008.87 Y
J08224744-5726530AB 1.060.01 1.170.01 0.7220.003 137.50.3 2010.09 Y
J08310177+4012115AB 0.160.02 0.130.02 1.8990.001 121.80.3 2008.02 N
J08412528-5736021AB 0.080.01 0.100.01 1.4670.001 348.30.3 2010.09 Y
J08445566-0637259AB 0.600.14 0.650.14 0.2760.007 22.00.3 2008.87 Y
J08472263-4959574AB 0.220.01 0.320.01 1.8350.001 13.50.3 2010.10 N
J08483696-1353087BC 0.580.01 0.620.00 0.3620.001 169.00.3 2010.09 Y
J08540240-3051366AB 3.030.02 3.280.02 1.7320.010 157.30.3 2010.09 N
J09053033-4918382AB 4.860.06 5.500.06 4.1850.012 258.70.3 2010.08 Y
J09075823+2154111AB 0.920.10 1.080.09 0.1070.001 192.51.1 2008.88 Y
J09164398-2447428AB 0.920.07 0.900.21 0.0760.012 160.51.5 2010.08 Y
J09174473+4612246AB 0.450.13 0.360.12 0.2540.001 65.30.6 2008.87 Y
J09180165-5452332AB 1.180.02 1.180.02 0.4860.001 83.10.3 2010.08 Y
J09345604-7804193AB 1.680.07 1.740.06 0.4310.005 344.20.3 2010.10 N
J09365782-2610111AB 0.540.04 0.600.03 0.3890.004 279.50.8 2010.08 Y
J09423823-6229028AB 0.200.01 0.300.01 1.2880.004 264.00.3 2010.10 Y
J10023100-2814280AB 2.020.08 1.730.09 0.5590.004 38.90.3 2010.09 Y
J10122171-0128160AB 1.900.02 1.970.01 2.9990.007 291.20.3 2010.09 Y
J10140807-7636327AB 1.450.05 1.760.05 0.2260.002 108.10.5 2010.10 N
J10162867-0520320AB 2.810.55 2.330.32 3.1980.001 195.70.3 2008.02 N
J10364483+1521394AB 1.260.05 1.340.04 1.0420.001 193.40.3 2008.88 N
J10364483+1521394AC 1.320.02 1.340.14 0.8850.001 193.70.3 2008.88 N
J10374401-0548577AB 2.390.04 2.760.13 0.5140.001 359.00.3 2010.11 Y
J10394600+6545213AB 1.570.04 1.630.04 1.1390.002 320.60.3 2008.87 Y
J11091380-3001398AB 0.940.02 1.160.02 0.4360.001 25.00.3 2010.08 N
J11102788-3731520AB 0.410.01 0.370.01 1.5230.001 209.30.3 2010.08 N
J11254754-4410267AB 0.880.05 0.5530.003 259.70.4 2010.08 Y
J11281625+3136017AB 1.130.04 1.340.05 1.1030.002 141.00.3 2008.88 Y
J11315526-3436272AB 5.200.04 6.930.18 1.8970.011 354.60.3 2010.11 N
J12062214-1314559AB 2.190.04 2.460.06 0.4200.003 64.90.3 2010.11 Y
J1206557+700749AB 2.020.05 2.030.03 5.6290.007 60.30.3 2009.42 N
J12134173-1122405AB 1.480.06 1.710.07 1.2960.002 269.10.3 2009.13 Y
J12173945-6409418AB 0.180.01 0.000.05 5.2520.005 238.00.3 2010.11 Y
J12173945-6409418AD 2.500.03 0.1570.002 285.36.9 2010.11 Y
J12173945-6409418BC 1.050.01 1.870.01 0.6130.001 317.90.3 2010.11 Y
J12345629-4538075AB 0.510.03 0.480.02 0.6160.001 313.50.3 2010.08 N
J12351726+1318054AB 0.450.09 0.550.10 0.3320.001 56.80.3 2009.41 N
J12392104-5337579AB 0.060.01 0.080.01 1.4550.001 199.20.3 2010.10 Y
J12545056+4048474AB 1.590.34 1.790.29 0.6090.001 32.70.3 2009.41 Y
J12550001+3118248AB 0.470.01 0.470.01 0.7140.001 350.00.3 2009.41 Y
J13013268+6337496AB 0.900.27 0.1680.006 358.20.8 2009.42 Y
J13015919+4241160AB 1.660.07 1.890.07 2.9080.008 247.90.3 2009.42 Y
J13022691-5200507AB 1.330.06 1.220.06 0.0850.004 104.71.1 2010.08 Y
J13022691-5200507AC 1.660.02 1.740.01 0.8480.008 247.10.3 2010.08 Y
J13025257-5201384AB 0.480.02 0.470.06 0.4780.003 190.20.3 2010.08 Y
J13061131+7025377AB 1.260.01 1.360.01 3.8290.001 102.40.3 2009.42 Y
J13082484+3019094AB 0.880.36 1.000.41 0.2100.003 0.20.6 2009.42 Y
J13120525+3213332AB 0.650.17 0.980.22 0.9010.002 227.00.3 2009.41 Y
J13120689+3213179AB 1.160.29 1.170.11 0.1610.001 285.91.2 2009.42 Y
J13151846-0249516AB 0.770.23 1.200.32 0.2150.002 201.50.3 2009.13 Y
J13195689-6831142AB 1.670.04 1.960.03 0.8780.002 166.90.3 2010.10 Y
J13293209+5142114AB 1.610.02 1.980.05 1.7880.001 303.90.3 2009.42 Y
J13414631+5815197AB 0.790.09 0.900.08 0.5580.001 249.20.3 2009.13 Y
J13493313-6818291AB 1.390.20 1.500.06 0.1090.016 240.74.4 2010.10 Y
J13493313-6818291AC 1.120.01 1.510.01 1.2860.005 289.60.3 2010.10 Y
J13534589+5210298AB 0.300.02 0.150.01 1.0050.002 343.90.4 2008.64 Y
J13584500+3140179AB 0.990.36 1.510.36 0.1220.001 309.72.9 2009.42 Y
J14360274+1334484AB 0.030.03 0.040.01 1.1940.002 48.50.3 2009.42 Y
J14430789+1720463AB 2.960.02 3.330.03 4.7680.002 3.70.3 2009.42 Y
J14433804-0414354AB 0.240.02 0.270.02 0.9650.001 287.70.3 2008.45 Y
J15032251-0040310AB 0.410.02 0.390.02 3.7750.010 274.50.3 2009.13 Y
J15280061+3431226AB 1.020.08 0.960.06 0.4180.002 322.00.3 2009.42 Y
J15290296+4646240AB 0.720.07 0.690.16 0.2680.003 176.30.3 2009.41 Y
J15312428+1900268AB 2.950.07 3.390.10 0.5170.001 283.20.3 2009.42 Y
J15370409+3748275AB 1.620.18 1.840.09 0.2830.001 80.80.4 2009.42 Y
J15553178+3512028AB 2.140.04 2.210.05 1.5940.003 257.50.3 2008.45 N
J15594729+4403595AB 5.510.12 6.330.03 5.6380.004 284.80.3 2009.42 Y
J16232165+6149149AB 0.590.17 0.560.19 0.3820.003 211.90.6 2009.42 Y
J16291031+7804399AB 2.040.04 1.250.02 0.3410.002 6.10.3 2009.42 Y
J16363309+6353452AB 3.370.33 3.700.21 0.1990.008 102.40.4 2009.42 Y
J16363309+6353452AC 1.900.02 2.230.06 3.3620.005 198.30.3 2009.42 N
J16411543+5344110AB 0.970.04 0.730.06 0.0990.005 94.40.3 2009.42 Y
J16510995+3555071AB 1.580.06 1.840.13 1.0350.001 316.40.3 2009.41 Y
J16552880-0820103AB 0.480.11 0.550.10 0.2240.002 81.00.7 2009.42 N
J16590962+2058160AB 1.030.10 1.220.12 0.6890.001 139.00.3 2009.42 Y
J17021204+5103284AB 0.340.04 0.330.01 0.8160.001 63.40.3 2009.42 Y
J17035283+3211456AB 1.760.03 1.930.04 1.2600.001 142.60.3 2009.41 N
J1724591+210838AB 0.030.01 0.040.01 3.3990.004 24.00.3 2008.63 Y
J17250940-0633536AB 0.840.12 1.070.12 0.4370.001 283.50.6 2009.42 Y
J17380077+3329457AB 0.600.03 0.850.05 1.0290.002 157.90.3 2009.41 Y
J18110625+3543573AB 0.410.01 0.610.01 5.2240.008 26.20.3 2009.41 Y
J18162484+5013570AB 0.240.14 0.370.07 0.7010.001 332.70.3 2009.41 Y
J18464053-0916238AB 3.540.27 3.950.42 3.4190.003 266.60.3 2008.45 Y
J18471129+2212413AB 1.090.06 1.120.03 0.3710.001 269.90.4 2009.42 Y
J18592937-0403042AB 0.560.10 0.720.12 0.2970.002 137.50.4 2009.42 Y
J19105480+3017476AB 1.690.05 1.990.13 0.2590.001 122.80.4 2008.63 Y
J19105480+3017476AC 1.200.09 1.420.08 0.7280.001 65.20.3 2008.63 Y
J19213210+4230520AB 1.600.09 1.770.11 0.1260.004 154.40.3 2008.63 Y
J19224005-0612076AB 1.060.18 1.520.36 0.1460.001 79.91.0 2009.42 Y
J19425324-4406278AB 1.390.11 0.8360.002 349.80.3 2008.87 Y
J19432464-3722108AB 2.840.08 2.890.07 1.6230.004 303.70.3 2008.87 Y
J20003177+5921289AB 0.640.24 0.690.21 0.3180.002 267.30.6 2009.41 Y
J20100002-2801410AB 0.800.04 0.750.03 0.6150.001 280.40.3 2008.87 Y
J20163382-0711456AB 0.630.15 0.1070.007 352.42.1 2008.44 Y
J20500010-1154092AB 2.220.21 2.610.30 0.4590.007 350.30.6 2008.63 Y
J20531465-0221218AB 1.160.11 1.380.13 0.0860.002 321.08.0 2008.88 Y
J21035992+1218570AB 0.110.03 0.120.03 0.8360.005 70.00.4 2009.42 Y
J21091375-0814041AB 0.700.01 0.940.06 0.9730.002 120.40.3 2008.88 Y
J21203506+3419476AB 0.990.13 0.890.14 0.1090.002 217.31.3 2008.87 Y
J21205172-0301545AB 0.740.05 0.820.05 1.3050.002 69.70.3 2008.63 Y
J21295166-0220070AB 1.560.25 1.920.36 0.7190.001 60.30.3 2008.59 Y
J21365560-0840313AB 2.570.36 3.440.68 0.2410.008 109.02.8 2008.59 Y
J21372900-0555082AB 0.330.15 0.550.09 0.2220.001 172.20.3 2008.88 Y
J21422932+1233175AB 1.180.14 1.370.16 4.7770.003 8.90.3 2007.84 Y
J22014336-0925139AB 0.280.07 0.380.08 0.9300.002 206.20.3 2008.59 Y
J22232904+3227334AB 0.040.02 0.050.01 1.4670.001 234.90.3 2009.42 N
J22240821+1728466AB 1.000.14 1.160.22 0.1460.007 208.80.8 2009.42 Y
J22332264-0936537AB 0.040.02 0.010.02 1.5470.002 278.50.3 2007.85 N
J22382974-6522423AB 0.230.01 0.200.02 0.8420.001 155.80.3 2008.87 N
J22401867-4931045AB 0.140.01 0.160.01 4.0390.001 41.00.3 2008.87 N
J22495622+1744414AB 1.170.17 1.110.26 0.1170.004 10.00.7 2008.59 Y
J23062378+1236269AB 0.390.09 0.490.01 0.4260.001 316.90.3 2008.59 N
J23172807+1936469AB 1.500.12 1.700.15 0.2930.001 19.20.3 2008.59 N
J23261182+1700082AB 1.570.09 1.900.12 0.1950.002 51.80.7 2008.63 Y
J23261707+2752034AB 0.520.10 0.470.10 0.1510.001 14.10.3 2008.59 Y
J23450477+1458573AB 1.690.05 1.760.05 0.1070.004 177.51.4 2008.59 Y
J23450477+1458573AC 0.000.05 0.050.05 1.2220.002 175.90.3 2008.59 Y
J23495365+2427493AB 1.130.04 1.230.08 0.1310.001 324.61.6 2008.88 Y
J23551649-0235417AB 0.610.16 0.670.08 0.6940.001 120.40.3 2008.63 Y
J23570417-0337559AB 1.710.05 2.060.27 0.1910.001 282.40.4 2008.88 Y
J23581366-1724338AB 0.010.01 0.030.01 1.9890.001 355.70.3 2008.87 N
Table 2: continued.
2MASS ID SpT SpT Sep. Per. Sample
[] [] [AU] [yr]