No description available.

<p> Fragmentation during encounters between protostellar disks provides a possible scenario for the formation of substellar objects such as brown dwarfs and planets. A series of simulations of protostellar disk encounters were performed to investigate the fragmentation under different encounter parameters, and to characterize the properties of any resultant fragments. It was found that the initial disk minimum Toomre Q must satisfy Qini ;S 1.1 for the fragmentation to be induced by the encounters. Fragments of substellar mass can form via disk fragmentation, shock layer fragmentation and tidal tail fragmentation, and the effectiveness of each mechanism is closely related to the initial disk configuration. The fragmentation is also constrained by the relative encounter velocity since the number of fragments decreases quickly with increasing velocity. </p> <p> In comparing to previous studies of protostellar disk encounters it was also found that resolving both the local Jeans Mass during the encounter and the disks' vertical structure are critical to prevent artificial fragmentation and give the correct picture. Heating and cooling rates were estimated in both the optically thin and thick regimes. The comparison between the two indicates that during strong impacts the heating rate increases rapidly but is still comparable to the cooling rate, so the locally isothermal equation of state used in this study is an acceptable approximation. </p> <p> 32 clumps formed in various Qini = 0.9 disk-disk encounters were taken as the sample in an analysis of fragment properties and prospects for their further evolution. The results show that the clump masses are all less than the hydrogen burning mass limit ~ 0.075M0 , so the objects are substellar. Most of the clumps are of brown dwarf mass since the formation of planetary mass clumps is suppressed due to numerical resolution. The mass distribution is broadly consistent to the observed initial mass function in Pleiades. The clumps have highly flattened disk-like shapes and possess large spin angular momentum, which implies that young brown dwarfs may develop disks, jets, or planetary mass companions. About one third of the fragments are unbound to the stars and likely to form free floating brown dwarfs. Orbital analyses of the clumps which are bound to the stars show that there is a lack of close brown dwarf companions ( R < 3 AU), which is consistent to the observed "brown dwarf desert". Many of the orbits are highly eccentric and intersect with other orbits, so ejection of some clumps due to gravitational scattering is likely. Also, dispersion of gas during the encounter and the high spin angular momentum of the clumps may provide mechanisms other than ejection to prevent the clumps from accreting more mass, making the simulated clumps representative of the long term substellar mass function. </p> / Thesis / Master of Science (MSc)

The aim of this thesis is to use a cross-match between WISE, 2MASS and SDSS to identify a large sample of M dwarfs. Through the careful characterisation and quality control of these M dwarfs I aim to identify rare systems (i.e. unresolved UCD companions, young M dwarfs, late M dwarfs and M dwarfs with common proper motion companions). Locating ultracool companions to M dwarfs is important for constraining low-mass formation models, the measurement of substellar dynamical masses and radii, and for testing ultracool evolutionary models. This is done by using an optimised method for identifying M dwarfs which may have unresolved ultracool companions. To do this I construct a catalogue of 440 694 M dwarf candidates, from WISE, 2MASS and SDSS, based on optical- and near-infrared colours and reduced proper motion. With strict reddening, photometric and quality constraints I isolate a sub-sample of 36 898 M dwarfs and search for possible mid-infrared M dwarf + ultracool dwarf candidates by comparing M dwarfs which have similar optical/near-infrared colours (chosen for their sensitivity to effective temperature and metallicity). I present 1 082 M dwarf + ultracool dwarf candidates for follow-up. Using simulated ultracool dwarf companions to M dwarfs, I estimate that the occurrence of unresolved ultracool companions amongst my M dwarf + ultracool dwarf candidates should be at least four times the average for my full M dwarf catalogue. I discuss yields of candidates based on my simulations. The possible contamination and bias from misidentified M dwarfs is then discussed, from chance alignments with other M dwarfs and UCDs, from chance alignments with giant stars, from chance alignments with galaxies, and from blended systems (via visual inspection). I then use optical spectra from LAMOST to spectral type a subset of my M dwarf + ultracool dwarf candidates. These candidates need confirming as true M dwarf + ultracool dwarf systems thus I present a new method I developed to use low resolution near-infrared spectra which relies on two colour similar objects (one an excess candidate, one not) having very similar spectra. A spectral difference of these two colour similar objects should leave the signature of a UCD in the residual of their differences, which I look for using the difference in two spectral bands designed to identify UCD spectral features. I then present the methods used to identify other rare systems from my full M dwarf catalogue. Young M dwarfs were identified by measuring equivalent widths of Hα from the LAMOST spectra, and by measuring rotation periods from Kepler 2 light curves. I identify late M dwarfs photometrically (using reduced proper motion and colour cuts) and spectroscopically (using the LAMOST spectra with spectral indices from the literature). Also I present common proper motion analysis aimed at finding Tycho-2 primaries for my M dwarfs and look for physically separated M dwarf + M dwarf pairs (internally within my full M dwarf catalogue).

A number of substellar companions to evolved cool stars have now been reported. Cool giants are distinct from their progenitor main-sequence low-mass stars in a number of ways. First, the mass loss rates of cool giant stars are orders of magnitude greater than for the late-type main-sequence stars. Secondly, on the cool side of the Linsky–Haisch ‘dividing line’, K and M giant stars are not X-ray sources, although they do show evidence for chromospheres. As a result, cool star winds are largely neutral for those spectral types, suggesting that planetary or brown dwarf magnetospheres will not be effective in standing off the stellar wind. In this case, one expects the formation of a bow shock morphology at the companion, deep inside its magnetosphere. We explore radio emissions from substellar companions to giant stars using (a) the radiometric Bode's law and (b) a model for a bow shock morphology. Stars that are X-ray emitters likely have fully ionized winds, and the radio emission can be at the milli-Jansky level in favourable conditions. Non-coronal giant stars produce only micro-Jansky level emissions when adjusted for low-level ionizations. If the largely neutral flow penetrates the magnetosphere, a bow shock results that can be strong enough to ionize hydrogen. The incoherent cyclotron emission is sub-micro-Jansky. However, the long wavelength radio emission of Solar system objects is dominated by the cyclotron maser instability (CMI) mechanism. Our study leads to the following two observational prospects. First, for coronal giant stars that have ionized winds, application of the radiometic Bode's law indicates that long wavelength emission from substellar companions to giant stars may be detectable or nearly detectable with existing facilities. Secondly, for the non-coronal giant stars that have neutral winds, the resultant bow shock may act as a ‘feeder’ of electrons that is well embedded in the companion's magnetosphere. Incoherent cyclotron emissions are far too faint to be detectable, even with next generation facilities; however, much brighter flux densities may be achievable when CMI is considered.

No description available.

Les naines brunes sont définies comme des objets généralement plus massifs que les planètes géantes, mais qui demeurent moins massifs que les plus petites étoiles. Étant incapables de fusionner de l’hydrogène en hélium comme les étoiles de la séquence principale en raison de leur faible masse, les naines brunes rayonnent seulement leur chaleur initiale de formation et se refroidissent continuellement au fil du temps. Cette perpétuelle diminution en luminosité introduit une dégénérescence entre leurs propriétés physiques, car il devient impossible de distinguer par sa seule luminosité une jeune naine brune massive de celle d’une vielle naine brune moins massive. Une modélisation atmosphérique et évolutive devient donc nécessaire pour contraindre les propriétés physiques (masse, rayon, âge, température effective, métallicité) des naines brunes sans compagnons, où seulement la luminosité peut être mesurée directement. Le flux émergeant de ces modèles semble bien reproduire ceux des naines brunes observées jusqu’à présent. Cependant, les paramètres physiques qu’ils prédisent demeurent sans calibration empirique, car il n’existe pas suffisamment de mesures indépendantes de ces paramètres venant de naines brunes observées qui permettrait de vérifier les prédictions des modèles. L’étude de naines brunes binaires éclipsant une étoile ouvre la possibilité de prendre des mesures directes de ses caractéristiques physiques via des analyses de vitesses radiales, de transits et d’éclipses secondaires, le tout de manière indépendante des modèles. Ce mémoire porte sur l’étude d’une naine brune binaire éclipsante découverte en 2011 via photométrie de transit par le télescope Kepler: LHS 6343 C. Des observations de transit (Kepler) en plus d’observations de vitesses radiales (Keck/HIRES) et d’éclipses secondaires (Kepler, HST, Spitzer) permettent la mesure directe de tous ses paramètres physiques importants sauf l’âge. Ce mémoire apporte une première analyse des données d’éclipse secondaire HST pour obtenir un spectre d’émission de la naine brune dans la bande passante WFC3-G141 (1.1 à 1.7 µm), permettant d’identifier un type spectrale de T1.5. De plus, ce mémoire met à jour la masse et le rayon de LHS 6343 C en utilisant une distance Gaia DR3 et des relations stellaires empiriques. Ce nouvel ensemble de paramètres est ensuite comparé à ceux prédits par des modèles atmosphériques, où l’on trouve que ceux en déséquilibre chimique reproduisent mieux les données comparés à ceux en équilibre chimique. Finalement, des modèles d’évolution sont utilisés pour déterminer l’âge de la naine brune. / Brown dwarfs are defined as substellar objects that are generally more massive than giant planets, but which remain less massive than the smallest stars. Being unable to fuse hydrogen into helium like main-sequence stars due to their low mass, brown dwarfs do not have access to a long-term energy source. They therefore radiate only their initial heat of formation and cool continuously over time. This perpetual decrease in luminosity introduces a degeneracy between their physical properties, making it impossible to distinguish a young massive brown dwarf from an older less massive one based on their luminosity and spectra alone. Therefore, atmospheric and evolutionary modelling becomes necessary to obtain other properties (e.g. mass, radius, age, effective temperature) of field brown dwarfs, since only their luminosity can be measured directly. Fortunately, the luminosities and spectra of the best models reproduce observations well. However, the physical parameters they predict (i.e. mass, radius, effective temperature, metallicity) lack an empirical calibration; i.e. there are not enough independent measurements of these parameters to meaningfully confirm the predictive power of models. One of the scenarios allowing the direct measurement of several physical characteristics is provided by brown dwarf eclipsing binaries (BDEB), i.e. a brown dwarf orbiting a star. With radial velocity, transit, and secondary eclipse analyses, all but the age of a BDEB can be determined independently of models. This thesis pertains to the study of a minimally irradiated BDEB, LHS 6343 C, discovered in 2011 via transit photometry by the Kepler telescope. Since its discovery, a greater amount of transit (Kepler) observations in addition to radial velocity (Keck/HIRES) and secondary eclipse (Kepler, HST, Spitzer) observations allow for everything but an age measurement to be obtained. This thesis provides a first analysis of the HST secondary eclipse data to obtain a brown dwarf emission spectrum in the WFC3-G141 filter (1.1 to 1.7 µm), identifying it as a T1.5 dwarf. In addition, this thesis updates the physical parameters of previous studies using a Gaia DR3 distance and empirical stellar relations. This new set of parameters is then compared to those predicted by atmospheric models, where those in chemical nonequilibrium reproduce the observed flux better than chemical equilibrium or cloud models. Finally, evolutionary models are used to determine the age of the brown dwarf.