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According to the current cosmological paradigm, ``Lambda Cold Dark Matter'' (LambdaCDM), only ~20% of the gravitating matter in the universe is made up of ordinary (i.e. baryonic) matter, while the rest consists of invisible dark matter (DM) particles, which existence can be inferred from their gravitational influence on baryonic matter and light. Despite the large success of the LambdaCDM model in explaining the large scale structure of the Universe and the conditions of the early Universe, there has been debate on whether this model can fully explain the observations of low mass (dwarf) galaxies. The Local Group (LG), which hosts most of the known dwarf galaxies, is a unique laboratory to test the predictions of the LambdaCDM model on small scales. I analyze the kinematics of LG members, including the Milky~Way-Andromeda (MW-M31) pair and dwarf galaxies, in order to constrain the mass of the LG. I construct samples of LG analogs from large cosmological N-body simulations, according to the following kinematics constraints: (a) the separation and relative velocity of the MW-M31 pair; (b) the receding velocity of dwarf galaxies in the outskirts of the LG. I find that these constraints yield a median total mass of 2*10^{12} solar masses for the MW and M31, but with a large uncertainty. Based on the mass and the kinematics constraints, I select twelve LG candidates for the APOSTLE simulations project. The APOSTLE project consists of high-resolution cosmological hydrodynamical simulations of the LG candidates, using the EAGLE galaxy formation model. I show that dwarf satellites of MW and M31 analogs in APOSTLE are in good agreement with observations, in terms of number, luminosity and kinematics. There have been tensions between the observed masses of LG dwarf spheroidals and the predictions of N-body simulations within the LambdaCDM framework; simulations tend to over-predict the mass of dwarfs. This problem is known as the ``too-big-to-fail'' problem. I find that the enclosed mass within the half-light radii of Galactic classical dwarf spheroidals, is in excellent agreement with the simulated satellites in APOSTLE, and that there is no too-big-to-fail problem in APOSTLE simulations. A few factors contribute in solving the problem: (a) the mass of haloes in hydrodynamical simulations are lower compared to their N-body counterparts; (b) stellar mass-halo mass relation in APOSTLE is different than the ones used to argue for the too-big-to-fail problem; (c) number of massive satellites correlates with the virial mass of the host, i.e. MW analogs with virial masses above ~ 3*10^{12} solar masses would have faced too-big-to-fail problems; (d) uncertainties in observations were underestimated in previous works. Stellar mass-halo mass relation in APOSTLE predicts that all isolated dwarf galaxies should live in haloes with maximum circular velocity (V_max) above 20 km/s. Satellite galaxies, however, can inhabit lower mass haloes due to tidal stripping which removes mass from the inner regions of satellites as they orbit their hosts. I examine all satellites of the MW and M31, and find that many of them live in haloes less massive than V_max=20 km/s. I additionally show that the low mass population is following a different trend in stellar mass-size relation compared to the rest of the satellites or field dwarfs. I use stellar mass-halo mass relation of APOSTLE field galaxies, along with tidal stripping trajectories derived in Penarrubia et al., in order to predict the properties of the progenitors of the LG satellites. According to this prediction, some satellites have lost a significant amount of dark matter as well as stellar mass. Cra~II, And~XIX, XXI, and XXV have lost 99 per-cent of their stellar mass in the past. I show that the mass discrepancy-acceleration relation of dwarf galaxies in the LG is at odds with MOdified Newtonian Dynamics (MOND) predictions, whereas tidal stripping can explain the observations very well. I compare observed velocity dispersion of LG satellites with the predicted values by MOND. The observations and MOND predictions are inconsistent, in particular in the regime of ultra faint dwarf galaxies. / Graduate

The Milky Way (MW) and M31 both harbour massive satellite galaxies, the Large Magellanic Cloud (LMC) and M33, which may comprise up to 10 per cent of their host's total mass. Massive satellites can change the orbital barycentre of the host-satellite system by tens of kiloparsec and are cosmologically expected to harbour dwarf satellite galaxies of their own. Assessing the impact of these effects crucially depends on the orbital histories of the LMC and M33. Here, we revisit the dynamics of theMW-LMC system and present the first detailed analysis of the M31-M33 system utilizing high-precision proper motions and statistics from the dark-matter-only Illustris cosmological simulation. With the latest Hubble Space Telescope proper motion measurements of M31, we reliably constrain M33' s interaction history with its host. In particular, like the LMC, M33 is either on its first passage (t(inf) < 2 Gyr ago) or if M31 is massive (>= 2 x 10(12) M-circle dot), it is on a long-period orbit of about 6 Gyr. Cosmological analogues of the LMC and M33 identified in Illustris support this picture and provide further insight about their host masses. We conclude that, cosmologically, massive satellites such as the LMC and M33 are likely completing their first orbits about their hosts. We also find that the orbital energies of such analogues prefer an MW halo mass similar to 1.5 x 10(12) M-circle dot and an M31 halo mass >= 1.5 x 10(12)M(circle dot). Despite conventional wisdom, we conclude it is highly improbable that M33 made a close (< 100 kpc) approach to M31 recently (t(peri) < 3 Gyr ago). Such orbits are rare (< 1 per cent) within the 4s error space allowed by observations. This conclusion cannot be explained by perturbative effects through four-body encounters amongst the MW, M31, M33, and the LMC. This surprising result implies that we must search for a new explanation for M33' s strongly warped gas and stellar discs.

In the era of high-precision astrometry, space observatories like the Hubble Space Telescope (HST) and Gaia are providing unprecedented 6D phase-space information of satellite galaxies. Such measurements can shed light on the structure and assembly history of the Local Group, but improved statistical methods are needed to use them efficiently. Here we illustrate such a method using analogues of the Local Group's two most massive satellite galaxies, the Large Magellanic Cloud (LMC) and Triangulum (M33), from the Illustris dark-matter-only cosmological simulation. We use a Bayesian inference scheme combining measurements of positions, velocities and specific orbital angular momenta (j) of the LMC/M33 with importance sampling of their simulated analogues to compute posterior estimates of the Milky Way (MW) and Andromeda's (M31) halo masses. We conclude that the resulting host halo mass is more susceptible to bias when using measurements of the current position and velocity of satellites, especially when satellites are at short-lived phases of their orbits (i.e. at pericentre). Instead, the j value of a satellite is well conserved over time and provides a more reliable constraint on host mass. The inferred virial mass of the MW(M31) using j of the LMC (M33) is M-vir,M- MW = 1.02(-0.55)(+0.77) x 10(12) M-circle dot (M-vir,M- M31 = 1.37(-0.75)(+1.39) x 10(12) M-circle dot). Choosing simulated analogues whose j values are consistent with the conventional picture of a previous (<3 Gyr ago), close encounter (<100 kpc) of M33 about M31 results in a very low virial mass for M31 (similar to 10(12) M-circle dot). This supports the new scenario put forth in Patel, Besla & Sohn, wherein M33 is on its first passage about M31 or on a long-period orbit. We conclude that this Bayesian inference scheme, utilizing satellite j, is a promising method to reduce the current factor of 2 spread in the mass range of the MW and M31. This method is easily adaptable to include additional satellites as new 6D phase-space information becomes available from HST, Gaia and the James Webb Space Telescope.

Thesis (Ph. D.)--University of Washington, 2002. / Vita. Includes bibliographical references (p. 301-311).

Although exotic objects like supermassive black holes (SMBHs) and dark matter halos do not emit or interact with light, we can still detect them across the vastness of space. By observing the gravitational dance of objects we can see, astronomers are able to infer the mass of the invisible objects they orbit. This has led to the discovery that nearly every massive galaxy hosts a SMBH at its center, and has confirmed that every galaxy is embedded in an extended halo of dark matter. However, the practice of inferring mass from the motions of bright kinematics tracers has many complications, not the least of which is that we seldom observe more than the line-of-sight component of the instantaneous velocity of a star. Consequently, astronomers must build dynamical models of the galaxies they wish to study. These models often rely on overly restrictive assumptions, or are crippled by degeneracies amongst their parameters and lack predictive power. In this thesis, I introduce a significant advancement into the field of dynamical modeling. My modeling technique is based on the powerful principle of orbit superposition, also known as Schwarzschild Modeling. This technique is robust to many of the degeneracies associated with dynamical modeling, and has enjoyed much success in measuring the SMBHs and dark matter halos of large elliptical or bulge-dominated galaxies. I use it in Chapter 2 to accurately measure the SMBH in the Sombrero Galaxy (NGC 4594) and to constrain its dark matter halo. Unfortunately, when measuring dark matter halos with Schwarzschild Modeling, the modeler is required to adopt a parameterization for the dark matter density profile. Often this is precisely the quantity one wishes to measure. To avoid this reliance on a priori parameterizations, I introduce a technique that calculates the profile non-parametrically. Armed with this powerful new technique, I set out to measure the distribution of dark matter in the halos of some of the smallest galaxies in the Universe. These dwarf spheroidal galaxies (dSphs) orbit the Milky Way as satellites, and their dark matter content has been studied extensively. However, the models used to probe their halos have been simplistic and required overly restrictive assumptions. As a result, robust conclusions about their dark matter content have remained elusive. Into this controversial and active area of study, I bring Non-Parametric Schwarzschild Modeling. The results I find offer the most robust and detailed measurements of the dark matter profiles in the dSphs to date. I begin my study with the first application of standard Schwarzschild Modeling to any dSph galaxy by using it in Chapter 3 on Fornax. This chapter details the process of re-tooling Schwarzschild Modeling for the purpose of measuring these small galaxies. In Chapter 4, I introduce the fully non-parametric technique, and apply it to Draco as proof of concept. Chapter 5 presents the main results of this thesis. Here I apply Non-Parametric Schwarzschild Modeling to Draco, Carina, Fornax, Sculptor, and Sextans. By relaxing the assumption of a parameterization for the dark matter profile, I find a variety of profile types in these five galaxies---some of which are consistent with past observations, others consistent with predictions from simulations, and still others were completely unanticipated. Finally, in Chapter 6 I describe the modeling of these galaxies in more detail. I demonstrate the accuracy of Non-Parametric Schwarzschild Modeling by recovering a known dark matter profile from artificial simulated data. I also expound upon the modeling results by presenting the detailed orbit structure of the five dSphs. Lastly, I compare my results to hydrodynamical simulations to explore the link between dark matter profile type and the baryon content of the dSphs. / text

We present the discovery of a very faint stellar system, SMASH 1, that is potentially a satellite of the Large Magellanic Cloud. Found within the Survey of the MAgellanic Stellar History (SMASH), SMASH 1 is a compact (r(h) 9.1(-3.4)(+5.9)pc) and very low luminosity (M-V = -1.0 +/- 0.9, L-V = 10(2.3 +/- 0.4) L-circle dot) stellar system that is revealed by its sparsely populated main sequence and a handful of red giant branch candidate member stars. The photometric properties of these stars are compatible with a metal-poor ([Fe/H] = -2.2) and old (13 Gyr) isochrone located at a distance modulus of similar to 18.8, i.e., a distance of similar to 57 kpc. Situated at 11 degrees.3 from the LMC in projection, its three-dimensional distance from the Cloud is similar to 13 kpc, consistent with a connection to the LMC, whose tidal radius is at least 16 kpc. Although the nature of SMASH 1 remains uncertain, its compactness favors it being a stellar cluster and hence dark-matter free. If this is the case, its dynamical tidal radius is only less than or similar to 19 pc at this distance from the LMC, and smaller than the system's extent on the sky. Its low luminosity and apparent high ellipticity (epsilon = 0.62(-0.21)(+0.17)) with its major axis pointing toward the LMC may well be the tell-tale sign of its imminent tidal demise.

We present a chemodynamical analysis of the Leo V dwarf galaxy, based on the Keck II DEIMOS spectra of eight member stars. We find a systemic velocity for the system of nu(r) = 170.9(+2.1) (-1.9) km s(-1) and barely resolve a velocity dispersion for the system, with sigma nu(r) = 2.3(+3.2) (-1.6) km s(-1), consistent with previous studies of Leo V. The poorly resolved dispersion means we are unable to adequately constrain the dark-matter content of Leo V. We find an average metallicity for the dwarf of [ Fe/ H] =-2.48 +/- 0.21 and measure a significant spread in the iron abundance of its member stars, with -3.1 <= [ Fe/ H] <=-1.9 dex, which clearly identifies Leo V as a dwarf galaxy that has been able to self-enrich its stellar population through extended star formation. Owing to the tentative photometric evidence for the tidal substructure around Leo V, we also investigate whether there is any evidence for tidal stripping or shocking of the system within its dynamics. We measure a significant velocity gradient across the system, of dv d chi = -4.1(+2.8) (-2.6) km s(-1) arcmin(-1) ( or d nu/d chi=-71.9(vertical bar 50.8) (-45.6) km s(-1) kpc(-1)), which points almost directly towards the Galactic Centre. We argue that Leo V is likely a dwarf on the brink of dissolution, having just barely survived a past encounter with the centre of the Milky Way.

We present results from MMT/Hectochelle spectroscopy of 390 red giant candidate stars along the line of sight to the recently discovered Galactic satellite Crater 2. Modeling the joint distribution of stellar positions, velocities, and metallicities as a mixture of Crater 2 and Galactic foreground populations, we identify similar to 62 members of Crater 2, for which we resolve a line-of-sight velocity dispersion of sigma(nu los) = 2.7(-0.3)(+0.3) km s(-1) and a. mean velocity of <nu(los)> = 87.5(-0.4)(+0.4) km s(-1) (solar rest frame). We also resolve a metallicity dispersion of sigma([Fe/H]) = 0.22(-0.03)(+0.04) dex and a mean of <[Fe/H]> = 1.98(-0.1)(+0.1) dex that is 0.28 +/- 0.14 dex poorer than estimated from photometry. Despite Crater 2's relatively large size (projected halflight radius R-h similar to 1 kpc) and intermediate luminosity (M-V similar to -8), its velocity dispersion is the coldest that has been resolved for any dwarf galaxy. These properties make Crater 2 the most extreme low-density outlier in dynamical as well as structural scaling relations among the Milky Way's dwarf spheroidals. Even so, under assumptions of dynamical equilibrium and negligible contamination by unresolved binary stars, the observed velocity distribution implies a gravitationally dominant dark matter halo, with a dynamical mass of. 4.4(-0.9)(+1.2) x 10(6) M-circle dot and a mass-to-light ratio of 53(-11)(+15) M-circle dot/L-V,L-circle dot enclosed within a radius of similar to 1 kpc, where the equivalent circular velocity is 4.3(-0.5)(+0.5) km s(-1).

Uma previsão fundamental do cenário L cold dark matter (LCDM) na formação de estruturas é que os halos galácticos de DM do tamanho da Via Láctea (MW) crescem pela acreção de subsistemas menores. Neste contexto, simulações deNcorpos prevêem um número de sub-halos de matéria escura, cujo tamanho e massa são comparáveis às galáxias anãs, que é muito maior do que as galáxias satélites conhecidas. Este é o que se convencionu chamar de problema das satélites faltantes (MSP). A interpretação mais popular do MSP é que os sub-halos de matéria escura menores são extremamente ineficientes na formação de estrelas, o que torna mais difícil detectá-los. Com a chegada dos grandes levantamentos fotométricos, nos últimos anos, a descoberta de uma nova população de galáxias satélites que orbitam a MW fornece evidências empíricas para acreditar que realmente existem várias galáxias pouco luminosas não detectadas ou que simplesmente habitam regiões no céu que ainda não foram observadas. Neste trabalho implementamos um algoritmo estatístico eficiente para detectar subestruturas ultra fracas da MW. O código, chamado SPARSEX, foi testado e otimizado usando um conjunto de objetos estelares previamente identificados nos dados do Sloan Digital Sky Survey (SDSS), conseguindo recuperar todos os objetos com sucesso. Além disso, a aplicação do algoritmo aos dados dos dois primeiro anos do Dark Energy Survey (DES) deu como resultado centenas de candidatos a sistemas estelares. Dezessete sistemas estelares detectados em comum com outras técnicas de busca por subestruturas, implementadas dentro do grupo de colaboração do DES, foram publicados em três artigos em 2015. Um dos candidatos publicados é o aglomerado estelar DES 1. DES1 foi detectado pelo código SPARSEX com uma alta significância estatística e aparece nas imagens do DES como uma concentração compacta de fontes pontuais azuis. O sistema estelar é consistente com uma população velha e pobre em metal. Assumindo dois diferentes perfis de densidade, os quais permitem estimar a probabilidade de que cada estrela realmente pertença ao sistema, determinamos uma distância heliocêntrica e uma magnitude absoluta total num intervalo de 77.6—87.1 kpc e 3.00 . MV . 2.21, respectivamente. O raio à meia-luz desse objeto, rh 9.88 pc, e a luminosidade são consistentes com um aglomerado estelar de baixa luminosidade do halo externo. DES1 também é x alongado (e 0.6), o que faz supor que este objeto está em estágio avançado de dissolução. Mais tarde, através de uma cuidadosa reanálise de nossos resultados, dois novos candidatos foram detectados, DES J01111341 e DES J0225+0304. Os candidatos estão localizados a uma distância heliocêntrica de 25 kpc e parecem também estar dominados por populações estelares velhas e pobres em metais. Suas distâncias ao plano orbital da galáxia anã de Sagitário, 1.73 kpc (DES J01111341) e 0.50 kpc (DES J0225+0304), indicam que eles estão possivelmente associados com a corrente da anã de Sagitário. O raio à meia-luz (rh ' 4.55 pc) e a luminosidade (MV ' +0.3) de DES J01111341 são consistentes com um aglomerado estelar ultra fraco, enquanto o raio à meia-luz (rh ' 18.55 pc) e a luminosidade (MV ' 1.1) de DES J0225+0304 colocam este objeto em uma região ambígua do plano tamanho-luminosidade entre aglomerados estelares e galáxias anãs. Determinações dos parâmetros característicos da corrente de Sagitário, tais como o espalhamento de metalicidade (2.18 . [Fe/H] . 0.95) e o gradiente de distância (23 kpc . D . 29 kpc), dentro da área amostrada do DES no hemisfério sul, também indicam uma possível associação com estes sistemas. Se esses objetos forem confirmados através de follow-up espectroscópico como sistemas ligados gravitacionalmente e compartilharem uma trajetoria Galáctica com a corrente de Sagitário, DES J01111341 e DES J0225+0304 seriam os primeiros sistemas estelares ultra fracos associados com tal corrente. Recentemente, nós reportamos a descoberta de um novo aglomerado estelar, DES 3. O novo sistema foi detectado como uma sobredensidade estelar nos dados do primeiro ano do DES e confirmado com follow-up fotométrico obtido com o Southerm Astrophysical Research (SOAR) Telecope. Nós determinamos que DES 3 está localizado a uma distância heliocêntrica de 76 kpc e é dominado por uma população velha (' 9.8Ganos) e pobre em metal ([Fe/H] ' 1.88). Embora os valores de idade e metalicidade de DES 3 são semelhantes aos aglomerados globulares, o seu raio à meia-luz (rh 6.5 pc) e a luminosidade (MV 1.9) são mais indicativos de um aglomerados estelar fraco. Com base no tamanho angular aparente, o DES 3, com um valor de rh 0.03, está entre os menores aglomerados estelares fracos conhecidos até à data. Estas novas detecções indicam que o censo de satélites da MW é ainda incompleto. A identificação e estudo de novos satélites em futuros surveys, como por exemplo o Large Synoptic Survey Telescope (LSST) será crucial para a nossa compreensão das subestruturas existentes no halo Galáctico e a evolução da Galáxia como um todo. / A fundamental prediction of the L cold dark matter (LCDM) scenario of structure formation is that galactic DM haloes of the size of the Milky Way (MW) grow by the accretion of smaller sub-systems. In this context, Nbody simulations predict a number of dark matter subhalos, with size and mass comparable to dwarf galaxies, but which is much larger than currently known satellite galaxies. This is what is conventionally called the missing satellites problem (MSP). The most popular interpretation of the MSP is that the smaller dark matter subhalos are extremely inefficient in star formation, making it more difficult to detect them. With the arrival of large photometric surveys, in recent years, the discovery of a new population of satellite galaxies orbiting the MW provides empirical evidence to believe that there are actually several low luminosity galaxies that were not yet detected or that simply inhabit regions in the sky that have not yet been observed. In this work we present an efficient statistical algorithm to detect ultra-faint MW substructures. The code, called SPARSEX, was tested and optimized using a set of stellar objects previously identified in the Sloan Digital Sky Survey (SDSS) data. It has detected successfully all known objects. In addition, the algorithm was applied on the first two years of Dark Energy Survey (DES) data, resulting in hundreds of stellar system candidates. Seventeen stellar systems detected in common with other substructure search techniques implemented within the DES collaboration were published in three papers in 2015. In particular, one published candidate is a star cluster, DES 1. DES 1 was detected by the SPARSEX code with high statistical significance and appears in DES images as a compact concentration of blue point sources. The stellar system is consistent with being dominated by an old and metal-poor population. Assuming two different density profiles, based on which we may evaluate a membership probability for each star, we determined a heliocentric distance and total absolute magnitude in the ranges of 77.6—87.1 kpc and 3.00 . MV . 2.21, respectively. The half-light radius of this object, rh 9.88 pc, and luminosity are consistent with a low-mass halo star cluster. DES1 is also elongated (e 0.6), which suggests that this object is in advanced stage of dissolution. Later, through a careful reanalysis of our results, two new candidates were detected, DES J01111341 e DES J0225+0304. The candidates are located at a heliocentric xii distance of 25 kpc and appear to have old and metal-poor populations as well. Their distances to the Sagittarius dwarf orbital plane, 1.73 kpc (DES J01111341) and 0.50 kpc (DES J0225+0304), indicate that they are possibly associated with the Sagittarius dwarf stream. The half-light radius (rh ' 4.55 pc) and luminosity (MV ' +0.3) of DES J01111341 are consistent with it being an ultra-faint star cluster, while the half-light radius (rh ' 18.55 pc) and luminosity (MV ' 1.1) of DES J0225+0304 place it in an ambiguous region of size-luminosity space between star clusters and dwarf galaxies. Determinations of the characteristic parameters of the Sagittarius stream, such as its metallicity spread (2.18 . [Fe/H] . 0.95) and distance gradient (23 kpc . D . 29 kpc), within the DES footprint in the Southern hemisphere, also indicate a possible association with these systems. If theses objects are confirmed through spectroscopic follow-up to be gravitationally bound systems and to share a Galactic trajectory with the Sagittarius stream, DES J01111341 and DES J0225+0304 would be the first ultra-faint stellar systems associated with the Sagittarius stream. Recently, we reported the discovery of a new star cluster, DES 3. The new system was detected as a stellar overdensity in first-year DES data, and confirmed with deeper photometry from the Southern Astrophysical Research (SOAR) telescope. We determine that DES 3 is located at a heliocentric distance of 76 kpc and it is dominated by an old (' 9.8 Gyr) and metal-poor ([Fe/H] ' 1.88) population. While the age and metallicity values of DES 3 are similar to globular clusters, its half-light radius (rh 6.5 pc) and luminosity (MV 1.9) are more indicative of faint star clusters. Based on the apparent angular size, DES 3, with a value of rh 0.03, is among the smallest faint star clusters known to date. These new detections indicate that the MW satellites census is still incomplete. The identification and study of new satellites in future surveys, such as the Large Synoptic Survey Telescope (LSST), will be crucial to our understanding of substructures in the Galactic halo and the evolution of the Galaxy as a whole.