Stellar Evolution in the Galactic Bulge J.A

Total Page:16

File Type:pdf, Size:1020Kb

Stellar Evolution in the Galactic Bulge J.A on the UK Schmidt telescope. FLAIR4 is a fibre-fed spectrograph which will be able to obtaln spectra of up to 100 ob- jects per exposure down to B = 18.5 and agreement has been reached to rlde piggy-back on another programme working at the SGP. The remaining 235 candidates in this magnitude range In the ottler selected fields would need to be observed with the 2,2-m, 3.6-m or Nl-r, In addition, experience from the EMSS follow-up has shown that often more than one stellar object with a reasonable favratio is associated wlth one X-ray source. The secondary crite- rion for stellar X-ray idmtlfication Is the presence of chromospheric emksion rn llnes or rotatlonally broadened absorp- tion lines In the spectrum of the star. This wlll require higher-resolution spec- trampy particularly for RS CVn and W UMa blneries and solar-type stars wlth moderate levels of chromospheric activity. Therefore, towards the end of the survey this type of spectroscopic work will be necessary far an estlrnated 250 stars. I All members of our team feel that it is important to allow time for follow-up obsewations of Important, exciting, in- "gUr8 3- teresting or new objects as soon as specifically to meet the requirements of allow team members to profit better possible. We have therefore requested idenmcation, an extra allocation be from the somewhat arduous tasks d that, contiguous with the time allotted made to allow for follow-up. This will survey identification. PROFILE OF A KEY PROGRAMME Stellar Evolution in the Galactic Bulge J.A. BLOMMAERJ, A.G. BROWN, U.J. HABING, J. LUB, Y.K. NG,R.S. LE POOLE, P. T. DE ZEEU W, Sterre wacht Leiden, the Netherlands G. BERTEL LI, A. BRESSAN, C. CHIOSI, Osservatorio As tronomico, Padova, Italy W.E.C. J. VAN DER VEEN, Columbia University, New York, USA H. E. SCH WARZ, ESQ M. W. FHST, South African Astronomical Obsewatory, Cape Town, South Africa targe-scale maps at infrared wave- Some parts of the Galactic Bulge out- Plaut's painstaking work by measuring lengths obtained with IRAS and COBE side the galactic plane can be studled B and R Schmidt plates with an automa- show our Milky Way as an edge-on spi- optically, In particular, there is a 65 by tic measuring machine, and using a ral galaxy, and clearly reveal the Galac- 6:5 field (900 pc by 900 pc) of low and photo-electric callbration sequence. He tic Bulge. This separate component of homogeneous extlnctkn, centred at obtained more accurate magnitudes, our Galaxy can be considered as the I = O0, b = -1V, which in the rnid-fif- and confirmed Plaut's list of variable nearest ellipsoidal stellar system. ties was chosen by Baade and Plaut as stars. As a result, nearly all Miras, Long- Studies of its stellar content are crucial a good field to search for variable stars Period Variables, Semi-Regular Vari- not only for our understanding of stellar by photographic techniques (cf. Blaauw, ables, and also the RR Lyrae stars have evolution and stellar populations in gen- 1955). It is often referred to as the now been identified. Accurate perlods erat, but also for calibrating the rnea- Palomar-Groningen Field Nr. 3, or sim- and light curves have been determined surernents of the cotours and line ply as the Baade-Plaut field. Its location for all stars with periods less than 300 strengths of the integrated light of ellipti- IS illustrated in Figure 1. Recently, days. We are extending Wesselink's cal galaxies (Whitford, 1986). Wesselink (1987) has repeated part of work, with the aim of constructing a 7Re Bulge of our Galaxy (ESO phtqm@h8 1986, Mwm€~er,4@14-75), The phofogreph camappmxlmtely 80 by 45 degree~f.The Baade-Plaut neld Is indicated by the ccashed square. T-p's dew CCD phohmtiy fieids are denow by astahk fhe dpen drcleg am BQmand TBmdn@s (1-1 sumy Wds W late-type glmts. The didreetanQle indIcete~the central W studied h the IR by Catchpole et a/. (1NO). 14aa&'s Windows: NGC 65ZP,Sgr I end Sgr 11. Hertzsprung-Russdl diagram for a sam- the evolution of these late-type stars. Do the ESO Schmidt telescope - centred ple of mow than one million stars In the Miras evolve Into IR stars by an incraas- around the prominent Ha or [0111] emis- Saade-Plaut field. This Is done by Ing mass loss or do these two groups sbn lines - with available continuum UK means of automated photographic pho- repremt late-lype stars wlth different Schmidt R plates. tometry (in U, B, R, I) which yields mag- masses and therefore differed We expect to obtain many objects in nitudes and colours to an accuracy of lumlnosltles? It has always been dlfflcult all phases of the AGB evolution, so that 0.03 mag. Because the number of stars to distinguish between these two a comparison of the relative numbers is so large, we expect that even "fast" scenarios as dlstanms and therefore will yield the duration of each phase, evolutionary phases will be well rep- lumjnmities generally are uncertain. including the fast ones. The results will resented. The Baade-Plaut fleld is Weal for a be analysed using state-of-the-art &I- The evolution of low and Intermediate study of the late and luminous stages of lar ewrlutlonary tracks. This should allow mass stars (1-8 MQ) ultimately leads to stellar evolution in the Galactic Bulge. a precise delineation of the link between the Asymptotic Giant Branch phase Ail the objects are at abwt the same Mlras, Long-Period Variables, Smi- (AGB), which is followed by the forma- distance, and many of the AGB stars Regular Variables and OWTR stars, and tion of a planetary nebula. Miand have been found already through a derivation of an accurate period- OH/IR stars are situated at the top of the Wessellnk's work. In ddltion, we have a luminosity relation. The direct relation AGB. Thy are very luminous, long sample of candidate IR stars selected between mass-losing giant stars and perlodlc, mass-losing variables: M tras from the lRAS Point Source Catalogue planetary nebulae can be established have periods up to 500 days, while IR by means of the F25F 12 dux ratio crite- independent of distance-scale related stars have even larger periods. During rion (cf. Whitdock et al., 1986). We are problems. this phase the stars enshroud thm- carrying out near-infrared photometry We are taklng optlcal spectra of many selves In a clrcumstellar gaddust shell. on these objects to Investigate the na- of the Mira's, from which we hope to General scenarios for AGB evolution are ture of the IRA$ sources, and to deter- derive their metallicities, so that we can available (e.g., van der Veen 1989), but mine the bolomebic luminosities of the address the luminosity/metal abun- much more quantitative work has to be AGB stars (cf. Whitetock et al,, 1990). dance differentiation. The spectra wlll done and several details have to be When repeated wMciently often, such also provide radial vejocitles, thus shed- cleared up. In particular, at present it is measurements will also give the pulsa- dlng Ilght on the dynamics of the Bulge. Unclear whether or not there Is Increas- tlonal period of the star. Finally, we will The mix of stellar objects as a function ing mass loss on the upper AGE, and 1f also search for planetmy nebulae by of galactic latitude (or mMlicity) can be there is, what consequences this has for comparing narrow band exposures with determined, In particular when our study of the Baade-Plaut field is combined vide information on the history of the Temdrup, D.M., 1988. Astron. J., 98,884. with similar studies of other Bulge fields, Bulge. van der Vm, W.E.C.J., 1989. Astron. As- such as Baade's window (Terndmp, troph., 210, 1&. 1988; Rlch, 1989). and the central region References Wesseflnk, T., 1887. A ~~tr(cShrdy of (Catchpole et at., 1990). This is impor- Blaaw, A,, 1955. 1AU Sympodurn No. 1, Variable stars in a field nwthe Gelactk CenW, PhD the&, Unlvemity of Nljmegen. tant also for the understanding of the Coordination of Galactic Rasearch (Cam- Mdge University Press). Whltelock, PA, Feast, M. and Catchpole, stellar composition of the bulges of R.M., 1986. MmNdt. R. Astt. See., m,1. other galaxies. Bl-, V.M., and Terndrup, D.M., 1989. As- tmJ., 08, 843. Whitelock, PA, Feast, M., and Catchpole, In summary,this Key Project aims at Catchpole, R.M., Whitel&, PA, Glass, 1.S.. R.M., 1490. Mon. htR, Ask SQC., In Improvlng our understanding of stellar 1-0. Mon. Not. R. Astr. Soe., In preas. PW. evolution on the AGE by a compre- Rich, R,M., 1989. In IAU Symposium No. 136. Whltfwd, A.E., 1986. Ann Rev. Astron. AS- hensive study of the Baade-Plaut field The Center of the Galaxy, ed. M. Mms troph., 24, 19. in the Galactic Bulge. Thisa will pro- (Dordrmht: Kluwar), p. 63. PROFILE OF A KEY PROGRAMME Kinematics of the Local Universe G. PA TUREL ', L. BOTTINELLI~,P. FOUQU~', R. GARNIERI, L. GOUGUENHEIM~, P. TEERIKORPl3 'Observatoire de Lyon, Saint-Genis Laval, France 'ERA D, Observatoire de Paris-Meudon, Meudon, France 3Turku University Observatory, Tuorla, Finland Introduction of our necessarily subjective point of examples: the location, first discovered view and the subtle biases which affect by H, Shapley (1) from the asymmetry of How matter is organized in the Uni- this description. Historical evidence the dlstributlon of globular clusters, was verse is a fascinating problem to solve shows that understanding the determi- accepted only when dynamical argu- because it imposes severe constraints nation of the velocity field is of funda- ments were glven by J.H.
Recommended publications
  • The Intrinsic Shape of Galaxy Bulges 3
    The intrinsic shape of galaxy bulges J. M´endez-Abreu Abstract The knowledge of the intrinsic three-dimensional (3D) structure of galaxy components provides crucial information about the physical processes driving their formationand evolution.In this paper I discuss the main developments and results in the quest to better understand the 3D shape of galaxy bulges. I start by establishing the basic geometrical description of the problem. Our understanding of the intrinsic shape of elliptical galaxies and galaxy discs is then presented in a historical context, in order to place the role that the 3D structure of bulges play in the broader picture of galaxy evolution. Our current view on the 3D shape of the Milky Way bulge and future prospects in the field are also depicted. 1 Introduction and overview Galaxies are three-dimensional (3D) structures moving under the dictates of gravity in a 3D Universe. From our position on the Earth, astronomers have only the op- portunity to observe their properties projected onto a two-dimensional (2D) plane, usually called the plane of the sky. Since we can neither circumnavigate galaxies nor wait until they spin around, our knowledge of the intrinsic shape of galaxies is still limited, relying on sensible, but sometimes not accurate, physical and geometrical hypotheses. Despite the obvious difficulties inherent to measure the intrinsic 3D shape of galaxies, it is doubtless that it keeps an invaluable piece of information about their formation and evolution. In fact, astronomers have acknowledged this since galaxies arXiv:1502.00265v2 [astro-ph.GA] 31 Aug 2015 were established to be island universes and the topic has produced an outstanding amount of literature during the last century.
    [Show full text]
  • Dark Matter and Background Light
    Dark Matter and Background Light J.M. Overduin Gravity Probe B, Hansen Experimental Physics Laboratory, Stanford University, Stanford, California, U.S.A. 94305-4085 and P.S. Wesson Department of Physics, University of Waterloo, Ontario, Canada N2L 3G1 Abstract Progress in observational cosmology over the past five years has established that the Universe is dominated dynamically by dark matter and dark energy. Both these new and apparently independent forms of matter-energy have properties that are inconsistent with anything in the existing standard model of particle physics, and it appears that the latter must be extended. We review what is known about dark matter and energy from their impact on the light of the night sky. Most of the candidates that have been proposed so far are not perfectly black, but decay into or otherwise interact with photons in characteristic ways that can be accurately modelled and compared with observational data. We show how experimental limits on the intensity of cosmic background radiation in the microwave, infrared, optical, arXiv:astro-ph/0407207v1 10 Jul 2004 ultraviolet, x-ray and γ-ray bands put strong limits on decaying vacuum energy, light axions, neutrinos, unstable weakly-interacting massive particles (WIMPs) and objects like black holes. Our conclusion is that the dark matter is most likely to be WIMPs if conventional cosmology holds; or higher-dimensional sources if spacetime needs to be extended. Key words: Cosmology, Background radiation, Dark matter, Black holes, Higher-dimensional field theory PACS: 98.80.-k, 98.70.Vc, 95.35.+d, 04.70.Dy, 04.50.+h Email addresses: [email protected] (J.M.
    [Show full text]
  • Eight More Low Luminosity Globular Clusters in the Sagittarius Dwarf Galaxy D
    Astronomy & Astrophysics manuscript no. 40714corr ©ESO 2021 June 8, 2021 Eight more low luminosity globular clusters in the Sagittarius dwarf galaxy D. Minniti1; 2, M. Gómez1, J. Alonso-García3; 4, R. K. Saito5, and E. R. Garro1 1 Departamento de Ciencias Físicas, Facultad de Ciencias Exactas, Universidad Andrés Bello, Fernández Concha 700, Las Condes, Santiago, Chile 2 Vatican Observatory, Vatican City State, V-00120, Italy 3 Centro de Astronomía (CITEVA), Universidad de Antofagasta, Av. Angamos 601, Antofagasta, Chile 4 Millennium Institute of Astrophysics, Santiago, Chile 5 Departamento de Fisica, Universidade Federal de Santa Catarina, Trindade 88040-900, Florianopolis, SC, Brazil Received; Accepted ABSTRACT Context. The Sagittarius (Sgr) dwarf galaxy is merging with the Milky Way, and the study of its globular clusters (GCs) is important to understand the history and outcome of this ongoing process. Aims. Our main goal is to characterize the GC system of the Sgr dwarf galaxy. This task is hampered by high foreground stellar contamination, mostly from the Galactic bulge. Methods. We performed a GC search specifically tailored to find new GC members within the main body of this dwarf galaxy using the combined data of the VISTA Variables in the Via Lactea Extended Survey (VVVX) near-infrared survey and the Gaia Early Data Release 3 (EDR3) optical database. Results. We applied proper motion (PM) cuts to discard foreground bulge and disk stars, and we found a number of GC candidates in the main body of the Sgr dwarf galaxy. We selected the best GCs as those objects that have significant overdensities above the stellar background of the Sgr galaxy and that possess color-magnitude diagrams (CMDs) with well-defined red giant branches (RGBs) consistent with the distance and reddening of this galaxy.
    [Show full text]
  • 978-3642540820 Isbn-10: 3642540821
    2018 Spring — PHYS 315 [8255] Book: Peter Schneider Extragalactic astronomy and cosmology ISBN-13: 978-3642540820 ISBN-10: 3642540821 3 credits Pre-requisites: PHYS122 or PHYS 122H with grade C or higher. A good grade in either PHYS 105 or PHYS 304 will be of some advantage, but not required. Material: scientific calculator Instructor: Professor T.J.Turner Office Hours, M,W,F by appointment only in PHYS 412 Phone 410 455 1978 email [email protected] Overview: The formation, constituents, structure and dynamics of galaxies. Galaxy types. Hierarchy of structure. AGN. Dark matter. Distance estimation. Course objectives: Main objectives are for students to become familiar with the characteristics and components of the various galaxy types in the known universe. Detailed Objectives: By the end of the course students will be able to -describe the various types of galaxies found in the universe -describe some of the observing techniques used in the study of galaxies -understand the components of our Galaxy, the Milky Way -understand the importance of supermassive black holes in galaxy nuclei -understand the importance of galaxy studies to cosmology Grading: Final Exam 20% 2 Mid term Exams 20% each Telescope attendance 10% Class attendance 10% Homework 20% The course will include (provisional topics, may be revised in the details): The Milky Way as a galaxy o Galactic coordinates o Determination of distances within our Galaxy + Trigonometric parallax + Proper motions + Moving cluster parallax + Photometric distance; extinction and reddening + Spectroscopic
    [Show full text]
  • Chemodynamical History of the Galactic Bulge Arxiv:1805.01142V1
    Chemodynamical history of the Galactic Bulge Beatriz Barbuy1, Cristina Chiappini2, Ortwin Gerhard3 1Department of Astronomy, Universidade de S~aoPaulo, S~aoPaulo 05508-090, Brazil; e-mail: [email protected], [email protected] 2Leibniz-Institut f¨urAstrophysik Potsdam (AIP), An der Sternwarte 16, 14482, Potsdam, Germany; e-mail: [email protected] 3Max-Planck-Institut f¨urextraterrestrische Physik P.O. Box 1312. D-85741 Garching, Germany; email: [email protected] Annu. Rev. Astron. Astrophys. 2018. Keywords 56:1{55 Copyright c 2018 by Annual Reviews. bulge, bar, stellar populations, chemical composition, dynamical All rights reserved evolution, chemical evolution, chemodynamical evolution Abstract The Galactic Bulge can uniquely be studied from large samples of in- dividual stars, and is therefore of prime importance for understanding the stellar population structure of bulges in general. Here the observa- tional evidence on the kinematics, chemical composition, and ages of Bulge stellar populations based on photometric and spectroscopic data is reviewed. The bulk of Bulge stars are old and span a metallicity range −1.5∼<[Fe/H]∼<+0.5. Stellar populations and chemical properties suggest a star formation timescale below ∼2 Gyr. The overall Bulge is barred and follows cylindrical rotation, and the more metal-rich stars trace a Box/Peanut (B/P) structure. Dynamical models demonstrate the different spatial and orbital distributions of metal-rich and metal- arXiv:1805.01142v1 [astro-ph.GA] 3 May 2018 poor stars. We discuss current Bulge formation scenarios based on dy- namical, chemical, chemodynamical and cosmological models. Despite impressive progress we do not yet have a successful fully self-consistent chemodynamical Bulge model in the cosmological framework, and we will also need more extensive chrono-chemical-kinematic 3D map of stars to better constrain such models.
    [Show full text]
  • Planets in the Galactic Bulge, Globular Clusters and in Nearby Galaxies
    Planets in the galactic bulge, globular clusters and in nearby Galaxies, or what is the impact of the stellar environment on the formation and evolution of planets? Eike W. Guenther Thüringer Landessternwarte Tautenburg Almost all we know about extrasolar planets is based on stars (planets) in the local solar neighbourhood! In this sense, know almost nothing about planetary systems in the universe! The percentage of stars with planets increases with the mass and the metallicity of the host star Metal rich host stars have more planets. More massive stars have more planets. Johnson et al 2010 The metallicity effect depends on the mass of the planet! Prantzos 2008, based on calculation from Mordasini et al 2006 Whether a massive, outer planet like Jupiter is necessary for the inner planets to be habitable is still an open issue. Consequences of metallicity effect: --> The frequency of (massive) planets should increase towards the inner galaxy. --> Planets should be rare in dwarf galaxies. However, we do not know if the metallicity and the mass of the host star are most important factors for planet formation. What are effects of the stellar density, or the presence/absence of hot ionizing stars in the vicinity? Expected number of extrasolar planet host stars as a function of Galactocentric distance for 6 < R < 10 kpc (Reid 2006). Metallicity effect+ sterilization from Super Novae + 4 Gyrs needed for complex life to emerge --> Galactic habitable zone (Linewaever at al. 2004). Key questions: ---> Is the metallicity and the mass of the host star really the main factors that determine how likely it is that a star has a planet or not? ---> What is the role that the environment plays in the formation and evolution of planets (encounters with other stars, presence of hot stars in the vicinity).
    [Show full text]
  • Evolution of Chemical Abundances in Seyfert Galaxies
    A&A 478, 335–351 (2008) Astronomy DOI: 10.1051/0004-6361:20078663 & c ESO 2008 Astrophysics Evolution of chemical abundances in Seyfert galaxies S. K. Ballero1,2,F.Matteucci1,2, L. Ciotti3,F.Calura2, and P. Padovani4 1 Dipartimento di Astronomia, Università di Trieste, via G.B. Tiepolo 11, 34143 Trieste, Italy e-mail: [email protected] 2 INAF, Osservatorio Astronomico di Trieste, via G.B. Tiepolo 11, 34143 Trieste, Italy 3 Dipartimento di Astronomia, Università di Bologna, via Ranzani 1, 40127 Bologna, Italy 4 European Organisation for Astronomical Research in the Southern Hemisphere (ESO), Karl-Schwarzschild-Str. 2, 85748 Garching bei München, Germany Received 12 September 2007 / Accepted 23 October 2007 ABSTRACT Aims. We study the chemical evolution of spiral bulges hosting Seyfert nuclei, based on updated chemical and spectro-photometrical evolution models for the bulge of our Galaxy, to make predictions about other quantities measured in Seyferts and to model the photometric features of local bulges. The chemical evolution model contains updated and detailed calculations of the Galactic potential and of the feedback from the central supermassive black hole, and the spectro-photometric model covers a wide range of stellar ages and metallicities. 9 11 Methods. We computed the evolution of bulges in the mass range 2 × 10 −10 M by scaling the efficiency of star formation and the bulge scalelength, as in the inverse-wind scenario for elliptical galaxies, and by considering an Eddington limited accretion onto the central supermassive black hole. Results. We successfully reproduced the observed relation between the masses of the black hole and of the host bulge.
    [Show full text]
  • Abstracts of Talks 1
    Abstracts of Talks 1 INVITED AND CONTRIBUTED TALKS (in order of presentation) Milky Way and Magellanic Cloud Surveys for Planetary Nebulae Quentin A. Parker, Macquarie University I will review current major progress in PN surveys in our own Galaxy and the Magellanic clouds whilst giving relevant historical context and background. The recent on-line availability of large-scale wide-field surveys of the Galaxy in several optical and near/mid-infrared passbands has provided unprecedented opportunities to refine selection techniques and eliminate contaminants. This has been coupled with surveys offering improved sensitivity and resolution, permitting more extreme ends of the PN luminosity function to be explored while probing hitherto underrepresented evolutionary states. Known PN in our Galaxy and LMC have been significantly increased over the last few years due primarily to the advent of narrow-band imaging in important nebula lines such as H-alpha, [OIII] and [SIII]. These PNe are generally of lower surface brightness, larger angular extent, in more obscured regions and in later stages of evolution than those in most previous surveys. A more representative PN population for in-depth study is now available, particularly in the LMC where the known distance adds considerable utility for derived PN parameters. Future prospects for Galactic and LMC PN research are briefly highlighted. Local Group Surveys for Planetary Nebulae Laura Magrini, INAF, Osservatorio Astrofisico di Arcetri The Local Group (LG) represents the best environment to study in detail the PN population in a large number of morphological types of galaxies. The closeness of the LG galaxies allows us to investigate the faintest side of the PN luminosity function and to detect PNe also in the less luminous galaxies, the dwarf galaxies, where a small number of them is expected.
    [Show full text]
  • Arxiv:Astro-Ph/9904370V2 4 Jun 1999 Ntecne Forglx Ge Ta.19,Gne Ta.19)An 1997) Al
    updated August 23, 2018 The Black Hole to Bulge Mass Relation in Active Galactic Nuclei A. Wandel1 Racah Institute of Physics, The Hebrew University, Jerusalem 91904, Israel ABSTRACT The masses of the central black holes in Active Galactic Nuclei (AGNs) can be estimated using the broad emission-lines as a probe of the virial mass inside the BLR. Using reverberation mapping to determine the size of the Broad Line Region (BLR) and the width of the variable component of the line profile Hβ line it is possible to find quite accurate virial mass estimates for AGN with adequate data. Compiling a sample of AGN with reliable central masses and bulge magnitudes we find an average black hole to bulge mass ratio of 0.0003, a factor of 20 less than the value found for normal galaxies and for bright quasars. This lower ratio is more consistent with the black hole mass density predicted from quasar light, and agrees with the value found for our Galaxy. We argue that the black hole to bulge mass ratio actually has a significantly larger range than indicated by MBHs detected in normal galaxies (using stellar dynamics) and in bright quasars, which may be biased towards larger black holes , and derive a scenario of black hole growth that explains the observed distribution. arXiv:astro-ph/9904370v2 4 Jun 1999 Subject headings: Galaxy: center — galaxies: active — galaxies: nuclei — galaxies: Seyfert — black holes — quasars: emission-lines — dark matter 1. Introduction Massive black holes (MBHs) have been postulated in quasars and active galaxies (Lynden-Bell 1969, Rees 1984).
    [Show full text]
  • Strong Evidence That the Galactic Bulge Is Shining in Gamma Rays
    Prepared for submission to JCAP Strong Evidence that the Galactic Bulge is Shining in Gamma Rays Oscar Macias,a;b;c Shunsaku Horiuchi,a Manoj Kaplinghat,d Chris Gordon,e Roland M. Crocker,f David M. Natafg aCenter for Neutrino Physics, Department of Physics, Virginia Tech, Blacksburg, VA 24061, USA bKavli Institute for the Physics and Mathematics of the Universe (WPI), University of Tokyo, Kashiwa, Chiba 277-8583, Japan cGRAPPA Institute, University of Amsterdam, 1098 XH Amsterdam, The Netherlands dCenter for Cosmology, Department of Physics and Astronomy, University of California, Irvine, Irvine, California 92697 USA eSchool of Physical and Chemical Sciences, University of Canterbury, Christchurch, New Zealand f Research School of Astronomy and Astrophysics, Australian National University, Canberra, Australia gCenter for Astrophysical Sciences and Department of Physics and Astronomy, The Johns Hopkins University, Baltimore, MD 21218 E-mail: [email protected] Abstract. There is growing evidence that the Galactic Center Excess identified in the Fermi- LAT gamma-ray data arises from a population of faint astrophysical sources. We provide compelling supporting evidence by showing that the morphology of the excess traces the stellar over-density of the Galactic bulge. By adopting a template of the bulge stars obtained from a triaxial 3D fit to the diffuse near-infrared emission, we show that it is detected at high significance. The significance deteriorates when either the position or the orientation of the template is artificially shifted, supporting the correlation of the gamma-ray data with the Galactic bulge. In deriving these results, we have used more sophisticated templates at low-latitudes for the Fermi bubbles compared to previous work and the three-dimensional arXiv:1901.03822v3 [astro-ph.HE] 20 Sep 2019 Inverse Compton (IC) maps recently released by the GALPROP team.
    [Show full text]
  • The Never-Ending Realm of Galaxies
    The Multi-Bang Universe: The Never-Ending Realm of Galaxies Mário Everaldo de Souza Departamento de Física, Universidade Federal de Sergipe, 49.100-000, Brazil Abstract A new cosmological model is proposed for the dynamics of the Universe and the formation and evolution of galaxies. It is shown that the matter of the Universe contracts and expands in cycles, and that galaxies in a particu- lar cycle have imprints from the previous cycle. It is proposed that RHIC’s liquid gets trapped in the cores of galaxies in the beginning of each cycle and is liberated with time and is, thus, the power engine of AGNs. It is also shown that the large-scale structure is a permanent property of the Universe, and thus, it is not created. It is proposed that spiral galaxies and elliptical galaxies are formed by mergers of nucleon vortices (vorteons) at the time of the big squeeze and immediately afterwards and that the merging process, in general, lasts an extremely long time, of many billion years. It is concluded then that the Universe is eternal and that space should be infinite or almost. Keywords Big Bang, RHIC’s liquid, Galaxy Formation, Galaxy Evolution, LCDM Bang Theory: the universal expansion, the Cosmic Micro- 1. Introduction wave Background (CMB) radiation and Primordial or Big The article from 1924 by Alexander Friedmann "Über Bang Nucleosynthesis (BBN). Since then there have been die Möglichkeit einer Welt mit konstanter negativer several improvements in the measurements of the CMB Krümmung des Raumes" ("On the possibility of a world spectrum and its anisotropies by COBE [6], WMAP [7], with constant negative curvature of space") is the theoreti- and Planck 2013 [8].
    [Show full text]
  • GBX2018-Abstract-V2.Pdf
    Scientific Rationale The bulge is a primary component of the Milky Way, comprising ∼25% of its mass. All major Galactic stellar populations intersect there, reaching their highest densities. Thus it is truly a crossroads. Current theory suggests that the bulge is the most ancient component of the Galaxy. Therefore, exploring the bulge is fundamental to understanding Galactic formation, structure and evolution. Indeed, thanks to the advent of multiplexed spectrographs on 8m-class telescopes, and to the availability of resolved, wide-field NIR photometry, our knowledge of the structural, chemical and kinematical properties of the Galactic bulge has improved dramatically in the last few years. At the same time, the interpretation of the accumulated data from this complex region is not straightforward, and many fundamental questions still remain to be answered. E.g. What is the age of the oldest stars? How was the metal-poor spheroid formed? What is the 3D shape of the bulge? What is the connection and interplay between the bulge and bar? Is there a separate bulge globular cluster population? What is the relationship of the central supermassive black hole with the bulge? Fortunately, this area of investigation is moving forward at a fast pace: since 2013, when the last large international conference on the bulge was organized, progress has been truly impressive. New massively multiplexed spectroscopic surveys (Gaia-ESO Survey, APOGEE South, MOONS., new deeper NIR photometric surveys (e.g., VVVX, the extension of the VVV Survey. as well as Gaia have recently begun or will begin imminently. Concomitantly, ever more detailed studies of galaxies at high-redshift promise to catch bulges at the time of their formation.
    [Show full text]