Models of Faint Galaxy Production through Star Cluster Evolution Jarrod Hurley (Centre for Astrophysics & Supercomputing) “Dynamics of Low-Mass Stellar.

Slides:



Advertisements
Similar presentations
Who Wants To Be A Millionaire?
Advertisements

Welcome to Who Wants to be a Millionaire
1 Copyright © 2013 Elsevier Inc. All rights reserved. Appendix 01.
1 VO Theory Use Cases – Intermediate Scale David De Young Project Scientist US NVO IVOA Theory Interest Group S. Lorenzo del Escorial - 10/05.
Multiplication Facts Review. 6 x 4 = 24 5 x 5 = 25.
Number Sense and Operations Exit Patterns, Functions, and Algebra Geometry and Spatial Sense.
Conference Introduction Duncan Forbes Swinburne University.
Accretion High Energy Astrophysics
High energy Astrophysics Mat Page Mullard Space Science Lab, UCL Revision lecture.
Astronomical Solutions to Galactic Dark Matter Will Sutherland Institute of Astronomy, Cambridge.
Welcome to Who Wants to be a Millionaire
£1 Million £500,000 £250,000 £125,000 £64,000 £32,000 £16,000 £8,000 £4,000 £2,000 £1,000 £500 £300 £200 £100 Welcome.
Welcome to Who Wants to be a Millionaire
Welcome to Who Wants to be a Millionaire
$100 $200 $300 $400 $100 $200 $300 $400 $100 $200 $300 $400 $100 $200 $300 $400 $100 $200 $300 $400.
arvard.edu/phot o/2007/m51/. Confronting Stellar Feedback Simulations with Observations of Hot Gas in Elliptical Galaxies Q. Daniel Wang,
Late gas accretion onto primordial mini-halos a model for pre-reionization dwarfs and extragalactic compact High-Velocity Clouds Massimo Ricotti (U of.
From protostellar cores to disk galaxies - Zurich - 09/2007 S.Walch, A.Burkert, T.Naab Munich University Observatory S.Walch, A.Burkert, T.Naab Munich.
Daniel Ceverino (HU) Potsdam, 2009 Avishai Dekel (HU), Reem Sari(HU), Tobias Goerdt(HU), Anatoly Klypin (NMSU) High-Redshift Clumpy Disks & Bulges in Cosmological.
Cold dust in the Galactic halo: first detection of dust emission in a high-velocity cloud : Francois Boulanger et Marc-Antoine Miville-Deschênes Miville.
Dense Molecular Gas in Galaxies Near and Far Yu GAO Purple Mountain Observatory, Nanjing Chinese Academy of Sciences.
Subaru UM 2009/01/15 1 Extended ionized gas regions around the Coma cluster galaxies Michitoshi YOSHIDA Okayama Astrophysical Observatory, NAOJ with Masafumi.
Hot Gas in Damped Lyman- Systems Hidden Baryons & Metals in Galactic Halos at z=2-4 Andrew Fox (ESO-Chile) with P. Petitjean, C. Ledoux, R. Srianand, J.
Observational Constraints on Hot Gas Accretion Joel Bregman University of Michigan Collaborators: Mike Anderson, Xinyu Dai.
VOORBLAD.
15. Oktober Oktober Oktober 2012.
Interactions between Galaxies Galaxy Dynamics Françoise COMBES.
Paul AlexanderThird Cavendish-KAIST Symposium September 2006 Extragalactic Astrophysics and Cosmology in the Cavendish Astrophysics Group Paul Alexander.
10 Year Old Topic 2 9 Year Old Topic 4 8 Year Old Topic 5 8 Year Old Topic 6 7 Year Old Topic 7 7 Year Old Topic 8 6 Year Old Topic 9 6 Year Old Topic.
OPEN DAYS B11 Creating synergies between EU funds: demographic change and active ageing in European Territorial Cooperation and the ESF 9 October.
Multiply Binomials (ax + b)(cx +d) (ax + by)(cx +dy)
SZ effects by using high-resolution simulations Lauro Moscardini Dipartimento di Astronomia Università di Bologna, Italy Orsay,
Benjamin Banneker Charter Academy of Technology Making AYP Benjamin Banneker Charter Academy of Technology Making AYP.
Slippery Slope
Equations of Circles. Equation of a Circle The center of a circle is given by (h, k) The radius of a circle is given by r The equation of a circle in.
Star Formation at Very Low Metallicity Anne-Katharina Jappsen.
Yuichi Matsuda (NAOJ) 松田 有一(国立天文台) Ly-alpha morphology-density high-z 1.
©Brooks/Cole, 2001 Chapter 12 Derived Types-- Enumerated, Structure and Union.
Zurück zur ersten Seite Dynamical Decay of Young Few-Body Clusters and “Isolated“ T Tauri Stars Michael Sterzik, ESO Richard Durisen, Indiana University.
Number Factors and Multiples Saturday, 09 September 2006 ©RSH.
EXAMPLE 3 Use synthetic division
THE CASE FOR MODIFIED GRAVITY James Binney Oxford University.
The Large Scale Structure of the Universe Clusters of galaxies X-rays from clusters of galaxies Sheets and voids.
European Southern Observatory
General Astrophysics with TPF-C David Spergel Princeton.
Tidal Disruption from Supermassive Black Hole Binaries in Merging Galaxies: Before & After the Coalescence Shuo Li NAOC Collaborated with Rainer Spurzem,
Tidal Disruption of Globular Clusters in Dwarf Galaxies J. Peñarrubia Santiago 2011 in collaboration with: M.Walker; G. Gilmore & S. Koposov.
Particle Astrophysics & Cosmology SS Chapter 7 Dark Matter.
Simon Portegies Zwart (Univ. Amsterdam with 2 GRAPE-6 boards)
Particle Astrophysics & Cosmology SS Chapter 8 Structure Formation.
The Nature of the Least Luminous Galaxies Josh Simon Carnegie Observatories Josh Simon Carnegie Observatories Marla Geha (Yale) Quinn Minor (SUNY Oneonta)
The Milky Way Galaxy James Binney Oxford University.
The remote globular cluster system of M31 LAMOST Workshop, 19 th July 2010 Dougal Mackey (RSAA, ANU)1 The Newly-Discovered Remote Globular Cluster System.
Hot gas in galaxy pairs Olga Melnyk. It is known that the dark matter is concentrated in individual haloes of galaxies and is located in the volume of.
The accretion history of the halo of M31 as probed by its globular cluster population Avon Huxor et al. Astrophysics Group HH Wills Physics Laboratory.
White Dwarf Binaries in Globular Clusters Fred Rasio (Northwestern)
Globular Cluters in Dwarf Galaxies. But first, a digression regarding tides... Leo I.
A CDM view of the Local Group dSphs Jorge Peñarrubia In collaboration with Julio F. Navarro & Alan McConnachie Jorge Peñarrubia In collaboration with Julio.
Globular Cluster - Dwarf Galaxy Connection W1: a case study in our neighborhood Ann Arbor, Aug Beth Willman W1 DEIMOS Observations M.Geha (HIA/Yale)
The Ultra-Faint Milky Way Satellites
The influence of baryons on the matter distribution and shape of dark matter halos Weipeng Lin , Yipeng Jing ( Shanghai Astronomical Observatory , CAS.
Mass Profiles of Galaxy Clusters Drew Newman Newman et al. 2009, “The Distribution of Dark Matter Over Three Decades in Radius in the Lensing Cluster Abell.
The formation of ultra-compact dwarf galaxies and nucleated dwarf galaxies Collaborators: Ben Moore, Stelios Kazantzidis, Tobias Kaufmann, Andrea V. Macciò.
Pete Kuzma PhD student, Research School of Astronomy and Astrophysics
Learning about first galaxies using large surveys
Grand Rotation Curves & Galactic Roche Lobes in the Galaxy and M31 Yoshiaki Sofue (Meisei Uni.) at Meisei University.
The “Milky Way”.
Modeling the Extended Structure of Dwarf Spheroidals (Carina, Leo I)
(spectroscopically confirmed)
Presentation transcript:

Models of Faint Galaxy Production through Star Cluster Evolution Jarrod Hurley (Centre for Astrophysics & Supercomputing) “Dynamics of Low-Mass Stellar Systems” ESO, Santiago, Chile April

Models of Faint Galaxy Production through Star Cluster Evolution Sizes of low-mass stellar systems Huxor+11

Models of Faint Galaxy Production through Star Cluster Evolution Sizes of low-mass stellar systems Huxor+11 MW M31

Models of Faint Galaxy Production through Star Cluster Evolution Sizes of low-mass stellar systems Huxor+11 MW M31 dIrr

Models of Faint Galaxy Production through Star Cluster Evolution Sizes of low-mass stellar systems Huxor+11 M31 dIrr DM halo MW M31

Models of Faint Galaxy Production through Star Cluster Evolution simulations of low-mass stellar systems in different tidal fields Huxor+11 M31 dIrr DM halo MW M31

Models of Faint Galaxy Production through Star Cluster Evolution N-body simulation background Equation of Motion O(N 3 ) special-purpose GRAPE hardware stellar evolution binary evolution techniques for few-body subsystems tidal field [Hurley et al. 2001] [Mardling & Aarseth 2001; Mikkola 2006, etc.] [ NBODY4/NBODY6: Aarseth 1999; Aarseth 2003] GPU

Models of Faint Galaxy Production through Star Cluster Evolution Models of Extended Clusters? N = 100,000, 5% binaries, Z = 0.001, KTG IMF, Plummer/King

Models of Faint Galaxy Production through Star Cluster Evolution Models of Extended Clusters? N = 100,000, 5% binaries, Z = 0.001, KTG IMF, Plummer/King R GC = 10 kpc M G = 9x10 9 M sun M = 9x10 10 M sun point-mass point-mass or 3-component e.g. NGC6822 e.g. M31

Models of Faint Galaxy Production through Star Cluster Evolution Models of Extended Clusters? N = 100,000, 5% binaries, Z = 0.001, KTG IMF, Plummer/King e.g. NGC6822 e.g. M31

Models of Faint Galaxy Production through Star Cluster Evolution Models of Extended Clusters? N = 100,000, 5% binaries, Z = 0.001, KTG IMF, Plummer/King Hurley+Mackey10

Models of Faint Galaxy Production through Star Cluster Evolution Models of Extended Clusters? Da Costa+09

Models of Faint Galaxy Production through Star Cluster Evolution Models of Extended Clusters? Da Costa+09

Models of Faint Galaxy Production through Star Cluster Evolution The N = 200,000 model 200k 2% binaries R gc = 4 kpc 100k 5% binaries R gc = 8.5 kpc

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? size/pc sigma ~ 3-10 km/s Strigari+08

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? M NFW = 10 9 c = 16 R gc = 0.5 kpc

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? M NFW = 10 9 c = 16 R gc = 0.5 kpc

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? M NFW = 10 9 c = 16 R gc = 0.5 kpc

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? M NFW = 10 9 c = 16 R gc = 0.5 kpc

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20 N = 100,000, 5% binaries N = 28,000, 40% binaries

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20 Sand+10 Leo IV

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20 r pl = 27 pc r pl = 15 pc

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? N = 100,000, 5% binaries N = 28,000, 40% binaries Star cluster near centre (R gc =20pc), M NFW = 10 8, c=20 Martin+08

Models of Faint Galaxy Production through Star Cluster Evolution Models of Ultra-Faint Dwarfs? M 300 ~ 0.7x10 7 M sun sigma ~ 5 km/s

Models of Faint Galaxy Production through Star Cluster Evolution Future … complex tidal fields definition of tidal radius? explore initial N, f b, density, sigma … non-virial protoclusters, e.g. Hurley+Bekki08 include gas? …

N-body simulation background