Dark Matter: What is it? Where is it? Do we need it? How much? History: 1937: like many things in astronomy, dark matter was first postulated by Fritz Zwicky. Apply virial theorem to indiv. galaxies in the Virgo cluster Mgalaxy Apply virial theorem to cluster as a whole Mcluster Zwicky found M/Lcluster ~200 ?? M/Lgalaxy~8 ~1970: Vera Rubin, Ken Freeman and others explore rotation curves and (re-)find the need for dark matter (formerly called missing). Actual diagnosis: gravity acts stronger than expected on the basis of the identified mass (=sources of gravity) Reading: J Peacock, Cosmological Physics, Cambridge Press p367-386 rix@mpia.de Vatican 2003 Lecture 26 HWR Dark Matter on Different Scales • Basic hypotheses to test: – there is universal “dark matter”, which • was initially distributed like all known matter • interacts with the observed matter (and itself) mostly through gravity – OR, • there is a universal modification to the laws of gravity (Newton AND Einstein) that acts at large scales and/or weak accelerations. • Dark Matter appears to be needed in: – – – – – – rix@mpia.de Dwarf spheroidal galaxies: 500 pc Large galaxies: 20 kpc Galaxy halos: 50-500 kpc Galaxy Clusters: 1 Mpc Large-Scale Structure: 20 Mpc Cosmic Microwave Background Vatican 2003 Lecture 26 HWR Dark Matter Evidence Nearby: the Draco dwarf galaxy Sky image of Draco Stellar density contours of Draco from SDSS Odenkirchen et al 2001 Draco is a bound system in equilibrium Dsun rix@mpia.de 70 kpc Vatican 2003 Lecture 26 HWR Radial Profile and Kinematics of Draco Stellar density profile of Draco Modelling options 1) Stars only tot(r) = *(r) 2) Stars + DM: tot(r) = *(r) + DM(r) Giant stars with velocities measured • Estimate *(r) from stellar distribution • Giant stars as kinematic tracers - need velocity precision of 3 km/s rix@mpia.de Vatican 2003 Lecture 26 HWR Mass Modelling of Draco Velocity dispersion profile Expected (M/L)* ~ 2 Draco is dark matter dominated Jeans equation model Enclosed mass Try models with different DM profiles M (<10‘) well constrained rix@mpia.de Vatican 2003 Lecture 26 HWR Rotation Curves of Spiral Galaxies •Rotation curves show that DM is needed •Total (stars,gas,DM) rotation curve is v~const. for 2-8 Rexp •A so-called non-singular isothermal (s=const.) DM distribution often fits 2 well: r (r ) r0 / 1 r / rc •But, is this dark matter profile •Physically motivated? •Physically plausible? •Expectation from cosmological simulations: NFW profile r~r-1 at small radii and r~r-3 at large radii rix@mpia.de Vatican 2003 Lecture 26 HWR Degeneracies in Fitting Rotation Curves Rotation curves do not contain enough information to: Determine the ratio of star to DM mass Distinguish the radial profile of DM Van Albada et al 1985, ApJ, 295, 305 Navarro 1997 rix@mpia.de Dark matter at small radii is poorly understood! Vatican 2003 Lecture 26 HWR Dark Matter in Galaxy Halos Satellites to the Milky Way Prada et al 2003 tracers of the mass in the halo SDSS sample: isolated MW-like galaxies 0.5 satellites per galaxy x 1000 galaxies Synthetic galaxy with 500 satellites MW-like galaxies are at the center ofsystems dark unbound matter halos that extend to >200 kpc • identify satellite candidates • make a conservative rejection of unbound systems • calculate resulting velocity dispersion of satellites • compare to cosmological halo formation models good match rix@mpia.de DM density profile in the outer parts r~r-3 Vatican 2003 Lecture 26 HWR Dark Matter in Galaxy Clusters In galaxy clusters the masses can be measured three ways • Galaxy clusters contain hot gas ( bound by dark matter?) • Galaxy velocity dispersion • Gravitational lensing T = 106 K X-ray emission rix@mpia.de Vatican 2003 Lecture 26 HWR X-Ray Gas in Hydrostatic Exquilibrium dP GM ( r ) r 2 dr r M ( r ) kT d ln g d ln T ( ) mH g d ln r d ln r Mstars~Mgas~3x1013MSun Mtot,cluster(Rvirial)~1015MSun rix@mpia.de Vatican 2003 Lecture 26 HWR Other Lines of Evidence For Dark Matter • Gravitational lensing (Hans-Walter, next week) dark matter clumping on largest scales • The Cosmic Microwave Background and the curvature of space (Rachel, Friday) WM~0.27 • The growth of small fluctuations to strong fluctuations (Rachel, next week) rix@mpia.de Vatican 2003 Lecture 26 HWR Alternatives to Dark Matter • MOND: Modified Newtonian Dynamics (Milgrom 1980s-) Ansatz: for accelerations a less than a0, gravity behaves as a(a/a0) = GM/r2 as a(r) ~ 1/r of a < a0: flat rotation curves Note: • a < a0 untested in the lab • single value of a0 works for all rotation curves But: • No relativistic version of MOND • MOND has trouble explaining DM in cluster and far out in halos rix@mpia.de Vatican 2003 Lecture 26 HWR Summary: Dark Matter Evidence • A wide range of dynamical phenomena cannot be explained through the known (baryonic) mass content of the universe alone. • All (well, almost all) these problems can be solved if we make one radical assumption: 85% of all matter with rest mass (WM 0.25) is in a form (dark matter) that was – initially distributed as ordinary matter – interacts with the rest (almost) only through gravity – acts like a collisionless “fluid” • is cold, i.e. consists of non-relativistic particles • Stars,gas are now more concentrated/clumped than DM • We also need a “cosmological” constant (vacuum energy), i.e. a longdistance ‘repulsive’ force rix@mpia.de – galaxies sit at the center of much larger DM halos – Note: rbaryon ~8 x rstars Vatican 2003 Lecture 26 HWR rix@mpia.de Vatican 2003 Lecture 26 HWR Nature of the Dark Matter • Non-baryonic, to reconcile WM ~0.27 with primordial nucleosynthesis Wb~0.018 and large-scale structure growth • Cold: must not escape from potential wells • (Cold) Dark Matter Candidates: – Black holes – Low-mass objects (“MACHO”s, free-floating planets) – Elementary particles Massive Black Holes as Dark Matter Candidates – (one) plausible mass range: ~106 Msun (Lacey and Ostriker, 1985) – But, such massive black holes cannot be the dark matter in dwarf galaxies (Rix and Lake, 1985). – E.g. c.a. 80 BH’s in Draco, they would disrupt the galaxies! rix@mpia.de Vatican 2003 Lecture 26 HWR • MACHO’s: Massive Compact Halo Objects – Potential mass range: 0.08 MSun (stellar limit) to MEarth Observational test: gravitational microlensing • (MACHO and OGLE) experiments. Idea: • if all the dark matter in the Milky Way’s halo was MACHOS • there is a 10-6 chance that a star (e.g. in the Magellanic Cloud) has a MACHO exactly along the line of sight • focussing brightening of the stars’ image • as stars move dime dependent light curve. Implementation: monitor 106 stars rix@mpia.de Vatican 2003 Lecture 26 HWR Microlensing Searches Large Magellanic Cloud Micro-Lensing Cartoon Lensing Lightcurve rix@mpia.de Vatican 2003 Lecture 26 HWR Are MACHOs the Dark Matter? •MACHO’s make up (at most) 15% of the Milky Ways halo mass MACHO Mass •Inferred mass range: 0.4MSun Why would they be invisible? MACHOs are an enigma, but certainly not the solution to the dark matter problem Halo Mass Fraction in MACHOs rix@mpia.de Alternative: lensing by ordinary stars in the LMC or MW Vatican 2003 Lecture 26 HWR WIMPS as Dark Matter Candidates • “cold” Dark Matter: must become non-relativistic already at T >> 104K clumping • supersymmetric theories (SUSY) can naturally create particle (pairs with their SUSY partner) - lightest SUSY particle stable: neutralino, gravitino, higgsino, etc. • axions: hypothesized, very light particle; may arise in quantum chromodynamics WIMPS are a plausible, but not firm, consequence of several theories in particle physics rix@mpia.de Vatican 2003 Lecture 26 HWR Towards detecting WIMPS • WIMPS: may have exceedingly rare elastic scattering events with crystals and one may measure the recoil. • However: many other particles/processes interact with crystals high false detection rate. • Reduce background deep tunnels (e.g. Gran Sasso) • Search for seasonal signature rix@mpia.de Vatican 2003 Lecture 26 HWR A first detection? … Or not The DAMA experiment in the Gran Sasso claimed to have found a seasonal variation ? 50 GeV particles Other experiments seem to rule out DAMA PROBLEM: cross-section could be 1000 times smaller than current limits rix@mpia.de Vatican 2003 Lecture 26 HWR Dark Matter Up-Shot • Cold, collisionless ‚Dark Matter‘ with WDM 0.25 explains a wide range of phenomena (not only rotation curves) •„universal dark matter“ works •Stars/cold gas are concentrated/clumped than DM •DM poorly understood inside galaxies • Nature of Dark Matter unknown •We only know what it is NOT! rix@mpia.de Vatican 2003 Lecture 26 HWR