Dark Matter: Observations, Theories, Experiments Szydagis 02.25.2015 1 / 17 Figure credit: X-ray: NASA/CXC/CfA/M. Markevitch et al.; Lensing Map: NASA/STScI; ESO WFI; Magellan/U. Arizona/ D. Clowe et al.; Optical image: NASA/STScI; Magellan/U. Arizona/D. Clowe et al.; Right: NASA / ESA / M. Bradac et al. An invisible universe out there!
Dark Matter: Observations, Theories, Experiments Szydagis 02.25.2015 1 / 17 Figure credit: X-ray: NASA/CXC/CfA/M. Markevitch et al.; Lensing Map: NASA/STScI;
Dark Matter: Observations, Theories, Experiments Szydagis
02.25.2015 1 / 17 Figure credit: X-ray: NASA/CXC/CfA/M. Markevitch
et al.; Lensing Map: NASA/STScI; ESO WFI; Magellan/U. Arizona/ D.
Clowe et al.; Optical image: NASA/STScI; Magellan/U. Arizona/D.
Clowe et al.; Right: NASA / ESA / M. Bradac et al. An invisible
universe out there!
Slide 2
A Fun Activity Three sets of groups based on where you are
siting Window: theory of modified gravity (use Rubin) Near me: dark
matter. Debate with window group Center of room: Design your own
dark matter detection experiment (direct or indirect/observational)
geared towards discovery and/or telling the difference between dark
matter and modified gravity models From articles, previous
knowledge, or fresh ideas Ambiguous location? Choose what you want
to do 5 minutes for discussion. 5-10 for public reporting 2 /
17
Slide 3
Historical Perspective In 1933, the Swiss astronomer Fritz
Zwicky discovered there was insufficient luminous matter in the
stars of the Coma cluster Based on looking at kinetic energies of
galaxies Too high: cluster should fly apart, unbound Famous for
coining todays term dark matter In 1970s, American astronomer Vera
Rubin found new, intragalactic piece of the puzzle Today: wealth of
observational evidence yet *conclusive* detection remains elusive
Image credit: zwicky-stiftung.ch Image credit: Princeton University
3 / 17
Slide 4
Rotation Curves Galaxies rotation curves consistently exhibit
unexpected behavior, consistent with missing mass at the ~90% level
~0.3 GeV/cm 3 in the Milky Way Intragalactic rotational speeds
gravitationally consistent with there being more matter than is
visible (shining) in the stars 4 / 17
http://w3.iihe.ac.be/icecube/3_Activities/1_WIMPs%20Analysis /,
~200 km/s for dark matter near sun, earth
Slide 5
Gravitational Lensing Gravitational distortion of light by
matter enables a calculation of the mass of the matter doing the
distorting (we saw on Feb. 9) Predicted by Einstein (in GR) and
first hint observed during a solar eclipse in 1919, but not as
galactic-scale lens until 1979 Our gravitational lensing studies
(especially of weak) concur with the rotation curves: extra mass! 5
/ 17 Credit: Karen Teramura, University of Hawai'i Institute for
Astronomy Image: NASA/ESA
Slide 6
The Bullet Cluster Considered nail in coffin for modified
gravity ideas Hot x-ray emitting gas in red superimposed in false
color on optical image Greatest mass, probable dark matter, in blue
(mapped using lensing) Galaxies collided but dark matter evaded
collision 6 / 17 Composite Credit: X-ray: NASA/CXC/CfA/M.
Markevitch et al.;M. Markevitch et al.; Lensing Map: NASA/STScI;
ESO WFI; Magellan/U. Arizona/D. Clowe et al.D. Clowe et al.
Optical: NASA/STScI; Magellan/U. Arizona/D. Clowe et al. > 1 Gpc
away!
Slide 7
Cosmic Microwave Background Echo, snapshot from ~400,000 years
after Big Bang, when photons and the plasma decoupled CMB favors
model where 27% of energy content of universe is in matter, but in
non-baryonic particles The best fit for explaining the angular
power spectrum of the temperature anisotropy Nucleosynthesis
agrees! 7 / 17 This pie chart and the intense calculations that
accompany it have come to be known by concordance as the Standard
Cosmological Model (or, CDM) Images: ESA / Planck Collaboration |
2013
Slide 8
Large-Scale Structure Observations (baryon acoustic
oscillations, galaxy clusters) and simulations agree well when the
presence of *cold* (non-relativistic) dark matter assumed We need
dark matter interacting weakly (as in rarely not necessarily via
the weak force), gravitationally (only?) 8 / 17 Michael L. Norman,
arXiv:1005.1 100 Difficult to achieve with hot dark matter, like
neutrinos. In the essay by Vera Rubin, she said we dont understand
the bubble + void structure of clusters and superclusters, but that
was late 80s!!
Slide 9
Particle Candidates The WIMP, or, the W eakly I nteracting M
assive P article = the vanilla candidate But, no Standard Model
particle has all needed traits Cold/slow (must be heavy) Cant be a
baryon (p, n, etc.) Interacts very weakly Stable, or very
long-lived Natural in SUSY or Kaluza- Klein (higher dimensions) 9 /
17 Fermilab fermions and bosons sfermions and bosinos Dirk
Laureyssens, 2002 / 2003 EXTRA SPATIAL DIMENSIONS? (analo- gous to
anti- matter)
Slide 10
Alternative Notions MACHOs: Ma ssive C ompact H alo O bjects
(joke with WIMP) Black holes, neutron stars, brown dwarfs
(protostars that failed to ignite, mega-Jupiter-sized), rogue
planets, anything non-luminous Dead concept: would result in
disagreement with our latest CMB measurements. Perhaps part of dark
matter, but cant be majority Axion (named after detergent), scalar
boson like heavy photon Hypothetical new particle that explains why
the strong nuclear force does not appear to break CP
(charge-parity) symmetry, when it should (strong CP problem, QCD:
Quantum Chromodynamics) Still in the running! Though as with WIMPs
no hard evidence yet Looking for them by trying to shine light
through walls, looking at sun, using high magnetic fields
(axioelectric effect), RF cavities 10 / 17
Slide 11
The WIMP Miracle As the universe expands, different types
(masses) of particles thermally freeze out at different times
Temperatures falling, with universe cooling off Dilution: drop in
densities Freeze-out occurs when particles can no longer find each
other (too far) or other types and interact 11 / 17 Dan Hooper,
FNAL With a weak-force cross- section (probability of scattering) a
~100 GeV mass (100x proton) particle would give us ALMOST EXACTLY
the dark matter energy density observed today, as a thermal relic
Beautiful picture, but sadly kind of dead (WIMP-less miracle?)
because havent found anything
Slide 12
Detection Strategies Indirect detection of dark matter (DM)
self- annihilation into Standard Model (SM) particles (gammas and
neutrinos) Direct detection, my focus today, since this is my work
Production of dark matter particles from the high- energy
collisions of a particle accelerator (LHC) 12 / 17 Diagram: Mike
Woods Collider experiments, like CMS, ATLAS (UAlbany works on)
Fermi-LAT, IceCube
Slide 13
Direct Detection Method Most searches are geared toward finding
WIMPs, in a model-independent fashion Something going bump in the
night, above background In most models, WIMPs scatter elastically
off nucleons (billiard-ball-like) Experiments deployed deep
underground, because depth reduces (overwhelming-rate) cosmic-ray
backgrounds 13 / 17 Mike Attisha, CDMS collaboration 2 main
interaction types: nuclear and electron recoil Low-energy
(exponentially favored) nuclear recoils (NR) are expected from
WIMPs, and electron recoils (ER) constitute primary background to
avoid misidentifying
Slide 14
Detector Response Atoms can be excited and scintillate and/or
be fully ionized by NR/ER Recoils can also cause lattice
vibrations, or boil superheated liquids Most robust searches
combine two methods Given rare interaction, figure of merit =
target mass X exposure time 14 / 17 charge from ionization
(electrons liberated) phonons (excitations within crystalline
structures) bubbles, boiling heat (atomic motion) light from
de-excitation (scintillation)
Slide 15
How Works A two-phase Xe detector Example of a time- projection
chamber (TPC) 122 photomultiplier tubes (PMTs) convert photons into
photo-electrons (phe) via photoelectric effect S1 (primary) and S2
(secondary) scintillation light, latter from charge Ratio tells you
ER or NR Sum gives you energy 15 / 17
Slide 16
Competitors (Lots) XENON, PandaX: same as LUX, the leader
(Europe, China) Spherical version (no electric field and
all-liquid): XMASS DarkSide, ArDM, DEAP/CLEAN: Similar concept
except instead of xenon with argon (not as dense, but also
scintillates, noble, and has advantage of S1 pulse-shape
discrimination) CDMS (one of first), CoGeNT: germanium crystals,
reading ionization (CDMS phonons too). Costly, difficult to scale
up, but low in background and good for low-mass WIMPs PICO, SIMPLE:
superheated fluids. Blind to ER backgrounds, but energy=? on
event-by-event level. Best for SD-proton 16 / 17
Slide 17
Conclusion & Homework 17 / 17 LUX (2014), 85 live-days
exclusion limit curve uncertainty band (in expected result)
XENON100 (2012), 225 live-days XENON100 (2011), 100 live-days
ZEPLIN-III CDMS-II Ge Edelweiss-II Some claims of discovery exist
(for light WIMPs) NOT discovering something is oftentimes equally
as valuable as discovering something (think Michelson-Morley and
the aether) Old HW: Make sure you do written assignment #5 by next
time (Friday) And you should have finished all of your dark matter
reading by today !! New HW: The 10 Greatest Discoveries of Modern
Astronomy http://wildammo.com/2010/10/22/t
he-10-most-amazing-discoveries-of- modern-astronomy/ (dark energy
tops the list) http://wildammo.com/2010/10/22/t
he-10-most-amazing-discoveries-of- modern-astronomy/ A Faster Walk
on the Dark Side http://cosmictimes.gsfc.nas
a.gov/teachers/guide/2006 /guide/faster_walk.html
http://cosmictimes.gsfc.nas a.gov/teachers/guide/2006
/guide/faster_walk.html HubbleSite Hubble Breakthroughs Cosmology
Science http://hubblesite.org/hubb le_discoveries/breakthroug
hs/cosmology http://hubblesite.org/hubb le_discoveries/breakthroug
hs/cosmology Including sublink http://hubblesite.org/h
ubble_discoveries/dark _energy/ (Find Out: Discovering Dark Energy)
http://hubblesite.org/h ubble_discoveries/dark _energy/ Dark
Questions Remain over Dark Energy (ABC) http://www.abc.net.au/sc
ience/articles/2009/12/0 9/2765371.htm http://www.abc.net.au/sc
ience/articles/2009/12/0 9/2765371.htm