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Introduction to Astrophysics
Professor David Cinabro
1
Thursday, April 25, 2013
Disclaimer
• Subject is vast• Covers everything from Physics of the
Atmosphere to the Origin and Fate of the Universe and everything in between
• Impossible to introduce all of it in ~1 hour
• Focus on research we do here– Professor Cinabro - Cosmology with SN– Professor Hackett - Accretion 2
Thursday, April 25, 2013
Cosmology with Supernovas
David Cinabro
Thursday, April 25, 2013
Cosmology Background• The study of the origin and evolution of
the Universe.• Last 20 years have been a “golden age”
in which we have learned:– Origin is a giant explosion known as the
Big Bang– Fate is most likely continued expansion– Most of the Universe is in the Dark Sector:
• Dark Matter: Unknown sort that dominates over ordinary matter
• Dark Energy: Unknown force that is pushing the Universe apart
Thursday, April 25, 2013
Discovery of the Expanding Universe: Hubble 1929
Finds that thevelocity gets larger with distance, the Hubble Law, and slope is the Hubble parameter, H
Measured distances to 25 galaxies:• Used cepheids for Andromeda and Local Group• Used brightest stars in the others• Compared distances with recession velocities.
Thursday, April 25, 2013
Echo of the Explosion: Gamow (1948)• Gamow and Alpher consider
the consequences of an expanding Universe.
• First conclusion is that the Universe should be filled with E+M radiaHon leI over from when it was small and hot.
• Today should be Microwaves (Blackbody with T = 3K).
Thursday, April 25, 2013
Cosmic Microwaves (1963)• Serendipitously observed at Bell Labs using a communicaHons instrument.
• Death blow to alternate Steady State cosmology of Fred Hoyle.
Thursday, April 25, 2013
Astronomer’s Periodic Table• Gamow, Alpher, Herman add in Nuclear Physics to calculate the abundances of the elements arising from the hot, dense early Universe (1948-‐56).
• Agrees with observaHons that grow increasingly precise.
Thursday, April 25, 2013
Triumph of the Big Bang• Ironically the term was coined ironically by Fred Hoyle, supporter of Steady State, in a 1949 radio broadcast.
• Three pillars:
1) Expanding Universe
2) Cosmic Microwave Background
3) Cosmic Elemental Abundances
• Only serious Cosmology by the mid-‐1970’s
• Unfortunately it leaves only two alternaHves for the fate of the Universe…
Thursday, April 25, 2013
Big Bang starts the expansion of the universe. But there is enough mass in the universe that gravity captures all the galaxies, the universe begins to contract, making gravity stronger, accelerates contracHon, and eventually the universe is compressed into a single point(?). We call this…
Thursday, April 25, 2013
The Big Crunch
Big Bang starts the expansion of the universe. But there is enough mass in the universe that gravity captures all the galaxies, the universe begins to contract, making gravity stronger, accelerates contracHon, and eventually the universe is compressed into a single point(?). We call this…
Thursday, April 25, 2013
Big Bang starts the expansion of the universe. But there is not enough mass in the universe for gravity to capture the galaxies, and the universe expands, at an ever slowing rate, forever. Stars begin to run out of fuel and burn out, and since the universe gets less and less dense no new stars form. It gets colder and colder unHl the universe freezes to death. We call this…
Thursday, April 25, 2013
The Big Chill
Big Bang starts the expansion of the universe. But there is not enough mass in the universe for gravity to capture the galaxies, and the universe expands, at an ever slowing rate, forever. Stars begin to run out of fuel and burn out, and since the universe gets less and less dense no new stars form. It gets colder and colder unHl the universe
Thursday, April 25, 2013
Cosmic Microwave BackgroundSnap shot of matter density of the universe at the photon surface of last scattering. Most accurate from Planck satellite.
Thursday, April 25, 2013
M51: June 2005 M51: July 2005
Thursday, April 25, 2013
Galaxy Clustering(Daniel Eisenstein)
Thursday, April 25, 2013
Galaxy Clustering(Daniel Eisenstein)
Thursday, April 25, 2013
Galaxy Clustering(Daniel Eisenstein)
Thursday, April 25, 2013
Galaxy Clustering(Daniel Eisenstein)
Thursday, April 25, 2013
Galaxy ClusteringObserve this in the distance between neighboring galaxies in large galaxy surveys such as Sloan Digital Sky Survey
Thursday, April 25, 2013
Describing the Universe
• How Astronomers describe the Universe on the cosmological scale.
• Repulsive cosmological constant(Λ) versus agracHve mass(m).
• 1.0 = Enough agracHve to force Big Crunch.
Ω
Ω
Λ
m1.0
1.0
Big Chill
Big Crunch
No Big Bang
0.0
Thursday, April 25, 2013
Concordance Model Cosmology
• Another three pillars
1) CMB map
2) SNIa vs redshiI
3) Galaxy clustering
• Dark Energy is most like a strong version of Einstein’s Cosmological Constant
Thursday, April 25, 2013
Cosmologies Golden Age
• The Universe is mostly stuff about which we are IGNORANT.
• Countless explanaHons, but none are very saHsfying and as yet no experiment or observaHon are decisive on the nature of the Dark Sector.
Thursday, April 25, 2013
Sloan Digital Sky Survey Supernova Search
• World’s sample of Supernovas is quite small (~1000)
• More would allow tests of Dark Energy (Is it constant in time? Is it constant in
space?)• Sloan Digital Sky Survey ideal for this
work (www.sdss.org)
Thursday, April 25, 2013
Supernova Candidate
Thursday, April 25, 2013
Asteroid
Thursday, April 25, 2013
Thursday, April 25, 2013
Thursday, April 25, 2013
Core Collapse SN Rate
29
Thursday, April 25, 2013
Galaxy Host Properties
30
Thursday, April 25, 2013
Galaxy Host Properties
31
Thursday, April 25, 2013
CCD R&D at LBNL
32
Thursday, April 25, 2013
REU Student Opportunities
• Vast• Continued analysis of SDSS-SN data set:
Comparison of model CCSN with real CCSN, Hostless SN... Opportunities at FNAL.
• MS-DESI: Take astro spectra like SDSS took images. CCD R&D work at LBNL.
• LSST: Monster scale up of SDSS. Workers needed for simulation and hardware. Opportunities at SLAC.
• Development of SN Software Analysis package SNANA. Work with WSU Comp Sci. 33
Thursday, April 25, 2013
ACCRETION POWER IN ASTROPHYSICS
Professor Cackettac・cre・ tion \a-ʻkrē-shən\: noun
the process of growth or enlargement typically by the gradual accumulation of additional layers or matter
Thursday, April 25, 2013
ACCRETION
• Accretion: process by which an object gains/accumulates mass
• Extremely important process throughout the Universe from young stars to supermassive black holes at the centers of galaxies
A young star forming and accreting matter from a disk
Credit: Hubble Space Telescope
Disk of gas
Jet
Artist’s impression of accretion onto a black hole
Thursday, April 25, 2013
A SOURCE OF ENERGY• Extraction of gravitational
potential energy as material accretes onto a massive object
➡ gravitational potential energy converted to radiation through friction
• Due to conservation of angular momentum, accreting material usually forms a rotating thin disk
Accretion in binary system
Accretion disk
Thursday, April 25, 2013
MORE EFFICIENT THAN FUSION!• Nuclear fusion, which powers
stars, is less than 1% efficient for H ➞ He:
Enuc = 0.007 mc2
• Energy from accretion is given by:
Eacc = GMm/R
• For compact objects (neutron star or black hole) accretion is greater than 20 times more efficient than fusion!
Nuclear fusion powers stars like the Sun
Thursday, April 25, 2013
MAXIMUM ACCRETION RATE
• As Eacc = GMm/R the more massive an object and the smaller it is, the greater the energy released through accretion
• But, there is a limit to how much energy is radiated away, the Eddington Limit: inward gravitational force on matter must be greater than the outward radiation pressure otherwise it would blow itself apart
Einstein & Eddington at the University of Cambridge
Thursday, April 25, 2013
COMPACT OBJECTS
• Accretion most powerful onto compact objects
• Black hole: a massive object whose gravitational force is so strong that not even light can escape
• Neutron star: a star about 1.5 times the mass of the Sun, but with a radius of only ~10 km - a star the size of a city!
Light near a black hole gets bent by the strong gravity there
Thursday, April 25, 2013
BLACK HOLESCome in several ‘flavors’:
• stellar-mass black holes (~10 Msun)
➡ formed in supernovae
• supermassive black holes (106 - 109 Msun)
➡ found at the centers of galaxies
Stars orbiting around the black hole at the center of the Milky
Way
Thursday, April 25, 2013
BLACK HOLESCome in several ‘flavors’:
• stellar-mass black holes (~10 Msun)
➡ formed in supernovae
• supermassive black holes (106 - 109 Msun)
➡ found at the centers of galaxies
Stars orbiting around the black hole at the center of the Milky
Way
Thursday, April 25, 2013
QUASARS• aka ‘Active Galactic Nuclei’
• Light from the central region outshines the entire galaxy!
• Only way to power is by accretion of gas onto a black hole
• Using the ‘Eddington Limit’ can estimate that black holes at the centers of galaxies must be typically between 106 - 109 Msun
The M87 Jet
PRC00-20 • Space Telescope Science Institute • NASA and The Hubble Heritage Team (STScI/AURA)
A nearby Active Galactic Nucleus shoots a high-
speed jet of gas
Light from accretion disk
Thursday, April 25, 2013
STELLAR-MASS BLACK HOLES
• Can be formed in a supernova explosion at the end of a massive star’s life
• Often found in binary systems
• Black hole can accrete matter from the companion star!
Matter can be pulled from the companion star to the black hole
Thursday, April 25, 2013
NEUTRON STARS• Also can be formed in
supernovae
• About 1.5 Msun in 10 km radius
• average density > than atomic nuclei
• densest observable matter in Universe
• made mostly of neutrons, but may contain exotic matter at the center
Inne
r C
ore: ?
Out
erCore
: n, p
, e
Crus
t: nucle
i, n, e
Where ? could be: hyperon condensate, kaon condensate,
strange quark matter...........
Thursday, April 25, 2013
NEUTRON STARS
• Like stellar-mass black holes, can often be found in binary systems
• Can also accrete matter from the companion star
Accretion onto a neutron star
Thursday, April 25, 2013
OBSERVING ACCRETION ONTO COMPACT OBJECTS
• Gas accreting onto black holes and neutron stars gets extremely hot (millions of degrees)
• The gas therefore emits thermally in X-rays
An all-sky X-ray image: the brightest X-ray sources in the sky come from accretion onto black holes and neutron stars
From MAXI onboard the ISS
Thursday, April 25, 2013
X-RAY TELESCOPES• X-rays do not penetrate the
Earth’s atmosphere, so have to go into space
• X-rays will pass through conventional optical telescope mirrors, so have to focus X-rays with special ‘grazing-incidence’ mirrors
• Major NASA and ESA missions are : Chandra and XMM-Newton
CHANDRA
XMM-NEWTON
Thursday, April 25, 2013
OBSERVING X-RAYSTHE
CHANDRA MIRRORS
Thursday, April 25, 2013
ACCRETION SUMMARY
• Accretion onto compacts objects is the ultimate power source in the Universe
• Prof. Cackett works on X-ray observations of accretion onto black holes and neutron stars to try and understand these objects
• Renee Ludlam will be working with Prof. Cackett this summer.
Thursday, April 25, 2013
Astrophysics Summary• Plenty of work to do. Last 2 years 6 projects.• Zaven Bush (galaxy vs. CCSN)• Johanna-Laina Fischer (new parameters in
SNIa light curves), Levente Dojcsak(new fitting model to SNIa light curves-led to a paper) at FNAL with John Marriner.
• Brett Sandler to SLAC worked with Rafe Schindler on IR Camera for DES.
• Rachael Merritt SN Host vs Field Galaxies, Aron Zell accretion in NS, Meridith Joyce on resolution of DES camera
Thursday, April 25, 2013