White Dwarf Stars: Crystals and Clocks S.O. Kepler.

Slides:



Advertisements
Similar presentations
Lecture I: Introduction to White Dwarfs S. R. Kulkarni, E. Ofek
Advertisements

Stellar Evolution.
Barbara G. Castanheira S. O. Kepler, D. Winget, J.J. Hermes, K. Bell, … University of Texas at Austin McDonald Observatory.
Marek Biesiada Department of Astrophysics and Cosmology University of Silesia Katowice, Poland 2 nd Vienna Central European Seminar on Particle Physics.
Introduction to Astrophysics Ronald L. Westra Department Mathematics Maastricht University.
Astronomy and the Electromagnetic Spectrum
Copyright © 2010 Pearson Education, Inc. Chapter 16 Galaxies and Dark Matter.
Neutron Stars and Black Holes
Supernova. Explosions Stars may explode cataclysmically. –Large energy release (10 3 – 10 6 L  ) –Short time period (few days) These explosions used.
LECTURE 20, NOVEMBER 9, 2010 ASTR 101, SECTION 3 INSTRUCTOR, JACK BRANDT 1ASTR 101-3, FALL 2010.
The Lives of Stars Chapter 12. Life on Main-Sequence Zero-Age Main Sequence (ZAMS) –main sequence location where stars are born Bottom/left edge of main.
Supernova and Neutron Stars
Astro 201: Sept. 30, 2010 Pick up Midterm #1 from piles along the wall. Correct answers are printed on the scantrons, I will post keys also and correct.
Neutron stars - Chapter Neutron stars The remains of cores of some massive stars that have become supernovae. Cores are a degenerate gas of mostly.
The Milky Way PHYS390 Astrophysics Professor Lee Carkner Lecture 19.
Chapter 23: Our Galaxy Our location in the galaxy Structure of the galaxy Dark matter Spiral arm formation Our own supermassive black hole.
Solar Systems & Night Sky Galaxies Cosmology Tools, Laws & Methods The Sun & Other.
Extra-Solar Planets Astronomy 311 Professor Lee Carkner Lecture 24.
A1143 – Q3 Grade Distribution: Curve +1%. Back to the Beginning: Big Bang Misnomer! Expansion not explosion No center or edges: isotropic and homogeneous.
Distances. Parallax Near objects appear to move more than far objects against a distant horizon. Trigonometric parallax is used to measure distance to.
Question 1 Stellar parallax is used to measure the a) sizes of stars.
9B The Milky Way Our Galactic Home. 9B 9B Goals Structure of our Galaxy. Its size and shape. How do stars and things move through it? Mass and Dark Matter.
The Milky Way Center, Shape Globular cluster system
The Milky Way. Structure of the Milky Way The Milky Way.
Quiz 1 Each quiz sheet has a different 5-digit symmetric number which must be filled in (as shown on the transparency, but NOT the same one!!!!!) Please.
Down the rabbit hole Large objects in space and the big bang theory.
Chapter 11 Surveying The Stars Surveying The Stars.
The Grouping of Stars in the H-R Diagram The Major Categories of Stars 1.The Main Sequence, 2.The Supergiants, 3.The Giants, 4.The White Dwarfs. Main Sequence.
Stellar Atmospheres: Motivation 1 Stellar Atmospheres: Literature Dimitri Mihalas –Stellar Atmospheres, W.H. Freeman, San Francisco Albrecht Unsöld –Physik.
Overview of Astronomy AST 200. Astronomy Nature designs the Experiment Nature designs the Experiment Tools Tools 1) Imaging 2) Spectroscopy 3) Computational.
Do black holes really exist? Dr Marek Kukula, Royal Observatory Greenwich.
Galaxies Read Your Textbook: Foundations of Astronomy
The Evolution of the Universe Nicola Loaring. The Big Bang According to scientists the Universe began ~15 billion years ago in a hot Big Bang. At creation.
Fusion, Explosions, and the Search for Supernova Remnants Crystal Brogan (NRAO)
Galaxies Chapter 16. Topics Types of galaxies Dark Matter Distances to galaxies Speed of galaxies Expansion of the universe and Hubble’s law.
STARS By Bodin Lay. Types of Stars Main Sequence Stars - The main sequence is the point in a star's evolution during which it maintains a stable nuclear.
Stellar Evolution. Consider a cloud of cold (50 deg K) atomic hydrogen gas. If an electron of one atom flips its spin state and the electron then has.
Mean period of pulsating white dwarfs as a spectroscopy-independent thermometer Anjum S. Mukadam, University of Washington Collaborators: M. H. Montgomery.
The Nature of Galaxies Chapter 17. Other Galaxies External to Milky Way –established by Edwin Hubble –used Cepheid variables to measure distance M31 (Andromeda.
The Stars Chapter 14 Great Idea: The Sun and other stars use nuclear fusion reactions to convert mass into energy. Eventually, when a star’s nuclear fuel.
Astronomy 340 Fall December 2005 Class #27.
© Sierra College Astronomy Department 1 Astronomy 10 Elementary Astronomy COURSE GOALS & OBJECTIVES.
Warm up The sun is 4.6 billion years old – how can it continue to produce so much heat and light?
Beata Malec University of Silesia XXXIII International Conference of Theoretical Physics MATTER TO THE DEEPEST: Recent Developments in Physics of Fundamental.
Anthropology Series In the Beginning How did the Universe begin? Don’t know!
Death of Stars II Physics 113 Goderya Chapter(s): 14
Earth & Space Science March 2015
Binary Orbits. Orbits Binary Stellar Systems 1/3 to 2/3 of stars in binary systems Rotate around center of mass (barycenter) Period - days to years for.
Copyright © 2010 Pearson Education, Inc. Clicker Questions Chapter 14 The Milky Way Galaxy.
I.Death of Stars White Dwarfs Neutron Stars Black Holes II.Cycle of Birth and Death of Stars (borrowed in part from Ch. 14) Outline of Chapter 13 Death.
Astronomy 1143 – Spring 2014 Lecture 21: The Evidence for Dark Matter.
1 The Stars Great Idea: The Sun and other stars use nuclear fusion reactions to convert mass into energy. Eventually, when a star’s nuclear fuel is depleted,
Galaxies: Our Galaxy: the Milky Way. . The Structure of the Milky Way Galactic Plane Galactic Center The actual structure of our Milky Way is very hard.
Chapter 25 Galaxies and Dark Matter. 25.1Dark Matter in the Universe 25.2Galaxy Collisions 25.3Galaxy Formation and Evolution 25.4Black Holes in Galaxies.
The Mass of the Galaxy Can be determined using Kepler’s 3 rd Law –Solar System: the orbital velocities of planets determined by mass of Sun –Galaxy: orbital.
Astronomy: A Beginner’s Guide to the Universe Seventh Edition © 2013 Pearson Education, Inc. Neutron Stars and Black Holes Chapter 13 Clickers.
Chapter 13 Post Main Sequence Stellar Evolution. The Sun.
When a star dies…. Introduction What are compact objects? –White dwarf, neutron stars & black holes Why study? –Because it’s fun! –Test of physics in.
“Globular” Clusters: M15: A globular cluster containing about 1 million (old) stars. distance = 10,000 pc radius  25 pc “turn-off age”  12 billion years.
Measuring the Stars How big are stars? How far away are they? How bright are they? How hot? How old, and how long do they live? What is their chemical.
Exploring the Universe with White Dwarf Stars: the First Year of the Freshman Research Initiative Astronomy Stream D. E. Winget, M. H. Montgomery, A. Allen,
Stellar Evolution Chapters 16, 17 & 18.
The lifecycles of stars
Evolution of the Solar System
Galaxies.
Galaxies Chapter 16.
ASTEROSEISMOLOGY OF LATE STAGES OF STELLAR EVOLUTION
The lifecycles of stars
The Link Between Underluminous Supernovae Explosions, Gravitational Waves and Extremely Low Mass White Dwarfs Alex Gianninas Mukremin Kilic, Warren Brown,
Presentation transcript:

White Dwarf Stars: Crystals and Clocks S.O. Kepler

White Dwarf Stars as Laboratories S.O. Kepler Department of Astronomy UFRGS - Brazil

Stellar Evolution Mass < 10 M sun : White Dwarf 10 M sun < Mass < 25 M sun : Neutron Star 10 M sun < Mass < 25 M sun : Neutron Star Mass > 25 M sun : Black Hole

Planetary Nebula Observed by the Hubble Space Telescope

Sirius and the White Dwarf Sírius B

White dwarfs pulsate as they cool

Intensity Changes With Time Multiperiodic, P=71s to 1500s, amp=4 mma to 300 mma

Pulsating White Dwarfs n Internal structure of the white dwarf (SNIa progenitors) (SNIa progenitors) n Cooling timescale n Age of the oldest stars in our galaxy High energy and high density physics High energy and high density physics

Pulsating White Dwarfs n White Dwarfs ~ 6000 (doubled in 2004) n Variable~ 115 (tripled in 2004) n DOV T eff = K 10 known, M= -1 n DBV T eff = K 13 know, M= 8 13 know, M= 8 n DAV T eff = K 92 known, M=12 92 known, M=12 Structure – SNIa progenitors

Pulsations … Seismology

Pulsations/Seismology: Y 10 e Y 11

Pulsations are global

Observations: 1.6 m telescope Laboratório Nacional de Astrofísica Brasópolis, MG

Whole Earth Telescope

Mass determination n UV spectra n Optical spectra n T ef = K n Massa = 1,1 M sol 0,6 M Sol

Mass distribution 300 stars PG survey

SDSS We fit all 1872 DA white dwarfs in SDSS

SDSS T eff determination

SDSS log g determination

Transição de fase para cristal A parte pontilhada corresponde a P(líquido quântico)/P(gás ideal) > 1. Efeitos quânticos iônicos são importantes à direita desta linha (  1975

DAV instability strip Need high S/N spectra of variables and non-variables to refine Teff and log g Need to find more variables and non-variables to determine log g dependence

Most Massive Pulsating WD

BPM37093 – Diamond in the Sky! 10’ 2 o = 12 x 10’ 17 light yr distant (40 quadrillion km)

Light Curve

Crystallization O C

Pulsations Present

Period in seconds

Phase Diagram

Crystallized or not?

BPM37093 in 1999

Super-Diamond? n Diamond n C crystal n FCC n 3,08A between atoms n 2 shared electrons n T < 8000 K n 10 K atm < P < 1,2x10 8 atm n BPM37093 n C crystal n BCC n 0,01A between nucleons n all electrons are free (degenerate) n T = 7 million K n P = 5x10 18 atm  = 36 Ton/cm 3  = 36 Ton/cm 3 n E ions > 2kT (quantized) n metallic quantum crystal o o

DBV instability strip Bárbara Castanheira - IUE

DBV GD 358

181 periodicities detected n Mass of each layer n M(R): Luminosity -> distance (1/10 uncertainty of parallax) (1/10 uncertainty of parallax) n Rotation law(r) [splitting (k)] n Magnetic field limit (6000 G) n 6 th order harmonics and combinations

Nuclear reaction rate Quantity of 22 Ne dependes mainly onQuantity of 22 Ne dependes mainly on  [C 12  16  Ne 20  Mg 24  ] NonResonantReaction T > 10 8 K and   g/cm 3 Uncertainty is around 50%!

C(  )O S 300

Mode identification with HST Chromatic amplitude changes

GD358 mode identification HST n Bárbara Castanheira l = 1 for k=8 and 9 in 1996 l = 1 for k=8 and 9 in 1996 probably l = 1 for other modes in 2000 probably l = 1 for other modes in 2000

GD358 mode identification HST n Bárbara Castanheira l = 1 for k=8 and 9 in 1996 l = 1 for k=8 and 9 in 1996 probably l = 1 for other modes in 2000 probably l = 1 for other modes in 2000

PNNV – DOV instalibility strip

Period (sec) PG

Frequency (  Hz) All PG

PG : 101 pulsations detected n T eff = K n Total mass : ( / ) M Sun n M(R): Luminosity -> distance n Mass of external layers n no harmonics or linear combination (no convection zone) (no convection zone)

PG modes detected k=   P=21.43s M= M Sun J. Edu S. Costa

Direct Method dP/dt Period (s ) P=516s dP/dt=( )x s/s

But period increases with time! dP/dt=( ) x 10 –11 s/s 1s/300 years

Most stable optical clock known

DAV

G117-B15A 2004 P=215s

Stable? Time scale = 2.2 Gyr Pulsars with dP/dt = s/s have timescale 0.1 Gyr, but PSR B , with P=5.3 ms and dP/dt=1.8x s/s has timescale of 9.5 Gyr.

Axions m ax cos2  < 4 meV E vacuum >2,5GeV &

Axions m ax > 1  eV or  ax > 1 tan  ratio of the vacuum energy of the two Higgs fields

Gravitons? Biesada & Malec (2002) Phys Rev D, 65 dP/dt: the string mass scale M s > 14,3 TeV/c 2 for 6 dimensions for Kaluza-Klein gravitons. The limit is negligible for higher dimensions

Variable G? Asteroseismological bound on G/G from pulsating white dwarfs Omar G. Benvenuto, Enrique García-Berro, and Jordi Isern PHYSICAL REVIEW D 69, (2004).

Why do pulsation periods change? R = 9,6 x 10 8 cm, dR/dt = 1 cm/yr T nucleus =12 million K, dT/dt = 0.05 K/year DAV Cooling dominates!

Photon vs neutrino emission

The Feynman diagram

Plasma neutrino (Weak interaction)

Two keys… n To excite the plasmon we must have n The plasma frequency is much higher for a degenerate gas, and increases with increasing density…

Effects of Neutrinos on Evolutionary Timescales EC GD 358

DBVs: dP/dt and Plasmon Neutrinos: 3-4!

Luminosity Function and Age of the Galaxy Age of the disk:  ± 2 yr Number of Stars Intensity

Age of the Universe Age = (11,5 ± 2,7) billion years Age of Universe = Age of disk + Halo + Formation of galaxy Age of disk + Halo + Formation of galaxy 9 ± 2 1,5 ± 1,5 1 ± 1 billion yr

HST: Galaxies formed 1 Gyr after Big-Bang

White dwarfs in globular cluster M – 8 days of exposure with HST Age= Gyr Age= Gyr Disk corrected we will do other globulars with SOAR

Age of the Universe in 2004 CMB - WMAP = ( ) GyrCMB - WMAP = ( ) Gyr Hubble constant: 1/H = (12 + 1) GyrHubble constant: 1/H = (12 + 1) Gyr Globular clusters: ( ) GyrGlobular clusters: ( ) Gyr Radiactive decay: ( ) GyrRadiactive decay: ( ) Gyr Cooling of white dwarf stars: ( ) GyrCooling of white dwarf stars: ( ) Gyr Distances to SNIa: (0.63/h)Gyr, Distances to SNIa: (0.63/h)Gyr,  10 years ago only white dwarfs gave age smaller than 15 billion years: smaller than 15 billion years: SN1987A NGC6903CenA SNIa

Spectra of DA, DB and DO

Mode identification with SOAR

Find more variables Frequency (Hz) Fractional Amplitude P=647s; A=48mma (V=18.6) P=329s; A=22mma

Detection of extra-solar planets Spectroscopy: detection of radial velocity variation around the center of mass

G117-B15A 2004 P=215s

Jupiter around G117-B15A? P=11.86 years, a=5.2 UA

Saturn around? P=29.46 years, a=9.5 UA

Search for planetary companions monitoring changes in pulse arrival time due to motion of star around barycenter. Orbit around center of mass with planetary companion

Detection Limits on Orbits of the Planets Doppler Sectroscopic Method (Current Limits) Pulsating White Dwarf Method (Current Limits)

Region of Planet Detection Quantitative Theoretical Limits of Stability? Time Squared

PMT CCD vs PMT

Measured Amplitude Difference

Change in Amplitudes

Amplitude vs Wavelength

CCD Data Analysis

That’s all folks!

Music?