European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Interferometric Observations of Supergiants: Direct Measures.

Slides:



Advertisements
Similar presentations
To measure the brightness distribution of galaxies, we must determine the surface brightness of the resolved galaxy. Surface brightness = magnitude within.
Advertisements

7B Stars … how I wonder what you are.. 7B Goals Tie together some topics from earlier in the semester to learn about stars: How do we know how far away.
1. absolute brightness - the brightness a star would have if it were 10 parsecs from Earth.
Susan CartwrightOur Evolving Universe1 Understanding Stars n What do we know? n From observations of nearby stars: l l luminosity/absolute magnitude l.
Stars Flux and Luminosity Brightness of stars and the magnitude scale Absolute magnitude and luminosity Distance modulus Temperature vs heat Temperature.
Stellar Continua How do we measure stellar continua? How precisely can we measure them? What are the units? What can we learn from the continuum? –Temperature.
Stars Stars are very far away.
ECLIPSING BINARIES IN OPEN CLUSTERS John Southworth Dr Pierre Maxted Dr Barry Smalley Astrophysics Group Keele University.
S U S I Stellar Angular Diameters Determined with SUSI J. Davis, M.J. Ireland, A.P. Jacob, J.R. North, S.M. Owens, J.G. Robertson, W.J. Tango, P.G. Tuthill.
The HR Diagram Astronomy 315 Professor Lee Carkner Lecture 8.
HD REVISITED John Southworth Dr Pierre Maxted Dr Barry Smalley Astrophysics Group Keele University.
Wavelength flux Spectral energy distributions of bright stars can be used to derive effective temperatures Ay 123 Lecture I - Physical Properties.
Mass to light ratio of the Milky Way disc Chris Flynn, Johan Holmberg, Laura Portinari Tuorla Observatory Burkhard Fuchs, Hartmut Jahrei ß Burkhard Fuchs,
… how I wonder what you are.
Compilation of stellar fundamental parameters from literature : high quality observations + primary methods Calibration stars for astrophysical parametrization.
Guiding Questions How far away are the stars?
Clicker Question: The HR diagram is a plot of stellar A: mass vs diameter. B: luminosity vs temperature C: mass vs luminosity D: temperature vs diameter.
Properties of Main Sequence Stars Masses Luminosities Lifetimes Distribution.
Building the Hertzsprung-Russell (H-R) Diagram Use the worksheets passed out in class.
22 March 2005 AST 2010: Chapter 171 The Stars: A Celestial Census.
Question 1 Stellar parallax is used to measure the a) sizes of stars.
Properties of Stars. Distance Luminosity (intrinsic brightness) Temperature (at the surface) Radius Mass.
Chapter 12: Surveying the Stars
Chapter 11 Surveying the Stars Properties of Stars Our goals for learning: How do we measure stellar luminosities? How do we measure stellar temperatures?
The Nature of the Stars Chapter 19. Parallax.
Copyright © 2010 Pearson Education, Inc. Chapter 10 Measuring the Stars.
The Impact of Dust on a Stellar Wind-Blown Bubbles Ed Churchwell & John Everett University of Wisconsin Oct , 2008Lowell Observatory Flagstaff, AZ.
Surveying the Stars Insert TCP 5e Chapter 15 Opener.
Hertzsprung-Russell Diagram
Chapter 10 Measuring the Stars. Units of Chapter 10 The Solar Neighborhood Luminosity and Apparent Brightness Stellar Temperatures Stellar Sizes The Hertzsprung-Russell.
Model atmospheres for Red Giant Stars Bertrand Plez GRAAL, Université de Montpellier 2 RED GIANTS AS PROBES OF THE STRUCTURE AND EVOLUTION OF THE MILKY.
Measuring Radii and Temperatures of Stars Definitions (again…) Direct measurement of radii – Speckle – Interferometry – Occultations – Eclipsing binaries.
Measuring the Stars How big are stars? How far away are they?
JHK-band Spectro-Interferometry of T Cep with the IOTA Interferometer G. Weigelt, U. Beckmann, J. Berger, T. Bloecker, M.K. Brewer, K.-H. Hofmann, M. Lacasse,
Properties of Stars.
Stars. Astronomy The study of space How astronomers measure distance 1. Light years– The distance light travels in one year 9.461x km.
Physical properties. Review Question What are the three ways we have of determining a stars temperature?
Lecture Outlines Astronomy Today 8th Edition Chaisson/McMillan © 2014 Pearson Education, Inc. Chapter 17.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2.
Copyright © 2010 Pearson Education, Inc. Chapter 10 Measuring the Stars.
Stars Other Suns. Physical Properties Luminosity Mass Diameter (radius) Must know distance to find out these properties!
Stars Classifying stars: H-R diagram Vogt-Russell theorem Mass-luminosity relation Evolution on the HR diagram.
Solid Molecules Neutral Gas Ionized Gas (Plasma) Level of ionization also reveals a star’s temperature 10 K 10 2 K 10 3 K 10 4 K 10 5 K 10 6 K.
Comprehensive Stellar Population Models and the Disentanglement of Age and Metallicity Effects Guy Worthey 1994, ApJS, 95, 107.
The IMF of the Orion Nebula Cluster Across the H-burning Limit Nicola Da Rio HST Orion Treasury Science Meeting STScI, Baltimore, September 12 th 13 th.
Stellar Continua How do we measure stellar continua?
Astrophysics of Life : Stars. 2 Wave Characteristics: Wavelength - Distance between successive wave peaks Period – Time between passing wave peaks Frequency.
1 Stellar Properties Basic Data Mass and Radius Spectral Classification Photometric Systems.
CHARA Collaboration Year-Five Science Review Dynamite Diameters Tabetha Boyajian GSU/CHARA Presented by Hal McAlister.
Chapter 10 Measuring the Stars. Star Cluster NGC ,000 light-years away.
Measuring Radii and Temperatures of Stars Definitions (again…) Direct measurement of radii – Speckle – Interferometry – Occultations – Eclipsing binaries.
Copyright © 2010 Pearson Education, Inc. Lecture Outline Chapter 10 Measuring the Stars.
Binary stars and clusters Chapter 11. Review Properties of stars –apparent brightness (apparent magnitude) measure energy/area/second –luminosity (absolute.
Dynamite Diameters Observations of main sequence stars with long baseline optical/infrared interferometry Tabetha Boyajian (Georgia State University /
Chapter 11: Characterizing Stars
Measuring the Stars What properties of stars might you want to determine?
Chapter 11: Chapter 11: Characterizing Stars. How near is the closest star other than the Sun? How near is the closest star other than the Sun? Is the.
Chapter 11 Surveying the Stars. How do we measure stellar luminosities?
1 Stellar structure and evolution Dr. Philippe Stee Observatoire de la Côte d’Azur – CNRS Slides mainly from S. Smartt.
T HE GJ 436 AND 55 C NC S YSTEMS : D IRECT E XOPLANETARY D IAMETER AND F UNDAMENTAL S TELLAR P ARAMETERS Kaspar von Braun (NASA Exoplanet Science Institute.
Copyright © 2012 Pearson Education, Inc. Chapter 11 Surveying the Stars.
Properties of Stars. "There are countless suns and countless earths all rotating around their suns in exactly the same way as the seven planets of our.
Charles Hakes Fort Lewis College1. Charles Hakes Fort Lewis College2.
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.
The Family of Stars.
Unit 2: The Sun and Other Stars
Chapter 10 Measuring the Stars
Unit 2: The Sun and Other Stars
Star Classes Los Cumbres Observatory.
Unit 2: The Sun and Other Stars
Presentation transcript:

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Interferometric Observations of Supergiants: Direct Measures of the Very Largest Stars Gerard T. van Belle PRIMA Instrument Scientist European Southern Observatory April 7, 2008

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Interferometric Observations of Supergiants: Direct Measures of the Very Largest Stars Gerard T. van Belle PRIMA Instrument Scientist European Southern Observatory March 17, 2009

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Back of the Envelope Estimate: Supergiants  Guesstimates (things we think we know) :  Main sequence stars: 1 M , 1 R   Supergiant stars: : 10 M , 100 R   Stellar lifetime T goes as T ~ M -4  There are ×10 4 fewer supergiants than main sequence stars  Supergiants are ~10 4 times brighter: will be detectable at a distance 100× further than main sequence stars  A volume ×10 6 greater  Number of observable targets goes linearly with volume  Ergo, 10 2 more supergiants to observe at a given apparent size  Most main sequence stars 100 R , so things are even better than this estimate Supergiants are obvious targets for interferometers! 3

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Back of the Envelope Estimate: M-Dwarfs  Guesstimates (things we think we know) :  Solar-type stars: 1 M , 1 R   M-dwarfs stars: : 0.4 M , 0.4 R   Stellar lifetime T goes as T ~ M -4  There are ×40 more M-dwarfs than solar-type stars  M-dwarfs are ~100× fainter: will be resolvable at a distance 10× smaller than main sequence stars  A volume ×10 3 smaller  Number of observable targets goes linearly with volume  Ergo, 25× fewer M-dwarfs to observe at a given apparent size  Already difficult to resolve more massive main sequence stars (solar type) due to small size M-dwarfs are not obvious targets for interferometers! 4

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 5 Essential Astrophysics: The HR Diagram  Track/model stellar evolution  Fundamental stellar properties  Luminosity  Radius  Temperature  Examine properties of groups of stars  Clusters, associations

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project CHARA of Yesteryear: M-Dwarf Diameters Berger Chabrier & Baraffe (1997) models Seiss models

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Metallicity Dependency of Diameter Deviation? Berger Measured diameters versus Chabrier & Baraffe (1997) models

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 8  Direct observation of fundamental stellar parameters  Effective temperature is defined as: which can be rewritten as:  F BOL is the bolometric flux (W cm -2 ),  R is the Rosseland mean stellar angular diameter (mas)  Linear radius is simply:  Hipparcos (Perryman et al. 1997) distances now available  For those M-dwarfs that are resolvable, they tend to be bright enough to have Hipparcos distances  But many nearby stars are too dim for good distances Basic Parameters from Angular Diameters (  )

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 9 Nuances of F BOL Fitting  Stars are not blackbody radiators  Especially cool dwarfs: many features  Spectral type estimates  Heterogeneous sources? By type (objective prism, slit spectroscopy, etc.) or practitioner  Spectral type template  Empirical model (Pickles 1998) versus theoretical model (eg. Hauschildt’s NextGen models)  Photometry  Wide- and narrow-band can be used usefully  However, peak of flux curve at ~1μm for many M-dwarfs: most photometry here is quite poor  Reddening  Can be degenerate with spectral type estimate in doing SED fitting  Not a significant factor for M-dwarfs

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 10 Bolometric Flux Fitting

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 11 Bolometric Flux Fitting II.

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 12 Limb darkening  Stars are not uniform disks  Gaseous, not solid, sphere  End up looking ‘into’ the star  Good and bad  Have to account for this  Measuring this can be used to characterize internal structure of star  Direct probe of internal temperature structure  For M-dwarfs, a model atmosphere will provide a correction factor from UD to LD  Correct account of molecular features? (Here be dragons!) HST Image of  Ori - Betelgeuse

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 13 Limb darkening. II  Effects are less striking in the near- IR  Most of the effects are seen at the higher spatial frequencies  Acceptable to do a UD fit, and scale  Gives the size of the mean radiating surface  Corrections are ~2% for M-dwarfs  Scales with temperature  Cooler → LD/UD↑ A-type Star Model (Claret et al. 1995) Uniform disk Limb darkened disk

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project 14 Current Stock of Results  Borrowing from Davis (1997), increase of 145 to 340 stars in the literature (as of ~2003)  Notable improvement: Application of interferometry to evolved stars  Notable area for improvement: Still main sequence stars, particularly late-type, and supergiants  Homogenous, large datasets are absent from the literature for both Previous CHARA work : 6 Diameters This work: 11 (and counting)

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Effective Temperature versus V-K  Most straightforward quantity: T EFF  “All V-K is good for is estimates of T EFF ”  This is not necessarily a bad thing  A significantly more robust index than spectral type  Down to 3500K, curve seems fairly linear with V-K  At T EFF <3500K, curve seems to flatten out

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Effective Temperature versus V-K  Red points: PTI data  Seems to bear out trend down to 3500K  Highlights power of CHARA, though, with smallest stars  Low T EFF versus V- K curve ‘flattening’ seen before: Miras  For Miras, was explained in terms of MOLsphere

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Linear Radius versus V-K  Significant amounts of scatter seen as a function of V-K  eg. at V-K~4.0, factors of 2 × see in linear radius  As with T EFF, starting to see 2 nd order effects?  Age?  [Fe/H]?  Or just evidence that V-K poor proxy for R?

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Linear Radius versus V-K  Red points: PTI data  Some scatter as well (but not as much)  Different V-K regime

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Influence of [Fe/H] in Linear Radius?  Ranges from [Fe/H]=-1.5 (small bubble) to (big bubble)  Interesting low [Fe/H] outliers at V-K~4  Average value of  [Neglected to provide [Fe/H] for PTI data yet]

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Radius versus Mass  Mass from mass-M K relationship found in Delfosse+ (2000)  Green points: Berger+ (2006) CHARA  Blue: new CHARA  Red line: Chabrier & Baraffe (1997) model ([Fe/H]=0)  Region of interest: M   Convection peculiarities in models?  Missing from new data  Deviations due to spotting?

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Temperature versus Radius  More ‘robust’ and model-independent than measures of M, [Fe/H]  However, a bit of plotting θ vs. θ  F BOL data is the additional information  As with T EFF vs. V-K, linear trend down to 3500K(?) with ‘pedestal’ at <3500K?

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Temperature versus Radius  Red points: PTI data  <3500K ‘pedestal’: 2 nd order TEFF effects dominating?  Age, [Fe/H]?

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Temperature versus Radius: Relationship of Mass?  Mass effect in T vs R?  Bubble size a function of mass  M 

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Remember this Plot? Berger+ 2006

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project Things Look a Little Different  Difficult to reproduce  Nominally includes Berger data  How to derive ‘predicted’ R values from CB97?  M V →M BOL with BC(T EFF )→L →R(L)  Oh, and [Fe/H] values for M- dwarfs? All over the place

European Organization for Astronomical Research in the Southern Hemisphere VLTI PRIMA Project The ‘To-Do’ List  Further CHARA observations  In the ‘sweet spot’ of R={0.5,0.8} R , V- K={2.25,3.25}, M={0.4,0.6} M   Better precision?  Currently at σ θ / θ ~ 4.5%  Possible with repeating measures?  Better supporting information  [Fe/H]  Homogenous measures a plus  Broad-band photometry: R,I (z?) bands  F BOL errors reported at ~1%, but with χ ν 2 >>1  Chase after the new generation of models