ChromoAstrology: What stars can tell us about chromospheres, or whatever T. R. Ayres (CASA)

Slides:



Advertisements
Similar presentations
Star Types and luminosity Do not write what is in yellow
Advertisements

UV Ceti Stars Jessica Windschitl Atmospheres Spring 2007.
Chapter 8 The Sun – Our Star.
The K Stars: Orange Giants & Brighter Dwarfs Presentation by Paramita Barai Astr 8600, Stellar Spectroscopy.
Supernova. Explosions Stars may explode cataclysmically. –Large energy release (10 3 – 10 6 L  ) –Short time period (few days) These explosions used.
The Sun’s Dynamic Atmosphere Lecture 15. Guiding Questions 1.What is the temperature and density structure of the Sun’s atmosphere? Does the atmosphere.
General Properties Absolute visual magnitude M V = 4.83 Central temperature = 15 million 0 K X = 0.73, Y = 0.25, Z = 0.02 Initial abundances: Age: ~ 4.52.
Stars Stars are very far away.
COOL STARS and ATOMIC PHYSICS Andrea Dupree Harvard-Smithsonian CfA 7 Aug High Accuracy Atomic Physics In Astronomy.
Chapter 6 Atoms and Starlight.
Nov. 6, 2008Thanks to Henrietta Leavitt Cepheid Multiplicity and Masses: Fundamental Parameters Nancy Remage Evans.
The Sun- Our Star. The Sun- Our Star Star Parts: core radiation zone convection zone photosphere chromosphere corona solar wind.
The Fainting of Alpha Centauri A, Resolved! T. R. Ayres (CASA), and friends.
The spectral resolution of x-ray telescopes has improved many hundred-fold over the past decade, enabling us to detect and resolve emission lines in hot.
Physics 681: Solar Physics and Instrumentation – Lecture 24 Carsten Denker NJIT Physics Department Center for Solar–Terrestrial Research.
Stars Introduction To “Atomic Astrophysics and Spectroscopy” (AAS) Anil Pradhan and Sultana Nahar Cambridge University Press 2011 Details at:
Layers of the Solar Atmosphere Corona Chromosphere Photosphere Details of solar activity can be seen more easily in the hotter outer layers, which are.
Youtube: Secrets of a Dynamic Sun The Sun – Our Star
Note key, please leave in binder. Our Sun
Stellar Surface Structures
The Sun as a Star The “Surface” of the Sun and Its Structure Outer Layers – 3 distinct region Photosphere Chromosphere Corona.
Non-LTE in Stars The Sun Early-type stars Other spectral types.
Surveying the Stars Insert TCP 5e Chapter 15 Opener.
I. Stars A.The Brightness of Stars -Star: A hot glowing sphere of gas that produces energy by fusion. -Fusion: The joining of separate nuclei. Common.
ChromoAstrology: What the stars can tell us about chromospheres T. R. Ayres (CASA)
The Sun: Our Star The Sun is an ordinary star and shines the same way other stars of its type do. The bright part normally seen is called the photosphere,
The Sun By Jack. What is the sun? The sun is a star, it is the closest star to Earth and is the centre of our solar system. It is an average star, meaning.
The Sun ROBOTS Summer Solar Structure Core - the center of the Sun where nuclear fusion releases a large amount of heat energy and converts hydrogen.
Stellar Activity Chromospheric activity is defined as: –The variability of a chromosphere and/or corona –Spots (plage and dark spots) –Flares Associated.
Note that the following lectures include animations and PowerPoint effects such as fly-ins and transitions that require you to be in PowerPoint's Slide.
The Sun Photo from
Stars The apparent twinkling of the stars is a product of the turbulence and motion of the Earth’s atmosphere Stars have different colors depending on.
Simultaneous optical and X-ray observations of flares and rotational modulation on the RS CVn binary HR 1099 (V711 Tau) from the MUSICOS 1998 campaign.
 The sun lies at the heart of the solar system, where it is by far the largest object. (1)It holds 99.8 percent of the solar system's mass and is (2)roughly.
The Sun – El Sol – Die Sonne ESPS- Palmer High School.
Visible Image of the Sun The Sun The Sun Our sole source of light and heat in the solar system A very common star: a glowing ball of gas held together.
Solar Wind and Coronal Mass Ejections
The Sun.
THE SUN. The Sun The sun has a diameter of 900,000 miles (>100 Earths could fit across it) >1 million Earths could fit inside it. The sun is composed.
The Sun Stellar Evolution: Low Mass Stars White Dwarfs
STARS There are billions of stars in our galaxy and each one is a little different than the others! This unit teaches us the physical properties of stars.
Stellar Activity Chromospheric activity is defined as: –The variability of a chromosphere and/or corona –Spots (plage and dark spots) –Flares Associated.
Chandra X-Ray Spectroscopy of DoAr 21: The Youngest PMS Star with a High-Resolution Grating Spectrum The High Energy Grating Spectrum of DoAr 21, binned.
Stellar Activity in the Kepler Era Tom Ayres (CASA)
Spectral Signature of Emergent Magnetic Flux D1 神尾 精 Solar Seminar Balasubramaniam,K.S., 2001, ApJ, 557, 366. Chae, J. et al., 2000, ApJ, 528,
1. active prominences - solar prominences that change in a matter of hours.
The Sun – Our Star Our sun is considered an “average” star and is one of the 100 BILLION stars that make up the Milky Way galaxy. But by no MEANS does.
Transition Region Heating and Structure in M Dwarfs: from Low Mass to Very Low Mass Stars Rachel Osten Hubble Fellow University of Maryland/NASA GSFC In.
The Magnetic Sun. What is the Sun? The Sun is a Star, but seen close-up. The Stars are other Suns but very far away.
Galaxies The basic structural unit of matter in the universe is the galaxy A galaxy is a collection of billions of _____________, gas, and dust held together.
The Sun, our favorite star!
Lecture 8 Optical depth.
The Sun – El Sol – Die Sonne ESPS- Palmer High School.
Part 6:The Sun Photo from
A105 Stars and Galaxies  Homework 6 due today  Next Week: Rooftop Session on Oct. 11 at 9 PM  Reading: 54.4, 55, 56.1, 57.3, 58, 59 Today’s APODAPOD.
Universe Tenth Edition Chapter 16 Our Star, the Sun Roger Freedman Robert Geller William Kaufmann III.
Copyright © 2012 Pearson Education, Inc. Chapter 11 Surveying the Stars.
THE SUN, OUR NEAREST STAR STARS ARE FORMED IN GIANT CLOUDS OF DUST CALLED NEBULA.
The Sun Created by the Lunar and Planetary Institute For Educational Use Only LPI is not responsible for the ways in which this powerpoint may be used.
How the Sun Shines. The Luminosities of Stars Stellar distances can be determined via parallax – the larger the distance, the smaller the parallax angle,
GOAL: To understand the physics of active region decay, and the Quiet Sun network APPROACH: Use physics-based numerical models to simulate the dynamic.
DAY 16 September 17, Agenda 1 st RP ‘Stuff’ back Grade Sheets Complete Star Notes Star Concept Map.
Stars and magnetic activity
The Sun as a Star The “Surface” of the Sun and Its Structure
Sun: General Properties
The Sun is the largest object in the solar system.
Questions 1 – 24: Due Wednesday, February 29, 5:00 pm.
Properties of the Sun Visual Vocabulary.
Atmospheres of Cool Stars
Presentation transcript:

ChromoAstrology: What stars can tell us about chromospheres, or whatever T. R. Ayres (CASA)

Chromospheres XXXXXXXXX

Sun Star.

one Sun many Stars

<- p-a heating mech??? Cartoon of solar chromosphere has complexified over past two decades (K. Schrijver + B. DePontieu), but stellar view still is very much 1D

Coronal heating by accreting pineapples??!!

Outline H-R Diagram Wilson- Bappu Effect Rotation-Age-Activity Connections Activity Cycles Flux-Flux Correlations Atmospheric Dynamics (super new!) Buried Coronae Guiding questions: What can unresolved stellar chromospheres tell us about the solar counterpart? Is Sun ‘normal’ in cosmic scheme of things?

Chromospheric H-R Diagram Chromospheres appear to be confined to ‘cool stars’, in convective half of H-R diagram Coronae are seen at earlier types, but ‘ionization thermostat’ that inspires chromospheres dies out at same place convection fails Not a coincidence! Originally thought to signal lack of acoustic energy, but dynamo needs convection too

Wilson-Bappu Effect: Barometer or Tachometer? Mg I + Mg II resonance lines in early-G supergiant  Camelopardalis (deep core absorptions are ISM) (from STIS ‘StarCAT’)

Average Mg II k-line profiles from active & quiet G-type dwarfs. FWHMs are same, despite very different core fluxes

Average Mg I profiles: active dwarfs have higher wing intensities; lineshapes are similar to Ca II H & K in L-A G stars

Mg II h & k line wings also higher in active dwarfs. Similar behavior seen in Ca II H & K of plage vs. quiet-Sun

Left : k lines of G-type giant supergiant solar twin (  Cen A) Right : scaled profiles k line widens dramatically with increasing luminosity (W- B Effect) For dwarfs, FWHM is ~100 km/s, already beyond any plausible Doppler broadening

Like h & k cores, Mg II damping wings broaden with increasing luminosity: important clue to physical origin of W-B Effect (Same behavior is seen in Ca II H & K)

Mg I in G giant supergiant solar twin Now, Mg I cores (and wings) do not broaden with luminosity (although some photospheric absorptions do)

WBE = Barometer !!! W-B Effect owes its existence to decreasing mean density but increasing thickness of chromospheres with decreasing gravity, partly a consequence of H - opacity, a P 2 species (whereas Ca + and Mg + are P 1 and Mg 0 is P 2 ), but equally important is radiative cooling by metals and H, which depends on electron density through collisions (also P 2 ). Electrons provide ‘thermostat’ via partial ionization of hydrogen: n e /n H increases 10 4 x over K, accounting for great thickness of chromosphere, at nearly const T. Wings and outer emission edges of Mg II lines form outside Doppler core and thus can directly reflect changes in chromospheric column mass with gravity

Rotation-Age-Activity Connection ’Skumanich laws’ confirm importance of dynamo, creating high levels of activity in fast rotating stars, but also root of magnetic braking, which ultimately quenches activity. Recent issues: ‘saturation’ at high spin rates; ‘basal’ emissions at low end (‘little [  2 ] dynamo’, waves & shocks)

Stellar Activity Cycles Long term Ca II emissions of nearby field star closely mimic Sun’s cycle. Visible brightness changes of Sun only few milli- mags, yet 10x larger than entire chromospheric energy budget (Radick, Lockwood, Skiff, & Baliunas 1998)

Most late-type stars of near-solar color show long term variations in Ca II emission, many cyclic. Others, typically low R HK and often subgiants, are ‘flat activity’ (Radick et al. 1998)

Solar variations on long (and short) timescales fall close to stars of similar activity (Radick et al. ’98; Lockwood et al. 2007)

Case Study: Cycles of Alpha Cen Alpha Centauri triple system. Two solar-like stars about 20 au apart (Sun-Uranus); dim red dwarf 10,000 au away Slightly metal rich compared with Sun, slightly older by ~1 Gyr. G2V primary ( “A” ) is near twin of our own star

Alpha Cen X-rays first detected by HEAO-I ; binary later resolved by Einstein. Surprising result: little Alpha Cen B twice as X-ray luminous as big A ROSAT carried out long term coronal campaign in 1990’s

XMM (0.2-2 keV): a Cen A visible in first few frames; disappears by mid-2004 (Robrade+ 2005) Note: Secondary also fading

The `Fainting’ of Alpha Cen A Solar physicist frets over stunning 50x drop of Sun’s twin in soft X-rays Is Sun’s cycle depth (only ~5x in keV band) somehow abnormal in coronal scheme of things?

Fe XII 195 (1 MK) coronal emission persists at spot minimum (left ; max at right). ‘Fuzzy ball’ devolves from magnetic carpet: small clumps of flux built by local dynamo, independent of deep seated el jefe dynamo responsible for sunspots and their decadal cycling

Since ‘00 Alpha Cen orbital separation closing rapidly: no longer easily resolvable by XMM, still trivial for Chandra. HRC campaign (since Oct ‘05) *surprisingly* captures both stars

2007 Chandra LETGS spectrum shows strikingly different A than 7 yrs earlier: hard emissions gone, but key Fe IX & X (dominating energy losses) unchanged (actually, stronger)

High-energy Yohkoh imaging, : 2-3 MK emission almost exclusively from active regions

Cycles Summary Stellar HK activity cycles solar- like in amplitude & duration; flat activity stars common; long term cycles at low activity give way to stochastic behavior at high, dominated by rotational modulations. At low end, long term photometric changes positively correlated with Ca II; opposite is true at high activity Lesson of a Cen A: Appearance of X-ray cycles very dependent on energy bands & instrumental responses, especially for soft sources like Sun where bulk of coronal emission is >5 nm

Flux-Flux Correlations Coronal X-rays show good correlation with TZ C IV (except for ‘X-ray deficient stars’); Mg II & C IV well correlated for all types

Chromosphere and ‘Transition Zone’ show better correlations with each other than either does with the corona Oddballs (X-ray deficient Hertzsprung gap stars, ‘noncoronal’ red giants) where Mg II–C IV appears normal, but X- rays are anomalous Correlation power laws nonlinear, steeper than unity: increasing activity not just filling factor effect -- new heating sources must come into play

Chromospheric Dynamics Recent FUV HST/COS study of 50 Myr solar analog EK Draconis (  Cen A [shaded] reference solar twin). Note bright Fe XXI emission, and very broad chromospheric (C II) and transition zone lines (Si IV), the latter significantly redshifted.

EK Draconis displays two FUV flares during mere 20 min observation; Si IV affected greatly, Fe XXI not so much, and C II hardly at all.

Upper: EK Dra (Si IV 1393 left, 1402 center) Lower: Alpha Cen A; double Gaussian fits indicate multiple dynamical components; EK lines are strongly redshifted (warm coronal rain?).

ChromoDynamics TZ line shapes of EK Dra are remarkable Basic profile consists of redshifted narrow component; and even more redshifted broad component, with about equal flux ratio (like Alpha Cen A, curiously) Emphasizes prevalence of ‘relentless’ kinematic processes shaping upper chromospheres: perhaps analogous to TZ explosive events but not clear…

Buried Coronae ‘Noncoronal’ red giants thought to completely lack X-rays (post-MS expansion = ultra-slow spin = no dynamo), until archetype (Arcturus) finally dug out of ‘coronal graveyard’ by Chandra, albeit at pathetically low L X

FUV ‘hot lines’ also detected in several graveyard giants by HST, but Si IV looked odd, and N V doublet was weak or missing. Distorted Si IV explained by blends with fluoresced H 2 lines. Curiously, de-blended profiles similar to legitimate coronal giants

Finally, recognized that Si IV emitting gas selectively absorbed by overlying cooler material. N V clobbered by C I absorptions near b-f edge. X-rays would be attenuated by chromospheric atomic H and He Coronae buried alive!

Conclusions Chromospheres are fundamental property of cool stars, doubtless because waves, shocks & magnetism are ubiquitous features of convective atmospheres Chromosphere adjusts electron density and thickness to balance mech heating Energy deposition can be highly dynamic Corona tightly coupled to chromosphere Sun appears perfectly ‘normal’ (for L-A * )

Final (provocative) Thoughts