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LINE PROFILES & WAVELENGTHS ACROSS STELLAR SURFACES LINE PROFILES & WAVELENGTHS ACROSS STELLAR SURFACES

LINE PROFILES & WAVELENGTHS ACROSS STELLAR SURFACES - PowerPoint Presentation

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LINE PROFILES & WAVELENGTHS ACROSS STELLAR SURFACES - PPT Presentation

Dainis Dravins Lund Observatory Sweden wwwastroluse dainis KVA Towards the science case for EELT HIRES Cambridge UK September 2012 STELLAR SURFACES where starlight and stellar spectra originate ID: 546125

stellar line lines shifts line stellar shifts lines wavelength lund observatory solar amp dainis profiles hydrodynamic models heidelberg originate

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Slide1

LINE PROFILES & WAVELENGTHS ACROSS STELLAR SURFACES

Dainis

Dravins

– Lund

Observatory

, Sweden

www.astro.lu.se

/~

dainis

KVA

Towards the science case for E-ELT

HIRES

, Cambridge UK, September 2012Slide2

STELLAR SURFACES… where starlight and stellar spectra originate

Simulations feasible for widely different stars

But … any precise physical conclusion

depends on the reliability of modeling

(

metallicity

, magnetic activity,

gravitational redshift, center-to-limb wavelength changes).

How does one verify/falsify 3-D simulations

(except for the spatially resolved Sun) ?

High-resolution spectroscopy acrossspatially resolved stellar disks !Granulation on a 12,000 K white dwarf (top) and a 3,800 K red giant. Areas differ by enormous factors: 7x7 km2 for the white dwarf, and 23x23 RSun2 for the giant.

(H.-G. Ludwig, Heidelberg)Slide3

LINE PROFILES FROM 3-D HYDRODYNAMIC SIMULATIONS

Model predictions insensitive to modest spatial smearing

(Models by Hans-Günter Ludwig,

Landessternwarte

Heidelberg

)

Spatially averagedline profiles from20 timesteps, andtemporal averages.

 = 620 nm = 3 eV5 line strengthsGIANT STAR

Teff= 5000 Klog g [cgs] = 2.5(approx. K0 III)

Stellar disk center;µ = cos  = 1.0Slide4

Figure by

Hiva

Pazira (Lund Observatory)

(1) Spatially

resolved spectroscopy with

E-ELT

Requires adaptive optics with integral-field unit

Left:

Hydrodynamic

simulation of the supergiant Betelgeuse (B.Freytag

)Right: Betelgeuse imaged with ESO’s 8.2 m VLT (Kervella et al., A&A, 504, 115)Top right: 40-m E-ELT diffraction limits at 550 nm & 1.04 μm.Slide5

(2) Selecting portions of stellar disk during exoplanet transits

Requires very high S/N in high-resolution spectrometers

Figure by

Hiva

Pazira

(Lund Observatory)Slide6

WAVELENGTH SHIFTS OF INTERGALACTIC ABSORPTION LINES

Dainis

Dravins

– Lund

Observatory

, Sweden

www.astro.lu.se

/~

dainis

KVA

Towards the science case for E-ELT

HIRES

, Cambridge UK, September 2012

HIRES quasar spectrum (

A.S.Cowie

,

Univ.of

Hawaii)Slide7

WHENEVER SPECTRAL LINES DO NOT ORIGINATE IN ISOTROPIC TURBULENCE, WAVELENGTH SHIFTS RESULT

SOLAR MODEL

Synthetic line profiles showing convective wavelength shifts originating in granulation

 = 620

nm; 

= 1, 3, 5

eV; 5 line strengths

Teff= 5700 K; log g [

cgs] = 4.4; G2 V

Solar disk center; µ = cos  = 1.0

(Models by Hans-Günter Ludwig, Landessternwarte Heidelberg) Observed solar granulation (Swedish Solar Telescope on La Palma; G.Scharmer

& M.G.Löfdahl

)Slide8

WHENEVER SPECTRAL LINES DO NOT ORIGINATE IN ISOTROPIC TURBULENCE, WAVELENGTH SHIFTS RESULT

… AND THE SAME MUST APPLY TO ALSO INTERGALACTIC CONVECTION, DRIVEN BY HEATING BY

AGNs

NEAR CLUSTER CENTERS

(

Even if

timescales

might be 100 Myr,

rather than solar 10

minutes)

Perseus cluster core in X-rays (Chandra), overlaid with Hα (WYIN). Arc-shaped H

α filaments suggest vortex-like

flows.

Density slices

at

three

times. Viscosity

stabilizes the bubble, allowing a flattened buoyant “cap” to form

. X-ray

brightness and inferred velocity field in Per-A can be reproduced

.

(Reynolds et al.: Buoyant radio-lobes in a viscous

intracluster

medium, MNRAS

357

, 242, 2005

)Slide9

INTERGALACTIC LINE ASYMMETRIES AND SHIFTS:

Plausible amount: 1

% of “general” line broadening

= 0.5 –

1 km/s

?

Mapping 3-D structure from different shifts in different lines

!

Need line synthesis from 3-D hydrodynamic models

!Lines closer to cluster centers gravitationally more

redshiftedMapping depth structure from multiple line components ?Probably useful to have resolving power approaching 1,000,000 ??Resolving lateral structure from secular time changes ???

ANALOGIES

AND

DIFFERENCES

TO

STELLAR

CONVECTION

: