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Asteroseismology A new revolution with the Kepler and TESS space missions Emeritus Professor Donald Kurtz Jeremiah Horrocks Institute University of Central Lancashire

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Page 1: Jeremiah Horrocks Institute University of Central

Asteroseismology

A new revolution with the Kepler and TESS

space missions

Emeritus Professor Donald Kurtz Jeremiah Horrocks Institute

University of Central Lancashire

Page 2: Jeremiah Horrocks Institute University of Central

At first sight it would seem that the deep interior of the Sun and stars

is less accessible to scientific investigation

than any other region of the universe.

1926

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1926

Our telescopes may probe farther and farther

into the depths of space; but how can we ever obtain

certain knowledge of that which is hidden

behind substantial barriers?

Page 4: Jeremiah Horrocks Institute University of Central

1926

What appliance can pierce through

the outer layers of a star and test

the conditions within?

Page 5: Jeremiah Horrocks Institute University of Central

Asteroseismology

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The Kepler Mission Space Telescope

Main mission: March 2009 – May 2013K2: May 2013 – October 30 2018

Page 8: Jeremiah Horrocks Institute University of Central

TESS2018

Page 9: Jeremiah Horrocks Institute University of Central

7 days of Kepler data for one of ~200,000 starsKIC10799291

The light curve

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Radial modesCepheidsP1/P0= 0.7

organ pipeP1/P0= 0.33

Page 11: Jeremiah Horrocks Institute University of Central

Structure of stellar pulsation modes

• n = number of radial nodes

• l = total number of surface nodes

• m = number of surface nodes that are lines of longitude

• l – m = number of surface nodes that are lines of latitude

 

Ylm q,j( ) = Nl

mPlm cosq( )eimj

Page 12: Jeremiah Horrocks Institute University of Central

Nonradial modes-Dipole modes( ) ( ) jqjq immm ePY cos, 11 µ

l = 1, m = -1 l = 1, m = 0 l = 1, m = +1

Animations courtesy of Rich Townsend

Page 13: Jeremiah Horrocks Institute University of Central

Nonradial modes -Quadrupole modes

( ) ( ) jqjq immm ePY cos, 22 µ

l = 2, m = -1l = 2, m = 0 l = 2, m = -2

Animations courtesy of Rich Townsend

Page 14: Jeremiah Horrocks Institute University of Central

Asteroseismology –how does it work?

• Turning radius

• Acoustic cavity

 

c 2 =G1p

r=

G1kT

m

• Sound speed

Page 15: Jeremiah Horrocks Institute University of Central

Driving mechanisms

Heat engine mechanism

• Gains heat on compression

• κ-mechanism (κappa = opacity)

• H, He, Fe main drivers

• Cepheids, RR Lyr stars,δ Sct stars, β Cep stars, SPB stars, roAp stars, pulsating white dwarfs, sdB variables, …

Stochastic driving

• Star resonates with acoustic noise

• Solar-like oscillators

• Main interest in exoplanet finding

Page 16: Jeremiah Horrocks Institute University of Central

Early versions of this figure were made by JørgenChristensen-Dalsgaard

(Aarhus University) and by Pieter Degroote (KU Leuven).

This updated version was produced by Peter Papicsbased on the version in his PhD Thesis (Papics, 2013).

Page 17: Jeremiah Horrocks Institute University of Central

The sun as a star - BiSON

Page 18: Jeremiah Horrocks Institute University of Central

The sun as a star - GOLF

large separationsmall separation

Page 19: Jeremiah Horrocks Institute University of Central

Saxo

Java

Gemma

Chaplin et al. 2010, ApJ, 713, L169

Dn µ r µM

R3nmax µ

g

Teff=GM / R2

Teff

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Stellar Age

White et al. 2011, ApJ, 743. 161

Page 22: Jeremiah Horrocks Institute University of Central

p modes and g modes

Aerts, Christensen-Dalsgaard, Kurtz 2010, Asteroseismology, Springer

Page 23: Jeremiah Horrocks Institute University of Central

The Sun

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KIC 11145123

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g modes

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g modes

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g mode splitting

• For high overtone dipole g modes Cn,l asymptotically approaches 0.5

• Cn,l ≈ l/(l+1) = 0.5 for KIC 11145123 g modes

• This is model independent

• The splitting between the g mode sectoral m = +1 and -1 frequencies measures the “average” rotation rate in the core.

• Pcore ≥ 105.13 ± 0.02 days

Page 31: Jeremiah Horrocks Institute University of Central

kernels

Page 32: Jeremiah Horrocks Institute University of Central

Dipole triplet

Quadrupole quintuplet

Radialsinglet

p modes

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p mode triplet

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p mode quintuplet

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p mode splitting

• For the p modes Cn,l < 0.03 ≈ 0

• This is model independent

• The splitting between the p mode frequencies measures the “average” rotation rate near the surface.

• Psurface ≤ 98.57 ± 0.02 days

• The surface rotates more quickly than the core

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The Ap stars

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The roAp stars

• Teff: 6600 – 8500 K

• Ppul: 4.68 – 23.6 min

• Aphot B: < 10 mmag

• Arv: < 8000 m s-1

• Bs: < 30 kG

• Very peculiar: atomic diffusion

• Oblique pulsators

• Chemically stratified atmospheres

log 5000

-5

-4

-3

-2

-1

0

Pr, Nd

H

Fe

Page 39: Jeremiah Horrocks Institute University of Central

HD154708 – 24.5 kG

Hubrig, Mathys, Kurtz et al., 2009, MNRAS, 396, 1018 1/18/2021IAC WS 2010 – Lecture 2

Page 40: Jeremiah Horrocks Institute University of Central

Heartbeat Stars – KOI-54

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Animation courtesy of Jim Fuller

Page 42: Jeremiah Horrocks Institute University of Central

Tidal Asteroseismology • HD 74423

• V = 8.6

• A7VkA0mA0 lambda Boo star

• Ellipsoidal variable

• Tidally trapped dipole oblique pulsator

• Pulsation axis = tidal axisFirst one!

• Essentially only one side of the star pulsates

Page 43: Jeremiah Horrocks Institute University of Central
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Page 46: Jeremiah Horrocks Institute University of Central

1926

What appliance can pierce through

the outer layers of a star and test

the conditions within?

Page 47: Jeremiah Horrocks Institute University of Central

Asteroseismology

A new revolution with the Kepler and TESS

space missions

Emeritus Professor Donald Kurtz Jeremiah Horrocks Institute

University of Central Lancashire