why we need song

31
Why We Need SONG Sarbani Basu Yale University

Upload: koko

Post on 21-Jan-2016

28 views

Category:

Documents


0 download

DESCRIPTION

Why We Need SONG. Sarbani Basu Yale University. Image courtesy J. Christensen-Dalsgaard. Observing in Velocity: Lower Noise. Observing in Velocity: non-zero l =3 response. We do not know how to model the near surface layers of stars. Problems convection/turbulence Atmospheres - PowerPoint PPT Presentation

TRANSCRIPT

Page 1: Why We Need  SONG

Why We Need SONG

Sarbani BasuYale University

Page 2: Why We Need  SONG

Image courtesyJ. Christensen-Dalsgaard

Page 3: Why We Need  SONG

Observing in Velocity: Lower Noise

Page 4: Why We Need  SONG

Observing in Velocity: non-zero l=3 response

Page 5: Why We Need  SONG

THE PESKY SURFACE TERM

We do not know how to model the near surface layers of stars. Problems

(1)convection/turbulence(2)Atmospheres (3)Low temperature opacities(4)Treatment of radiation in optically thin layers(5)…..

These problems introduce a frequency dependent offset between observed and modelled frequencies.

Page 6: Why We Need  SONG
Page 7: Why We Need  SONG

Surface term in Standard Solar Models

Page 8: Why We Need  SONG
Page 9: Why We Need  SONG

Same interior physics could still give rise to different surface terms

Page 10: Why We Need  SONG

What happens with deficient physics?

Page 11: Why We Need  SONG

Low Frequencies will help in modelling by defining the surface term

Page 12: Why We Need  SONG

Surface Term and Echelle Diagrams

Page 13: Why We Need  SONG

What we observe

Page 14: Why We Need  SONG

What we observe

Page 15: Why We Need  SONG
Page 16: Why We Need  SONG

What happens if we do not have low-frequency modes

obsν0

⎜⎜⎜

⎟⎟⎟

b

Page 17: Why We Need  SONG

What happens if we do not have low-frequency modes

obsν0

⎜⎜⎜

⎟⎟⎟

b

Page 18: Why We Need  SONG

Add Lower frequencies

Page 19: Why We Need  SONG

What else? Define other diagnostics

Separation Ratio: r

02=

ν(0,n+1) −ν(2,n)ν(1,n+1) −ν(1,n)

Separation Ratio: r

13=

ν(1,n+1) −ν(3,n)ν(2,n+1) −ν(2,n)

Page 20: Why We Need  SONG

2nd differences: δ 2ν =ν(n−1, l) −2ν(n, l) +ν(n+1, l)

Page 21: Why We Need  SONG

l=3 modes will allow inversions

A Hermitian Eigenvalue problem, therefore use the variational principle:

Page 22: Why We Need  SONG

How we invert frequecies

Page 23: Why We Need  SONG

The mode-sets

Page 24: Why We Need  SONG

The solutions

Page 25: Why We Need  SONG

The Averaging Kernels

Page 26: Why We Need  SONG

Cross-term kernels

Page 27: Why We Need  SONG
Page 28: Why We Need  SONG

Lower Turning Points of modes

Page 29: Why We Need  SONG

Add Low-Frequency modes to l=0,1,2 sets

Page 30: Why We Need  SONG

The Best Kepler Modeset (so far)

Low frequency modes will made a huge difference

Page 31: Why We Need  SONG

Conclusions

• Low-frequency modes will help us to model stars better.

• l=3 modes will help us invert frequency differences between a star and its model to determine how good a model is.

• SONG will be able to provide both low-frequency modes, as well as l=3 modes

ERGO

WE NEED SONG