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Fourier tachometer. 4. SIAMOIS. Principle. Scientific program. Schedule. Granada:16 - 18/04/ 08 ... Fourier tachometer. Another advantage: multi-object advantage ... – PowerPoint PPT presentation

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Title: Prsentation PowerPoint


1

SIAMOIS asteroseismic observations after CoRoT
the need for spectroscopic measurements
Benoit Mosser - LESIA (presented by
Jean-Pierre Maillard, IAP)
2
Outline
  • Asteroseismology
  • Photometric observations with CoRoT
  • Spectroscopic results from ground (HARPS, )
  • Performance comparison
  • Photometric measurements
  • Doppler measurements
  • Doppler measurements
  • Grating spectrometer
  • Fourier tachometer
  • 4. SIAMOIS
  • Principle
  • Scientific program
  • Schedule

3
Asteroseismology purpose
  • Age determination a few
  • Stellar radii (impact for exoplanet radii) a
    few
  • Stellar composition
  • Diagnostic of convective cores
  • Depth of convection and of second helium
    ionization zones
  • Mode excitation mechanisms (convection)
  • Rotation and internal structure

Specification eigenfrequency resolution
d? 0.2 µHz ? continuous observations (h gt
80 ) ? long duration (d? 1/T) (T gt 2.5
months)
4
CoRoT
  • launched on December 27th , 2006
  • by Soyuz 2, from Baikonour, Kazakhstan
  • low Earth polar orbit, 896 km altitude
  • orbital period 6184 s (1h43mn, 162 mHz)
  • high precision photometry
  • The CoRoT space mission was developped and is
    operated by CNES, with the contribution of
    Austria, Belgium, Brazil, ESA, Germany and Spain

5
CoRoT light curves
  • Typical CoRoT light curve
  • ? Photon noise limited performance 1 ppm
  • 150 days
  • Duty cycle 92

Typically 10-4 in 30 s
Variability below the 10-3 level over 20 days of
a 6th magnitude F star
6
Photometry (1)
HD 49933, mV5.7, F5V, observed during the
initial run (60 days)
Mode amplitudes 1 few ppm ? observation of
p-mode oscillations in solar-like stars not
achievable by photometric ground-based
measurements
7
Photometry (2)
HD 181420, mV6.7, F2V, first long run (150 days)
Stellar granulation important contribution at
low frequency ? limits the spectrum SNR for
f lt 2 mHz
8
Ground-based observations
  • solar-like oscillations in solar-like stars
  • HARPS _at_ ESO 3.6-m
  • UCLES _at_ AAT
  • CORALIE _at_ Euler telescope
  • SOPHIE _at_ OHP
  • instruments _at_ SARG, McD, Okoyama, Lick

Observations limited to a few days
9
Spectroscopic result (1)
  • Procyon, 10-day network observation
  • (11 observatories, Jan. 2007)
  • Identification of mixed modes
  • ? Definitely a post-MS star
  • Mosser et al 2008, AA 478, 197
  • Bedding et al 2008, in preparation

Day aliases (11.57 Hz) still present too short
duration compared to stellar rotation period
10
Spectroscopic result (2)
HD 203608 F6V mV 4.8 Old star of the thick
galactic disk 5 days observation with HARPS duty
cycle 40
Stellar modelling before with
asteroseismic constraints L/Lo 1.40
0.13 1.38 0.045 M/Mo 0.88 0.07 0.928
0.028 R/Ro 1.04 0.12 1.06 0.02 T (K) 6070
150 6051 45 Fe/H -0.60 0.10 -0.55 0.05
Age (Gyr) 10.5 4 7.2 0.3
Mosser et al 2008, submitted to AA
Precision still hampered by poor frequency
resolution and duty cycle
11
Doppler asteroseismometry
  • Principle photon noise limited performances
  • - Q quality factor of the spectrum
  • - Ne number of photoelectrons collected
  • Q depends on
  • - the spectral type and the v.sini (rotation) of
    the star
  • the type of instrument
  • GS grating spectrometer
  • FS Fourier Transform spectrometer

12
Quality factor
  • The quality factor Q gives
  • a measure of the
  • number
  • depth
  • width
  • of the lines in the stellar spectrum
  • Q dln A /dln l

Better Q factor for cooler stars Better
performances in the blue part of the visible
spectrum
Supposes a high resolving power ( 100 000) of
the grating spectrometer
13
Comparison Photometry/Spectrometry
Photometry Spectrometry Q stellar
oscillation quality factor Oscillation
amplitudes 1 ppm ?? 10 cm/s
Photometric observations dimmer targets, or
smaller telescope 1 ppm sensitivity require
space-borne observations
14
Doppler / photometry on the Sun
Solar granulation noise photometric observations
50 times noisier at low frequency than Doppler
measurements
15
Granulation noise
16
l3 modes
l3 modes have higher visibility in spectroscopy
Small separation
17
Doppler / photometry on the Sun
Core size determination
low frequency noise l3 modes
?
Inversion 4 times more precise with Doppler data
Gabriel et al 1998
18
Space / Ground
19
Fourier Transform Seismometry
Fourier transform Seismometry The Doppler signal
is retrieved from the interferogram of the
stellar spectrum
20
Fourier Transform Seismometry
FT seismometry successfully tested with the FTS
at CFHT Procyon Mosser et al. 1998, AA 340,
457 Jupiter Mosser et al. 2000, Icarus 144, 104
  • FTS at CFHT repeated scan of one selected
    fringe of the interferogram
  • shift of the fringe signal with time ? Doppler
    signal

21
FS quality factor
with
  • (Mosser, Maillard, Bouchy 2003, PASP 115, 990)
  • Q increases with
  • wavenumber s0
  • working path difference dopt
  • fringe contrast C
  • A high fringe contrast C requires a narrow
    bandwidth
  • To be compatible with a high Ne factor requires
    a dispersion of the
  • fringes (post-disperser) many adjacent
    narrow bandwiths

22
FS Q with post-dispersion
Fourier transform seismometry with
post-dispersion The Doppler signal is searched
in the interferogram of each spectral element
defined by the post-disperser
Q factor as a function of the post-dispersion
resolution and the spectral type for 3 vsini
23
GS / FS
GS HARPS (ref ThAr lamp) R 115000
FS post-dispersion resolution R 1000
dv(GS) / dv(FS) as a function of v sini and T
of the star
GS gt FS if reference ThAr lamp (Mosser et al.
2003) GS FS if reference iodine cell
24
GS / FS
FS smaller and simpler instrument than a GS
monolithic interferometer no moving parts
(SIAMOIS concept) ? possible
installation and setup at Dome C
25

SIAMOIS Système Interférentiel A Mesurer les
OscIllations Stellaires
  • A Fourier Spectrometer dedicated to
    asteroseismology with no moving parts
  • to be installed at Dome C behind a 40-cm
    telescope
  • phase A completed
  • P.I. B. Mosser
  • Scientific Committee
  • Th. Appourchaux (France, pdt), C. Catala (inst.
    scientist), S. Charpinet (France), D. Kurz (UK),
    Ph. Mathias (France), A. Noels (Belgium), E.
    Poretti (Italy),

26
SIAMOIS performances at Dome C
Photon noise limited performances SIAMOIS, at
Dome C, 40-cm telescope, 120 hours with 95 duty
cycle, mV 4 SNR on circumpolar targets
27
SIAMOIS performances at Dome C

SIAMOIS with post-disperser R 1000 at Dome C
for 3 solar-like stars
28
Targets
  • K, G, F, class IV V targets
  • Red giants
  • Delta-Scuti, gamma Dor, PMS

Since long-duration observations are required, a
40-cm telescope provides already a scientific
program on p-mode oscillation in solar-like
targets as large as the CoRoT program
29
Targets with a 40-cm telescope
COROT
Observable solar-like stars with p-mode
oscillations for a dedicated 40-cm telescope
  • 40-cm telescope
  • - 7 bright targets, type F, G, K class IV V
  • - many red giants d Scuti (v sin i lt 20 km/s)
  • Scientific program for more than 6 winterings
  • Program complementary to CoRoT

30
Clear sky fraction at Dome C
Clear sky fraction gt 90 during 84 of the time
Average number of consecutive clear days 6.8 days
31
Duty cycle
Better performance at Dome C compared to a 6-site
network (Mosser Aristidi 2007, PASP)
32
SIAMOIS
  • 40-cm telescope small size, low cost,
    easy antarctization, dedicated to the project
  • Interferometer fiber fed Mach Zehnder
    interferometer, operated at room temperature,
    monolithic no moving parts, photon
    noise limited performance
  • Data automatic pipeline reduction,
    telemetry limited flow lt 100 kb/day

Phase A completed, April 2007
33
Simulations
l 2 0 3 1
F6V star, mV 4.5, vsini 5 km/s, 90-day long
run Modelling stochastic excitation intrinsic
damping ? Lorentzian profiles (Anderson et al
1990)
34
Simulations
Longer lifetimes at low frequency ? clear
multiplets
l 2 0 3 1
F6V star, mV 4.5, vsini 5 km/s, 90-day long
run Precision on the eigenfrequency measurement
0.10 0.25 mHz (Libbrecht 1992)
35
Fourier tachometer
  • Another advantage multi-object advantage
  • ? simultaneous observations of several targets

First step small telescope FT Then
multi-targets observation small telescopes 1
FT
36
Planning budget
  • lt 2006
  • principle monolithic Fourier
  • Tachometer
  • 2007
  • thermo-mechanical analysis
  • phase A
  • 2009-2011
  • PDR
  • FDR
  • integration
  • 2011-2012
  • tests
  • summer campaign Dome C
  • 2013
  • First winterover at Dome C

LESIA (Obs. Paris), IAS (Orsay), LUAN (Nice),
OMP (Toulouse) SESO
Budget 860 k ltlt budget for an equivalent
6-site network
37
Perspectives
  • Asteroseismology requires uninterrupted
    long-duration time series !
  • 1 dedicated 40-cm telescope
  • first season observation
  • fiber FOV 5 (gtgt seeing)
  • stellar magnitude lt 5 for solar-like
    oscillations
  • lt 7 for classical pulsators
  • 2 or 3 dedicated small telescopes
  • - next step
  • simultaneous observations of 2 or 3 stars
  • 2-m class telescope?
  • stellar magnitude lt 8.5 for solar-like
    oscillations
  • increase of the number of reachable targets
  • possibility to achieve specific observations in
    selected targets
  • However, a dedicated telescope would be required

38
Other projects KEPLER
  • NASA launch nov 2008
  • High precision photometry
  • a few fields reserved
  • for asteroseismology
  • CoRoT ? Kepler
  • tel. 27 cm ? 95 cm
  • orbit polar ? L2
  • duty cycle in L2
  • sensitivety (mV gt 9), radiations in L2
  • ? exact scientific case for asteroseismology?
  • 29-31 October 2007 First KASC workshop, Paris.
    The Kepler Asteroseismic Science Consortium
    (KASC) is an international consortium of
    researchers dedicated to the asteroseismic
    analysis of Kepler data.

39
SONG
  • Project currently in phase 0
  • Danish asteroseismology centre, Aarhus
    University
  • Network of 6 to 8 small telescopes (60?80 cm)
  • Echelle spectrometer iodine cell
  • Expected schedule 1 prototype for 2012-2013

gtgt 2012
40
Comparison
41
Conclusions
Space-borne observations photometric
observations CoRot unique results Kepler
not primarily specified for asteroseismology
sensitivity for p-mode oscillations under
question very dim targets ? uncertainty on
fundamental parameters Ground-based observations
Doppler observations measurement of modes up
to degree l 3 much less low frequency
noise ? much better inversion and modelling
observation of low mass stars Network very late
schedule, complex organization Dome C unique
site for asteroseismology 3-month continuous
observation with duty cycle 90 High
performance with a 40-cm collector Better
performance than a 6-site network
http//siamois.obspm.fr
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