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Asteroseismology with A-STEP The sun from the South Pole Grec, Fossat & Pomerantz, 1980, Nature, 288, 541 Asteroseismology Angular structure of the modes • n = number of radial nodes • = total number of surface nodes • m = number of surface nodes that are lines of longitude • – m = number of surface nodes that are lines of latitude Dipole modes m 1 Y , P1m cos eim l=1, m=0 l=1, m=+1 Quadrupole modes Y2m , P2m cos eim l=2, m=0 l=2, m=-1 l=2, m=-2 p modes and g modes p modes (n,) = (8,100), (8,2) g mode (n,) = (10,5) Gough et al., 1996, Science, 272, 1281 p modes and g modes J. P. Cox, 1980, Theory of Stellar Pulsation, Princeton University Press. The sun as a star - BiSON The sun as a star - GOLF n 0 n 2 large separation small separation An asteroseismic HR diagram Solar-like Oscillations in Centauri Bedding, T., et al. 2004, ApJ, 614, 380 • UVES & UCLES • 42 oscillation frequencies • ℓ = 1-3 • Mode lifetimes only 1-2 days • Noise level = 2 cm s-1! From G. Houdek Amplitudes in velocity between 10 to 250 cm/s Amplitudes in intensity are of the order of 1-10 ppm roAp HR 1217 WET Xcov20 Kurtz et al., 2005, MNRAS, 358, 651 HR 1217 WET Xcov20 Kurtz et al., 2005, MNRAS, 358, 651 p modes: Cephei stars HD 129929 = V836 Cen 20-yr multicolour photometry Core overshooting with aOV = 0.1 Non-rigid rotation: 4 times faster near core Aerts et al., 2003, Science, 300, 926 Asteroseismology of HD129929: Core overshooting and nonrigid rotation p modes: EC 14026 stars - sdBV PG 1336 + 018 g Dor – mixed-mode pulsators HD 49434 White dwarfs – g-mode pulsators BPM 37093 A giant solar-like oscillator http://www.lcse.umn.edu/ COROT Field of view Adaptation of COROTLUX software for variables Input sample: Besançon model ~ 25000 stars Pulsation in EXO FoV Cep : 2 SPB : 29 Sct : 2500 g Dor : 3200 Hyb : 2200 Ceph : 1 LP : 46 Fraction of variables: 30%? Stellar limitation • Photon noise • Stellar noise • Activity < 10-4 up to M=15 low frequencies see S. Aigrain Instrumental limitation • Read-out noise • Thermal noise • Guiding noise • Cosmic rays • Gain variation • Shutter noise Lower than photon noise for M<16 negligible 2 p 3 5 . 10 PRNU~1%, I 3 4 S TBE no data. Global/pixel 1- 2 ms -> Ti > 30 s Atmospheric limitations of photometric observations • Transparency fluctuations • Interruptions (clouds) • Scintillation •Diffused light No dust, low humidity, snow < 15 % Better than anywhere else, but still limiting Few auroras, moon These values are still uncertain: A-STEP will contribute to the site qualification A few words about atmospheric turbulence and scintillation 2 2 2 r0 0.42 sec Z Cn (h)dh h 3 5 sec Z h 6 Cn 2(h)dh h 7 2 3 2 I 19.12 D 3 sec Z h 2Cn (h)dh h 7 I 19.12 2 5 / 6 0 6 11 6 5 K cos z I 4 / 3 D D h h From Dravins et al, 1997 Optical/interferometric parameters Integrated from h=8m Balloons (10) Seeing (arcs) 1.6 t0 (ms) 7.0 0 (arcs) 5.3 Dimms (March- May 05) 1.2 GSM h=3.5m L0 = 10 m h>0m opd 3 h > 30 m 1 3.6 Interferometric coherence times t0 = 0.31 r0/ v ~7 ms Integrated from h =30m Balloons AASTINO 2004 data Seeing (arcs) 0.4 0.27 ‘’ t0 (ms) 11.2 7.9 0 (arcs) 5.3 5.7 ‘’ s T0 = 0.31 L0/ v ~775 ms Optical/interferometric parameters Integrated from h=8m Balloons (10) Seeing (arcs) 1.6 t0 (ms) 7.0 0 (arcs) 5.3 Dimms (March- May 05) 1.2 GSM h=3.5m L0 = 10 m h>0m opd 3 h > 30 m 1 3.6 Interferometric coherence times t0 = 0.31 r0/ v ~7 ms Integrated from h =30m Balloons AASTINO 2004 data Seeing (arcs) 0.4 0.27 ‘’ t0 (ms) 11.2 7.9 0 (arcs) 5.3 5.7 ‘’ s T0 = 0.31 L0/ v ~775 ms Conclusion • Asteroseismology benefits a lot from continuity • A-STEP very similar to COROT EXO Field • Unlike COROT, the full dataset can be recovered • roAp, gDor are top-priority programs • PMS Scuti, Red Giants to be investigated • Solar-type stars ? Requirements • • • • • • 30 – 60 s integration time 90 days continuous observations Good guiding Precise timing Best telescope height still unknown Color photometry allow mode identification