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A Quest for Double-Mode Variables
And Other Tidbits from the Zoo of Pulsating Stars Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren Patrick Wils
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Based on Data from: CCD Visual All Sky Automated Survey: ASAS3
Northern Sky Variability Survey: NSVS Individual observers: C.W. Robertson (US) Joaquin Vidal (ES) Michael Koppelman (US) Neil Butterworth (AU) Paul Van Cauteren (BE) Russ Durkee (US) Stelios Klidis (GR) Visual AAVSO Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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In Collaboration with:
Adam Sodor (HU) Christopher Lloyd (UK) Ennio Poretti (IT) Klaus Bernhard (AT) Sebastian Otero (AR) Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Pulsating Variable Stars
Brightness variations because the star expands or contracts For “normal” stars, pulsations will die out rapidly Pulsations are stable only for certain periods in the life of a star: the “instability” strip in the HR diagram Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Radial Pulsation versus Non-Radial Pulsation
Spherical shape is kept Internal layers expand or contract as a whole Generally large amplitude Non-radial pulsation Parts of the surface move outward while others move inward “Nodes” on the surface of the star Smaller amplitude because total surface area will change less Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Non-Radial Pulsation Delta Scuti stars Small amplitude Short periods
Asteroseismology “star quakes”: probe the interior of stars Source examples: Delta Scuti Network Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Fundamental Mode versus Overtones: String Vibrations
Guitar, piano, ... Fundamental mode: 0 nodes, 1st overtone: 1 node, 2nd overtone: 2 nodes, ... Overtones are harmonics/higher octaves P(1O) = P(F)/2 P(2O) = 2P(1O)/3: exact (low) integer fractions Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Double-Mode Strings Genk, 13 May 2006
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Fundamental-Mode Pulsation
Radial pulsation All layers inside the star move in the same direction No “nodes” inside the star Example is exaggerated: the pulsations will never go deep into the core of the star Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Overtone Pulsation Radial pulsation
Different layers may move in different directions One or more “nodes” inside the star (layers that do not move) Do not confuse with harmonics from Fourier analysis 1st overtone example: Sine functions are an exact representation of the vibrations of a string, but not for the brightness of a pulsating star: a Fourier series is a just a mathematical representation for it, as there is no “pulsation sine” function. To model the vibration of a “double-mode string” one needs only 2 sine functions: 2 Fourier terms with one period and its first harmonic; for “double-mode” stars one needs 2 series with an “infinite” number of Fourier terms (2 incommensurate periods). Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Fundamental Mode/1st Overtone Pulsation
Stability of the mode depends on the physical properties of the star (location in HR diagram) Determined by theoretical calculations and: Phase difference + amplitude ratio for different colours “Pulsation constant” Q (Mbol, Teff, g, P) 1st Overtone: “Dwarf” Cepheids (DCEPS) RRc Mira/SR variables? Fundamental mode: Most Cepheids (Pop. I + II) HADS RRab Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Fundamental Mode/1st Overtone Pulsation
RRab 1st overtone: RRc Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Higher Overtones Almost symmetric light-curve Short periods
Some (very short period) Cepheids may be second overtone pulsators; but no examples in the Galactic field Unclear whether RRe stars really exist Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Double-Mode Pulsation
Two stable radial pulsation modes Linear combinations of independent modes Important objects for pulsation theories Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Double-Mode Pulsation: HADS
Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Double-Mode Pulsation: RRd
Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Double-Mode Pulsation
“Fixed” ratio between 1st overtone and fundamental period: No integer fractions (as in strings) Cepheids: ~0.705 RR: ~0.745 HADS: ~0.77 2 Galactic Cepheids are 1st/2nd overtone double-mode pulsators: CO Aur, HD Ratio for DCEP(B), RRd, HADS(B): ~ 3 Triple-Mode variables: AC And, V829 Aql, V823 Cas Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Petersen Diagram Period ratio versus fundamental period
“Spread” due to different metallicity or mass Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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How to Find Double-Mode Variables?
Lots of data needed (wide-field surveys!) Period analysis (PDM, Period04, ...) Look for periodic stars with unusually high scatter Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Double-Mode Stars Discovered
Type New Total (mag<14) DCEP(B) 4 22 HADS(B) 8 16 RRd References: IBVS 5501 A&A 440, 1097 IBVS 5698 And references therein Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Stars of Special Interest
Two modes: High amplitude -> radial Not a standard ratio Binary variables? No: linear combination modes! V371 Per Cepheid Periods 1.27 and 1.74 days Ratio 0.73 V767 Sgr Cepheid? Periods 0.54 and 0.67 days Ratio 0.80 (< 1st/2nd overtone) Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Beat Period Double-mode Cepheids = “Beat” Cepheids
1/Beat period = 1/Period1 – 1/Period2 Close periods => Long beat periods Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Blazhko Effect One or more frequencies very close to the main frequency Amplitude/phase modulation Beat periods 6-~1000 days RR Lyrae stars, especially RRab Very few Galactic RRc Blazhko stars known Two possible causes, both based on rotation: Resonance between radial and non-radial modes Oblique magnetic field Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Blazhko Effect: Examples
Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Radial Mode + Non-Radial Mode Pulsation
HADS: GSC : 1 radial + 2 non-radial modes Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Hertzsprung Sequence Genk, 13 May 2006
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Fourier Analysis: (Invariant) Phase Differences
Describe brightness variations mathematically using sine functions (Fourier series) V = V0 + A1 sin(wt + f1) + A2 sin(2wt + f2) + ... Phase difference fundamental mode + first harmonic: Small amplitude harmonic (bump) Large amplitude harmonic (RV Tau?) Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Fourier Analysis: Hertzsprung Sequence
Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Fourier Analysis: Generalized Phase Differences
Linear combination modes Double-mode G11: HADS, RR, Cepheids Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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RV Tau Stars Alternating faint/bright minima (like Beta Lyr!)
Best known example: R Sct Also double-mode with ratio 1:2 ? Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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RV Tau Stars: Sub-types
RVa RVb (binaries + circumstellar dust?) Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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RV Tau: Visual Data RVa RVb Genk, 13 May 2006
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DI Car RW Aur ? W Vir (Population II Cepheid) ? Like R Sct (RVa) ?
Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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DI Car Carbon star: link with R CrB ? Genk, 13 May 2006
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Open Questions Fixed G11? : more (accurate) data needed
Why aren’t there any W Vir DM-stars? DM-stars among LPV (BS Lyr)? Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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Conclusion A lot of variables have been under-observed, their real type not known Plenty of work that can be done by amateur astronomers: Long time series Multi-colour data Data mining Visual observers: more RV Tau stars! BS Lyr, other DM-Mira? Genk, 13 May 2006 VVS Werkgroep Veranderlijke Sterren
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