light and radial velocity variations due to low frequency oscillations in rotating stars jadwiga...
TRANSCRIPT
LLIGHT AND RADIAL VELOCITY IGHT AND RADIAL VELOCITY VARIATIONSVARIATIONS
DUE TO LOW FREQUENCY DUE TO LOW FREQUENCY OSCILLATIONS OSCILLATIONS
IN ROTATING STARSIN ROTATING STARS Jadwiga Daszyńska-Daszkiewicz Instytut Astronomiczny, Uniwersytet Wrocławski, Poland
Collaborators: Wojtek Dziembowski , Alosha Pamyatnykh
2222 NovemberNovember 2006, 2006, Porto Workshop Porto Workshop
INSTABILITY DOMAINS IN THE MAIN SEQUENCEINSTABILITY DOMAINS IN THE MAIN SEQUENCE
4.6 4.4 4.2 4.0 3.8 3.6
0
1
2
3
4
5
6
solar-likeoscillation
Dor
TAMS
ZAMS
1
2
4
12
30
60
Cep, field
Cep, NGC 3293
Cep, NGC 4755
Cep, NGC 6231
SPB Sct
OPAl 1996
X=0.70, Z=0.02, =1.0
logL
/Lo
logTeff A. A. PamyatnykhA. A. Pamyatnykh
for SPB pulsators often ~
Slow modes in the traditional approximationSlow modes in the traditional approximation
not too fast rotation: ( / crit)2 << 1
Cowling approximation
~ ~ << N(r)
Separation of the angular and radial dependences in eigenfunctions
s= 2/ (+1) (s) Ym (cos)eim
(cos) - the Hough functions
Modes with >0 propagate in the radiative zone (N>0).The radial wave number
Definition of mode degree, , for g-modes
s = 2/ 0 then (+1)
Retrograde r-mode with g-modes properties at s>|m|+1(Savonije 2005, Townsend 2005)
the Hough function
the Hough function
(, /2) – the normalized driving rate
For instability:
2/ - should match the thermal time scale in the driving zone
/2 – determines the r-dependence of eigenfunctions The pressure eigenfunction should be large in the driving zone
like (+1)/2 for high order g-modes in non-rotating stars
Radial displacementRadial displacement
Z = exp [i (m - t)]
in co-rotating system
m>0 - prograde modes
m<0 - retrograde modes
Oscillating atmospheric parametersOscillating atmospheric parameters
f (, /2)
Fx (Teff, log g)
hx (ns,Teff, log g)
Light variations in the x passband Light variations in the x passband
Pulsation velocity field Pulsation velocity field
Disc-averaged radial velocityDisc-averaged radial velocity
pulsational partpulsational part rotational partrotational part
the rotational contribution tothe rotational contribution to
arises from arises from rr, , n, n, FFbolbol, , gg
An example:An example:
M=6 MM=6 M, MS star, MS star
loglogTTeffeff= 4.205= 4.205
logL/LlogL/L= 3.204= 3.204
VVrotrot=0, 50, 150, 250 km/s=0, 50, 150, 250 km/s
Selected modes:Selected modes:
g-modes with g-modes with =1,2, most unstable =1,2, most unstable at each (at each (,m) ,m)
r-modes, most unstable with m= -1,-2r-modes, most unstable with m= -1,-2(only for V(only for Vrotrot ≥ 150 km/s) ≥ 150 km/s)
Hough functions for Hough functions for =1 and r mode with m= -1=1 and r mode with m= -1
Amplitudes of light and radial velocity variationsAmplitudes of light and radial velocity variations g-mode g-mode =1,m=0 and r-mode,=1,m=0 and r-mode, m=-1m=-1
Amplitudes of light and radial velocity variationsAmplitudes of light and radial velocity variations g-modes: g-modes: =1,=1, m= m= ±±11
Hough functions for Hough functions for =2 and r-mode with m= -2=2 and r-mode with m= -2
ProspectsProspects forfor modemode identificationidentification
Diagnostic diagrams ADiagnostic diagrams AVrad Vrad /A/AVV vs. A vs. AU U /A/AVV
fast rotation have a small effect on modefast rotation have a small effect on modestability stability butbut a large effect on visibility a large effect on visibility
there are large differences between modes there are large differences between modes in the light to radial velocity amplitude ratiosin the light to radial velocity amplitude ratios
rotation impairs mode visibility in the light rotation impairs mode visibility in the light butbut not in the mean radial velocity variations not in the mean radial velocity variations
Good prospects for mode identificationGood prospects for mode identification
g-modes with the same g-modes with the same and different m and different mddo not form regular multiplets and they haveo not form regular multiplets and they havedifferent visibility and instability propertiesdifferent visibility and instability properties