tests of convective zone radial differential rotation in intermediate...

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LBTO users meeting, Florence, June 20-23, 2017 Tests of convective zone radial differential rotation in intermediate-mass core-helium burning stars with PEPSI J. Tayar ([email protected]), M. H. Pinsonneault (OSU), I. Ilyin, K. G. Strassmeier (AIP) The problem: surface rotation rates of secondary clump stars are MUCH slower than models predict Why we needed PEPSI v sin(i) (km/s) Data Hipparcos Stars Massarotti et al. (2008) Model predictions Tayar et al. (in prep) Kawaler Angular Momentum Loss Solid Body Rotation Similar results using APOGEE- Kepler v sin(i)s (Tayar et al. 2015), Kepler surface rotation periods (Ceillier, Tayar, et al. submitted), and seismic envelope rotation rates (Deheuvels et al. 2015) Masses between 2.0 and 3.0 M o , log(g) between 3.1 and 2.0 Forward model from main sequence rotation distribution of Zorec & Royer (2012) One solution: radial differential rotation in the surface convection zone Convective Radiative Original model: solid body rotation New model: radial differential rotation Fix core to the base of the envelope Differential rotation slows down the surface The prediction: cores, envelopes, AND surfaces should have different rotation periods Core and envelope rotation periods are different Only one star in the sample has a measured surface period from spots Without surface periods, we can't tell whether the differential rotation is in the surface convective zone Adapted from Reiners & Schmitt (2002) R=270,000 allows us to measure v sin(i) down to ~ 1.3 km/s Using the seismically measured radii and inclination angles, we can convert between v sin(i) and period Envelope rotation periods predict v sin(i) from 2.4-4.4 km/s Differential rotation would predict lower v sin (i) PEPSI resolution R e s o l u t i o n v sin(i) (km/s) Lowest measurable v sin(i) Measuring v sin(i) Preliminary results We have tentative evidence of radial differential rotation in the surface convection zone of intermediate-mass core-helium burning stars Tayar et al. (in prep) (Days) Core and envelope periods from Deheuvels et al. (2015) Surface period from Ceillier, Tayar et al. (submitted) Data Fourier v sin(i) Goodness-of-fit Fourier v sin(i)+ v macro (fit) Envelope v sin(i)+ APOGEE v macro Rotational velocities and macroturbulent velocities are comparable Take the Fourier transform of individual lines to separate the two broadening components Use the iacob_broad package from Simon-Diaz & Herrero (2014) v sin(i) Period Average Solid body envelope Evidence for envelope differential rotation? Y error bars are currently off the scale of this plot Ongoing work: adding more lines, removing blended lines, improving error analysis, checking calibration, validating method

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Page 1: Tests of convective zone radial differential rotation in intermediate ...abell.as.arizona.edu/~lbtsci/UM2017/Presentations/LBTOUser_poster... · Tests of convective zone radial differential

LBTO users meeting, Florence, June 20-23, 2017

Tests of convective zone radial differential rotation in intermediate-mass core-helium burning stars with PEPSIJ. Tayar ([email protected]), M. H. Pinsonneault (OSU), I. Ilyin, K. G. Strassmeier (AIP)

The problem: surface rotation rates of secondary clump stars are

MUCH slower than models predict

Why we needed PEPSI

v sin(i) (km/s)

DataHipparcos StarsMassarotti et al. (2008)

Model predictionsTayar et al. (in prep)Kawaler Angular Momentum LossSolid Body Rotation

● Similar results using APOGEE-Kepler v sin(i)s (Tayar et al. 2015), Kepler surface rotation periods (Ceillier, Tayar, et al. submitted), and seismic envelope rotation rates (Deheuvels et al. 2015)

● Masses between 2.0 and 3.0 Mo, log(g) between 3.1 and 2.0

● Forward model from main sequence rotation distribution of Zorec & Royer (2012)

One solution: radial differential rotation in the surface convection zone

ConvectiveRadiative

Original model: solid body rotation

New model: radial differential rotation

Fix core to the base of the envelope

Differential rotation slows

down the surface

The prediction: cores, envelopes, AND surfaces should have different rotation periods

● Core and envelope rotation periods are different● Only one star in the sample has a measured surface period from

spots● Without surface periods, we can't tell whether the differential

rotation is in the surface convective zone

Adapted from Reiners & Schmitt (2002)

● R=270,000 allows us to measure v sin(i) down to ~ 1.3 km/s

● Using the seismically measured radii and inclination angles, we can convert between v sin(i) and period

● Envelope rotation periods predict v sin(i) from 2.4-4.4 km/s

● Differential rotation would predict lower v sin (i)

PEPSI resolution

Res

olu

tion

v sin(i) (km/s)

Lowest measurable v sin(i)

Measuring v sin(i)

Preliminary results

We have tentative evidence of radial differential rotation in the surface convection zone of

intermediate-mass core-helium burning stars

Tayar et al. (in prep)

(Days)

Core and envelope periods from Deheuvels et al. (2015)

Surface period from Ceillier, Tayar et al. (submitted)

Data

Fourier v sin(i)

Goodness-of-fitFourier v sin(i)+v macro (fit)Envelope v sin(i)+ APOGEE v macro

● Rotational velocities and macroturbulent velocities are comparable● Take the Fourier transform of individual lines to separate the two

broadening components● Use the iacob_broad package from Simon-Diaz & Herrero (2014)

v sin(i)

Period

Average

Solid body envelope

Evidence for envelope differential rotation?

● Y error bars are currently off the scale of this plot● Ongoing work: adding more lines, removing blended lines,

improving error analysis, checking calibration, validating method