TESS Proposal on behalf of TASC WG 4 Cadence: 2-min sampling

Similar documents
Solar-like oscillations in intermediate mass stars

The Plato Input Catalog (PIC)

arxiv: v1 [astro-ph.sr] 27 Dec 2011

ASTROPHYSICS. K D Abhyankar. Universities Press S T A R S A ND G A L A X I E S

Combining WASP and Kepler data: the case of the δ Sct star KIC

The BRITE satellite and Delta Scuti Stars: The Magnificent Seven

Lines of Hydrogen. Most prominent lines in many astronomical objects: Balmer lines of hydrogen

STEREO observations of HD90386 (RX Sex): a δ- Scuti or a hybrid star?

Improving Precision in Exoplanet Transit Detection. Aimée Hall Institute of Astronomy, Cambridge Supervisor: Simon Hodgkin

468 Six dierent tests were used to detect variables, with dierent sensitivities to light-curve features. The mathematical expression for the limiting

Time-Series Photometric Surveys: Some Musings

Impact of stellar micro-variability on transit detection from space

Study of Cataclysmic Variable B7 in NGC 6791: From the Ground and from Space

Chapter 8: The Family of Stars

Synergies & Opportunities for SONG in the TESS Era

The Milky Way Galaxy (ch. 23)

C. Ulusoy 1,2 and B. Ulaş3

Life in the Universe (1)

Properties of Stars (continued) Some Properties of Stars. What is brightness?

Project title: "Magnetic activities of the Sun and the stars probed by the newgeneration

The Family of Stars. Chapter 13. Triangulation. Trigonometric Parallax. Calculating Distance Using Parallax. Calculating Distance Using Parallax

On the Red Edge of the δ Scuti Instability Strip

THE OBSERVATION AND ANALYSIS OF STELLAR PHOTOSPHERES

Monitoring nearly 4000 nearby stellar systems with the OVRO-LWA in search of radio exoplanets

Introduction The Role of Astronomy p. 3 Astronomical Objects of Research p. 4 The Scale of the Universe p. 7 Spherical Astronomy Spherical

DRM Update Joe Liske

The effects of stellar rotation and magnetism on oscillation frequencies

ASTR-1020: Astronomy II Course Lecture Notes Section III

Asteroseismology with WFIRST

HD observed by the Kepler K2 mission: a rapidly oscillating Ap star pulsating in a distorted quadrupole mode

HR Diagram Student Guide

Diffusion and helioseismology

Laboratory: Milky Way

Whole Earth Telescope discovery of a strongly distorted quadrupole pulsation in the largest amplitude rapidly oscillating Ap star

SUPPLEMENTARY INFORMATION

The Physics of Exoplanets

Gravitational microlensing. Exoplanets Microlensing and Transit methods

TESS and Galactic Science

The first evidence for multiple pulsation axes: a new rapidly oscillating Ap star in the Kepler field, KIC

Frequency in c/d

JINA Observations, Now and in the Near Future

Lecture 12: Extrasolar planets. Astronomy 111 Monday October 9, 2017

Asteroseismology in Action: Probing the interiors of EHB stars

MULTIPLE CHOICE. Choose the one alternative that best completes the statement or answers the question.

Selection of stars to calibrate Gaia

Probing Stellar Structure with Pressure & Gravity modes the Sun and Red Giants. Yvonne Elsworth. Science on the Sphere 14/15 July 2014

Detailed chemical abundances of M-dwarf planet hosts from APOGEE observations

List of submitted target proposals

Astr 5465 Feb. 6, 2018 Today s Topics

Delaware Asteroseismic Research Center. Asteroseismology with the Whole Earth Telescope (and More!)

Igor Soszyński. Warsaw University Astronomical Observatory

Exoplanetary transits as seen by Gaia

Lecture 26 The Hertzsprung- Russell Diagram January 13b, 2014

DOME C AS A SETTING FOR THE PERMANENT ALL SKY SURVEY (PASS)

2019 Astronomy Team Selection Test

Evolution Beyond the Red Giants

PENNSYLVANIA SCIENCE OLYMPIAD STATE FINALS 2012 ASTRONOMY C DIVISION EXAM APRIL 27, 2012

Physical Parameters of KID , a Low-Mass, Double- Lined Eclipsing Binary

Kepler s Multiple Planet Systems

Measuring the Stars. The measurement of distances The family of distance-measurement techniques used by astronomers to chart the universe is called

Rømer Science Mission Plan

CCD photometry of δ Scuti stars 7 Aql and 8 Aql

New Results of Spectral Observations of CP Stars in the Li I 6708 Å Spectral Region with the 6 m BTA Telescope

Fundamental Astronomy

Stellar Astrophysics: Pulsating Stars. Stellar Pulsation

Stellar Astrophysics: Stellar Pulsation

Stars and Stellar Astrophysics. Kim Venn U. Victoria

The Milky Way, Hubble Law, the expansion of the Universe and Dark Matter Chapter 14 and 15 The Milky Way Galaxy and the two Magellanic Clouds.

Lecture 25: The Cosmic Distance Scale Sections 25-1, 26-4 and Box 26-1

Relativity and Astrophysics Lecture 15 Terry Herter. RR Lyrae Variables Cepheids Variables Period-Luminosity Relation. A Stellar Properties 2

The SKYGRID Project A Calibration Star Catalog for New Sensors. Stephen A. Gregory Boeing LTS. Tamara E. Payne Boeing LTS. John L. Africano Boeing LTS

arxiv: v1 [astro-ph] 3 Jul 2008

Compact Pulsators Observed by Kepler

Revision: Sun, Stars (and Planets) See web slides of Dr Clements for Planets revision. Juliet Pickering Office: Huxley 706

Asteroseismic Analysis of NASA s Kepler Space Telescope K2 Mission Data of Compact Stars

Considerations for planning TESS Extended Missions

Asteroseismology of Exoplanet Host Stars

Chapter 15 Surveying the Stars Pearson Education, Inc.

Habitability Outside the Solar System. A discussion of Bennett & Shostak Chapter 11 HNRS 228 Dr. H. Geller

Transiting Hot Jupiters near the Galactic Center

arxiv:astro-ph/ v2 6 Dec 2006

Monday, October 14, 2013 Reading: Chapter 8. Astronomy in the news?

A unifying explanation of complex frequency spectra of γ Dor, SPB and Be stars: combination frequencies and highly non-sinusoidal light curves

3.4 Transiting planets

THE LOCAL SYSTEM AND THE HENRY DRAPER EXTENSION

Reading and Announcements. Read Chapters 8.3, 11.5, 12.1 Quiz #5, Thursday, March 21 Homework #5 due Tuesday, March 19

Lecture Three: Stellar Populations. Stellar Properties: Stellar Populations = Stars in Galaxies. What defines luminous properties of galaxies

Planet Detection. AST 105 Intro Astronomy The Solar System

Photometric Studies of GEO Debris

NGC 2660 revisited. 1520, DK 8000 Aarhus C, Denmark. 1520, DK 8000 Aarhus C, Denmark

SEARCHING FOR MAGNETIC ACTIVITY IN SOLAR-LIKE STARS OBSERVED BY KEPLER

Parallax: Measuring the distance to Stars

Ground Based Gravitational Microlensing Searches for Extra-Solar Terrestrial Planets Sun Hong Rhie & David Bennett (University of Notre Dame)

Extrasolar Planets. Methods of detection Characterization Theoretical ideas Future prospects

arxiv: v1 [astro-ph.sr] 20 Oct 2016

KIC : a bright long-period roap star in the Kepler field

Discovering Exoplanets Transiting Bright and Unusual Stars with K2

Page # Astronomical Distances. Lecture 2. Astronomical Distances. Cosmic Distance Ladder. Distance Methods. Size of Earth

Modelling Brightness Variability of Sun-Like Stars

301 Physics 1/20/09. The Family of Stars. Chapter 12. Triangulation. Trigonometric Parallax. Course/Syllabus Overview Review of 301 stuff Start Ch.

Transcription:

TESS Proposal on behalf of TASC WG 4 Cadence: 2-min sampling Title: A survey of rapidly oscillating Ap stars Abstract: The magnetic, and chemically peculiar nature of the rapidly oscillating Ap (roap) stars makes them particularly interesting targets to investigate the combined effect of diffusion, pulsations and magnetic fields. These are relatively rare objects and a significant increase in their number can only be achieved through surveys. TESS offers the opportunity to systematically search for roap stars from space for the first time. We intend to take this opportunity to: (1) Establish the observational boundaries of the roap star instability strip; (2) Increase significantly the number of members of this class; (3) Establish the fraction of Ap stars that exhibit pulsations. All of these will have profound implications on our understanding of the roap star phenomenon and, consequently, on our ability to infer information on the physical processes that take place within their interiors. The roap stars are the only stars, other than the Sun, to offer the opportunity to visualize the three- dimensional structure of abundance distributions driven by atomic diffusion, and the three- dimensional atmospheric structure of the pulsations. Atomic diffusion is important in stellar structure and evolution with wide applications, and the roap stars provide the best observational tests of diffusion theory. Authors: Margarida S. Cunha, Vichi Antoci, Luis Balona, Dominic Bowman, Daniel Holdsworth, Oleg Kochukhov, Donald W. Kurtz, Patricia Lampens, Richard Monier, Simon Murphy, Joshua Pepper, Paola Quitral, Tyler Richey- Yowell, et al.

Science Case: So far 61 roap stars have been discovered (Smalley et al., 2015) and of these only 11 have been observed in short cadence from space. The quality of the ground- based data is generally inferior to the space- based data, with only the highest amplitude pulsations being detected. The Kepler data on roap stars demonstrate that their oscillations can easily be missed in ground- based observations. TESS will provide an unprecedented opportunity to obtain high- quality frequency spectra for the majority of the known roap stars and, simultaneously, discover many new members of this class. This will allow us to have a global and much more complete understanding of the properties of roap pulsations and conduct ensemble studies. The known roap stars have periods between 5 and 23 minutes. The 2- min cadence is thus appropriate to discover new members of this class, as well as to characterize the main pulsation modes in the majority of tem. Thus, we propose that all known roap stars are observed with TESS, with priority given to those for which no short- cadence data is yet available. Moreover, we propose a systematic search for members of this class using the 2- minute cadence with the three following objectives: (1) The limits of the roap star instability strip. The excitation mechanism acting on roap stars is still under debate. It is generally accepted that driving by the opacity mechanism acting in the hydrogen ionization region can explain many of the observed pulsations (Balmforth et at 2001). However, this mechanism does not succeed in explaining the exceedingly high frequencies observed in some roap stars, which have, alternatively, been suggested to be driven by turbulent pressure (Cunha et al. 2013). In addition, the theoretical instability strip predicted based on the opacity mechanism (Cunha 2002) seems to have blue- and red- edges that are too hot, when compared to current observations. To make definitive tests on the theoretical models for the excitation of roap stars pulsations it is imperative to know the true limits of the instability strip. That has so far been hampered by the difficulty in finding new objects of this class and by the selection biases employed in most roap ground- based surveys. The TESS mission provides an ideal opportunity to determine the extent of the roap instability strip. To detect roap stars at the limits of the instability strip, approximately 100 stars need to be observed. These were selected based on the following criteria: (1) Stars must be classified as CP2 (chemically peculiar) with enhanced Sr, Cr, Eu, Si; (2) Stars must cover the whole temperature range as evenly as possible; (3) Stars must be reasonably bright (7 9 mag); (4) The field must preferably be uncrowded. (2) A statistically sound sample of roap stars It will be many years before we have another opportunity like the one provided by TESS to take a leap forward in our understanding of chemically peculiar, magnetic stars. In order to increase significantly the sample of known roap stars we propose to observe 1221 roap star candidates in addition to those proposed for objective (1) above. Of these, 40 are stars that have been observed by the KELT survey and whose frequency spectra show evidence for pulsations in the frequency domain of roap stars, and 8 are members of a young cluster (Coma Ber), of which one is located at the hot border of the classical IS (this is 21 Com). Note that a detailed study of the chemical abundances of various A(m)/F stars of this cluster was already published (Gebran et al. 2008). The remaining 1173 stars are from the Michigan Spectral Catalogues volumes 1-5, and have an Ap spectral classification. TESS offers the first opportunity for an unbiased survey of this important class of stars. (3) The non-oscillating Ap stars A long- lasting open question in the context of pulsations in Ap stars is why some Ap stars, known as non- oscillating Ap (noap) stars, do not pulsate. These objects fall within the empirical roap instability strip, and in some cases have been shown to have spectral characteristics and fundamental parameters very similar to known roap stars. With this in mind, a carefully selected sample of 13 noap stars has been identified and given high priority, to clarify whether these stars are pulsating. In addition, from (1) and (2) we will be able to infer the fraction of Ap stars that exhibit rapid oscillations and how that fraction depends on the global properties of the stars. A follow- up spectroscopic ground- based program will be designed to assess whether the difference between roap and noap TESS pulsators is connected to the stars spectral properties.

Length of the time series: The project is well suited to TESS 2- minute cadence observations of limited duration (27 days). The high frequencies that characterize these stars mean that a large number of cycles can be observed even for the relatively short time span. The roap stars are oblique pulsators, and geometric information about their pulsation mode structure needs observations that span at least a full rotation cycle. Since most of these stars rotate with periods less than 27 days, TESS will fulfill this requirement admirably. A longer time series will improve the power spectrum and allow for an even better characterization of the targets. For new roap stars in fields observable for more than 27 days discovered in this survey, we may request changing their observation to the 20- sec cadence mode, when available. Quality of TESS data: Pulsations in the known roap stars have amplitudes in the 0.01-10 mmag range, in the traditional blue filters used in ground- based surveys. The amplitude reduction as a result of the red filter of TESS will be about a factor of 4 compared to these ground- based observations. Then the 1 100 μmag noise level expected over the full TESS magnitude range (3.7-12.2) of the targets considered in this proposal still gives S/N in the 5 100 range for a 1 mmag pulsation, and can still detect pulsations in the brighter stars down to about 10 μmag (see Fig. 1, extracted from the WG4 report). We therefore expect that many new roap stars will be discovered among the targets proposed. Moreover, strict pulsation amplitude limits will be set on the brighter- end targets when no high frequencies are found. With regards to crowding, the frequency range of the roap stars does overlap with those of some solar- like stars and some sdbv stars and variable white dwarfs. But the solar- like variability is at much lower amplitudes and has an easily recognizable pattern, and the sdbv and white dwarfs are all generally much fainter, so crowding will not be a problem for roap stars.

Priorities of the targets: Maximum priority is given to 56 stars previously identified as roap pulsators and 13 stars having very specific spectroscopic signatures that are typical of roap stars, all with absolute ecliptic latitudes equal or greater than 6 degrees. The next priority is given to the 40 stars observed by the KELT survey that are suspected to be roap star pulsators. These stars have been identified from the inspection of the periodograms produced from KELT data for stars with V<10 and B- V<0.5. Within these, priority is given by length of observation, followed by TESS magnitude. The next highest priority is given 8 Ap stars that are confirmed cluster members, ordered by magnitude. Following these two groups, priority will be given to a sample of 91 stars selected to determine the extent of the roap star instability strip. Stars in this sample may be substituted by other similar targets (similar spectral type, similar Teff, and similar crowding), if needed, but the total number should not be significantly smaller than that proposed, otherwise the scientific case will be compromised. Finally, the last group of targets, composed of 1173 Ap stars, is organized by length of observation, followed by TESS magnitude. Fig. 2: Sky coverage of the 56 known roap stars with ecliptic latitudes equal or greater than 6 degrees and 13 additional Ap stars with very specific spectroscopic signatures that are typical of roap stars, but for which no high frequency pulsations have yet been identified (the so- called noap stars). The grey band illustrates the galactic plane and the egg- shaped black feature is the approximate location of the Kepler FOV.

Fig. 2: Sky coverage of Ap targets proposed for the survey in search for new roap stars. Stars are concentrated towards the southern ecliptic hemisphere due to the use of the Michigan Catalogue for the identification of the Ap nature of most of the targets (this catalogue contains stars with declinations < than 5 o and no corresponding catalogue exists for higher declinations). The grey band illustrates the galactic plane and the egg- shaped black feature is the approximate location of the Kepler FOV. Ground-based observations in relation to this proposal: There is no requirement for additional ground- based observations for the stars in this proposal prior to the launch of TESS. Ground- based follow up will be organized in particular for a subset of the stars, aiming at establishing whether systematic spectroscopic differences exist between the roap and noap stars. References: Balmforth, N. J., Cunha, M. S., Dolez, N., et al., 2001, MNRAS, 323, 362 Balona, L. A., Catanzaro, G., Crause, L., et al., 2013, MNRAS, 432, 2808 Balona, L. A., Cunha, M. S., Kurtz, D. W., et al, 2011, MNRAS, 410, 517 Cunha, M. S., Alentiev, D., Brandão, I. M., et al., 2013, MNRAS, 436,1639 Cunha, M.S., 2002, MNRAS, 333, 47 Kurtz, D. W., Cunha, M. S., Saio, H., et al, 2011, MNRAS, 414, 2550 Smalley, B., Niemczura, E., Murphy, S. J., et al, 2015, MNRAS, 452, 3334