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BPS2016 Mercator Telescope Prof. Hans Van Winckel Instituut voor Sterrenkunde KU Leuven

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Page 1: Mercator Telescope

BPS2016

Mercator Telescope

Prof. Hans Van WinckelInstituut voor SterrenkundeKU Leuven

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BPS2016

European Southern Observatory La Silla-Paranal observatory

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BPS2016

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BPS2016

Why Mercator ?

E-ELT2014

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Mercator: Niche in observational astrophysics

Provides complementary unique possibilities to international (& space) facilities:TIMES-SERIES over a wide range of scales and cadencesRequirements: World-class instruments: instrument development programme Operational model: Pooled observations with priority driven scheduling. Userfriendly robust operational environment

: Big Science envelope

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Outline

-Mercator for experimental astrophysics-Instruments: HERMES-Instruments: Maia-Mercator Operations-Science results

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• Owned and operated by the Institute of Astronomy, KU Leuven

• In operation since 2001• Built in collaboration with the Observatoire de Genève

(Euler twin, Chile)• Roque de los Muchachos Observatory

• La Palma (Canary Islands, Spain)• Altitude: 2400 m• Prime site for astronomical observations in Europe• Large international collection of telescopes

The Mercator telescope

Mercator

Gran Telescopiode Canarias

Magic Cherenkov telescopes

Nordic Optical Telescope

William Hershel Telescope

Dutch & Swedish Solar Towers

Mercator

Isaac Newton Telescope

J. Kapteyn TelescopeLiverpool Telescope

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Mercator telescope optics

Φ 1.2 m

Ritchey-Chrétien optics: • 2 Hyperbolic mirrors

flat focal plane free of coma and spherical aberration

• Combined focal length: f 14.4 m (f/12)

• Central obscuration (7.5%)

M2

M1

Focal plane

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The Mercator telescope• Altitude-azimuthal telescope mounting:

To track targets during observation (sync. with daily earth rotation)

• 3 rotation axes: Azimuth Elevation Instrument rotation

• High-precision mechanisms:・ 9000 kg moving mass・ Blind pointing accuracy: 3 – 4 arcsec・ Closed-loop tracking precision:

< 0.1 arcsec

0.1 arcsec arctan 0.5 mm / 1 km

Azimuth

Elevation

Field rotation

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Why a high-resolution spectrograph ?

Radial velocity : (λ – λ0) / λ0= velocity/cHigh resolution: 85 000 corresponds to 3.5 km/s in VHigh stability to allow 10 m/s accuracy. Wide spectral domain helps

Strength of line = f(Teff, log(g), chemical composition)Wide spectral coverage ! Good sampling required

S/N: small telescoperequiresefficientinstrument

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HERMES-Consortium: Kick-off 19/01/2005 Science start: 01/06/2009

ROBco-i: H. Hensberge, Y Fremat

IvS-KULco-i: C. Waelkens

HERMESIAA-ULBco-i: A. Jorissen

Observatoire de GenèveLandessternwarte Tautenburgco-i: H. Lehman

Project Engineer: Gert RaskinPI: Hans Van Winckel

FNRS

Lotto

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HERMES: Niche in the telescope-market

Time series in radial velocity and in individual spectral lines, high S/N spectra of fainter stars: robust, efficient, high-resolution, spectrograph on Mercator =HERMES: High-Efficiency and Resolution Mercator Echelle Spectrograph

Pooling of HERMES observations with priority driven scheduling. All HERMES consortium nights are mainly (80%) scheduled from pool.

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Hermes: white pupil Design

F/10

15cm beam

R2.70blaze:69.7o

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Spectrograph room...

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Hermes Design

80 μm

300μm

60 μm

white lightcalibration light (ThAr,Ne)

2.15 arcsec/fibre2.5 arcsec/fibre

double slicer

acclimatisation !! +/- 0.01 K

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Software

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BPS2016

PR slide...

more details: PhD Gert Raskin

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Radial Velocity Stability

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First 7 years of science data: some numbersOn 15/5/2016 there were:

225904 fits files of which 67409 science exposures 5.7 Tb data (raw+reduced)

All data quicklook (on site) + fully reduced in Leuven + distributed rsync

62 science programmes (excluding the Spanish allocation, calibration institutes numbers)

References to Raskin et al., 2011, A&A 526, 69: 154 citations

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Complementary with space: the Kepler field in HERMES pointings

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MAIA 3-arm camera3 arms: U, V+G and R filtersUnique Frame Transfer CCD: 3x2K Fast-photometry possible.Full Frame Frame transfer: 20sec.Commissioning: April-May 2013

See Raskin et al., 2013, on toledoProsperity: Conny Aerts

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MAIA 3-arm camera: Frame Transfer3x2K frame transfer CCDs of the late Eddington mission0.28" per pixel1 controller so windowing is equal in all channels, exposure timesare multiplications of a given time

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Studying and exploiting stellar variability with MAIA

MAIA: identify pulsation modes from pulsation

amplitude ratiosG

R

UPulsation amplitudes depend on wavelength and pulsation mode

l=3, m=0 l=3, m=2 l=3, m=3

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Operational Model :Requirements: Robust (Telescope, Instruments) Easy to use Direct evaluation of quality Optimal monitoring schemes Science graded pipeline

so....: lots of software (MOCS, MESA, DRS (release 6))

Programmes: Phase I, Phase II converted into DB

Trouble Shooting: Night Report + fast feedback (7/7) Weekly skype conferences with whole team

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Current-Future Developments

Towards a new Telescope Control System based on soft-PLC, industrial standardisation, integrated approach. Proof of concept for control international instrument programmes (ESO E-ELT-METIS)

New fiber link for HERMES

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Important Science themes: Binary interaction physics

Binary channels plagued with uncertainties

Binary evolution

≠Singe star evolution

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Theory versus Observations

Izzard, 2010; Jorissen, 2015,Escorza 2016

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HERMES: binary star programme

Long timeseriesIntense timeseries

Not vacuum: 7yr stability is ~ 80 meter/second Ideal complement to (space) projects and larger infrastructure

Unique science is possibleHD5306. P=8380 days 15306

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Science Exploitation Examples

Heart-beat stars

At periastron

Orbits are stronglyelliptical

e.g.Beck et al., 2014, A&A564, 36; 2012, Nature 481, 55

Kepler Space Photometry + HERMES spectroscopy: Giant Binary stars in action

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PNe: first wide binaries detected: LoTr5Companion:- rapidly rotating s-process enhanced companion- very hot WD- Halo PNe

Van Winckel et al., 2014, A&A 563, L10

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Long-Period sdB

- core He post-RGB stars with tiny envelope- wide binaries are now being detected- gravitational redshift

Vos et al., 2012; 2013, 2015

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Radialvelocity(km/s)

Phase

BD+29 3070 BD+34 1543 Feige87

P=1254 d 972 d 938 d

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Long-period sdB- e - problem similar than post-AGB

- e-pumping mechanisms are needed *asymmetric RLOF * disc pumping by discs * included in MESA binary module

Vos et al, 2015

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Binary processes: BD+46.422. Period=140.7 d

Gorlova et al., 2012; Bollen et al. 2016

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Detailed studies of Interaction processesIRAS19135+3937

Kepler lightcurve: very smoothP is orbital period

Gorlova et al., 2015; Bollen et al. 2016

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Why Mercator ?

Niche in experimental astrophysicsThanks to: - instrument development programme (HERMES,Maia) - technology development programme (TCS, fibre link) - adequate operational model

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Only possible thanks to (Local) Team

Saskia Prins

Jesus Perez Padilla Florian Merges

IvS Mercator Team:CCI: Christoffel WaelkensProj Scientist: Hans Van WinckelProj. Engineer: Gert RaskinPhD student Wim PessemierMech. Johan Morren

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Hermes GR

Thinkshop 2013

HERMES observing

Thank you.