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Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX :...

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Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G. Grenoble - France
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Page 1: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Alain KLOTZ : C.E.S.R. Toulouse - France

Nicolas LODIEU : A.I.P. Postdam - Germany

Emmanuel CAUX : C.E.S.R. Toulouse - France

Jean-Louis MONIN : L.A.O.G. Grenoble - France

Page 2: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Characteristics of the Serpens cloudStar forming regionGalactic location : l=31.5° b=5.4°Apparent dimensions : ~ 20 arcmin for Av>5Central core : SVS 20 and its nebula

Estimated distance : 259 +/- 37 pc (Straizys et al. 1996) Extinction : >30 for radius < 1.5 arcmin from SVS 20Identified young stellar objects : > 100 (Kaas 1999, …)Estimated age : < 107 years (Giovannetti et al 1998, …)

High Background contamination1 low mass star 0.05 Msun identified (Lodieu et al. 2002)

Page 3: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Goal of this study

Plot the mass function specially for stars lighter than 0.5 Msun

(the “low mass” slope of the mass function is almost unknown).

Find new brown dwarfs candidates.

Establish a high resolution Av chart of the cloud in order toconstraint spectral types (and mass) of individual stars.

Determination of Av, distance modulus and mass for all stars from JHK magnitudes using (J-H)/(H-K) and K/(H-K) diagrams.

Page 4: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.
Page 5: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

ObservationsJHK 2x5 arcmin images from Pic du Midi (TBL-MOICAM)JHK 6x11 arcmin images from ESO (NTT-SOFI)JHK spectra from ESO (VLT-ISAAC)

JHK images from Pic-du-Midi-TBL, allowed us to identifiedan interesting field to observe with ESO-NTT.

JHK images from ESO-NTT allowed us to identify very lowmass star candidates.

JHK spectra from ESO-VLT allowed us to find a very lowmass star (Ser-BD 1) embedded in the Serpens cloud.

A three step strategy

Page 6: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

-0.2 0 0.2 0.4 0.6

-10

-5

0

5

10

15

20

H-K

K

MD

=1

8

MD

=1

2

MD

=1

1

MD

=1

3

-0.2 0 0.2 0.4 0.6-0.5

0

0.5

1

1.5

J-H

Av=

6.5

Av=

6.7

Av=

4.9

Av=

4.7

Extinction and distancemodulus determination (1)

From NTT-SOFI images:A total of ~9000 stars measured~ 2300 stars measured in JHK~ 3000 stars measured in HK

For each star measured in JHK

Av is measured from colour/colour diagram.MD is measured from colour/magnitude diag.

Three types of class are considered:

dwarfs (blue on diagrams)giants (red on diagrams)young 3.106 yr (magenta on diags.)

Right : an example for a star J=18.5, H=17.5, K=17. Thereare four couples of solutions (Av, MD) for a cool young

(4.7, 13), a cool dwarf (4.9, 11), a hot giant (6.5,18) and a hotdwarf (6.7, 12). Uncertainties are 1.5 for Av and 1.5 for MD.

Page 7: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

For each star measured in HK

J magnitude is estimated supposing the star is in the middle of the reddening band of the colour/colour diagram:

slope comes from Rieke & Lebosky (1985)Aj/Av=0.282, Ah/Av=0.175, Ak/Av=0.112

For each star outside the reddening band

A star having a red colour excess is considered in the Serpens cloud

J = H + slope*(H-K) + 0.15

Extinction and distancemodulus determination (2)

Page 8: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Spatial distribution of extinctionBuilding the Av chart of the field

•The observed field is divided in cells of 15x15 arcsec.

•In each cell, an average value of Av is computed from Av previously computed from stars,supposed to be cool dwarfs, measured in JHK or HK bands(method adapted from Lada et al. 1994).

•Cells which are empty of JHK or HK stars, will be computed from an empirical relation giving Av from the density of stars in the K band. This relationis established from cells treated rigorously.

Av chart. White is for Av>60. JHK image from NTT-SOFIDark is for Av~5.

Page 9: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Spectral types and mass determination (1)

(Av,MD) determination for stars lead also to the estimation of possible spectral types and masses. A maximum of 6 solutions are possible. One must select the “most” probable solution:

The simplified algorithm of the choice of the spectral class is:

A young star if its MD is compatible with Serpens cloud and if Av is not higher than background stars.

A giant star if its MD is less than 14 (maximum distance allowed for giants at this galactic latitude).

A cool dwarf if its Av is not too lower compared to the mean Av of the corresponding cell (expected if its distance modulus is lower or equal to that of Serpens cloud).

Else the star is assigned as a hot dwarf.

A method for a direct assignment

N.B. The majority of stars are assigned as cool dwarfs

Page 10: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Spectral types and mass determination (2)

Advantages of that method

Disadvantages of that method

Good accuracy for low and very low mass stars (M<0.5 Msun)Possibility to extract a mass function for low masses.

Individual assignments of (Av,MD, spectral type, mass)Finding peculiar stars is easy. A brown dwarf candidate was found by this way.

High precision photometry is needed0.05 mag error typically change 1.5 mag for Av and 1.5 mag for MD.Three JHK magnitudes are needed for a non ambiguous determination.

Poor accuracy for masses between 0.8 and 1.5 Msun

Comes from the “elbow” around M0 spectral types in colour/colour diagr. The choice of the most probable solution is ambiguous.

Page 11: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Luminosity functionDerived from stars observed in JHK bands

without IR excess & age=3 106 yr & mass < 0.8 Msun

10 12 14 160

1

2

3

4

5

6

7

8

9

K apparent magnitude

nu

mb

er

of s

tars

in th

e c

lou

d

Luminosity function

2 4 6 80

2

4

6

8

10

12

K absolute magnitude

nu

mb

er

of s

tars

in th

e c

lou

d

Luminosity function

202 stars were found at the distance modulus (+/- 1) of the Serpens cloud:28 stars (only !) fit the conditions (see upper histograms)17 other stars have an infrared colour excess11 other stars have only HK magnitude55 other stars have a blue colour excess91 stars were assigned as classical dwarfs

Page 12: Alain KLOTZ : C.E.S.R. Toulouse - France Nicolas LODIEU : A.I.P. Postdam - Germany Emmanuel CAUX : C.E.S.R. Toulouse - France Jean-Louis MONIN : L.A.O.G.

Mass function & conclusionDerived from stars observed in JHK bands

without IR excess & age=3 106 yr & mass < 0.8 Msun

0 0.2 0.4 0.6 0.80

1

2

3

4

5

6

7

8

masse

nu

mb

er

of s

tars

in th

e c

lou

d

Mass function

Not enough stars to concludeabout the slope of low masspart of the mass function

Location of brown dwarfs candidates(Ser-BD 1 was discovered

by this method).

There is not a dramatic fallof the mass function for masseslower than 0.5 solar mass.

This work is still in progress ! A refinementof the method will allow to growth the

number of stars to include in the mass function...


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