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The evolution of brown dwarf's infrared spectroscopic properties IR and Sub-mm Spectroscopy - a New Tool for Studying Stellar Evolution SpS1, Session 8, Thursday Aug 6th, 9h-9h35 France Allard & Isabelle Barrafe Directrices de Recherche, CNRS Centre de Recherche Astrophysique de Lyon
Burning: from VLM stars to planets stars brown dwarfs Planemos (planetary mass objects) = 3.5 10 6  K = 1 10 6  K = 2.4 10 6  K
MRR from planets to  solar type stars Chabrier et al. 2009, CS15 proceedings ,[object Object],[object Object],[object Object],[object Object],OGLE-TR-122 (M=0.085 M  ) Baraffe et al. 1998 Chabrier & Baraffe, ARAA 2000 Eclipsing binaries : rapid rotators & active Slower contraction due to magnetically driven inhibition of  convection and spot coverage? Eclipsing brown dwarf:  T eff  reversal : Stassun et al.  (2006) [ H  ]a = 7  [ H  ]b : Reiners et al. (2007) layered or oscillatory  convection? 5Z  , 9 M jup
Evolution of the surface temperature ,[object Object]
Atmospheric composition across the MLT
 
 
2200K 1800K 1000K Teff from  M   --->   L   ----->   T  dwarf Baraffe et al. ‘1998,2003; Chabrier et al. 2000 ,  Allard et al.  2001 Marley et al. 2000, 2002; Burrows et al. 2003, 2006 Formation and settling of « dust » in brown dwarf atmospheres
 
Gravity vs surface temperature ,[object Object]
H 2 O temperature dependence
0.1 Myr   log 10  g = 2.5 log 10  g =  3.0 H 2 ! Uncertainties at young ages!
Clouds in brown dwarfs Fergley & Lodders, Astrophysics Update 2,  edited by John W. Mason. ISBN 3-540-30312-X.  Published by Springer Verlag, Heidelberg, Germany, 2006, p.1 http://arxiv.org/abs/ astro-ph/0601381
Ruiz, Leggett & Allard (ApJ 491, L107, 1997)
Forsterite detected in BDs? ,[object Object],Cushing et al  (2006)
Effects of grains on atmosphere profiles: « green house » effect which heats up the outer layers
 
[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object]
[object Object],[object Object],[object Object],[object Object],[object Object]
Dynamical Transport N 2  and CO is transported from inner/warmer regions of the atmosphere, depleting NH 3  (N 2 ) and CH 4  (CO) Saumon et al. (2003)
2D RHD simulations  of cloud formation  in brown dwarf atmospheres ,[object Object],W350 x H80 km 2   over 36 hours  Gravity Waves !!!
3D Radiation Hydrodynamics Freytag & Allard 2009 3D radiation hydrodynamical simulation of a brown dwarf (T eff =1500K, logg=5, type L) atmosphere cube (340 x 340 x 113 km 3 ). Runtime: 1.8 hours stellar time (about 3 months on 6 processors). Time step: 0.18 sec (6 hydro steps, 1 viscosity step, 1 source step, 1 radiation step). Color coded (right) is the dust concentration (Mg 2 SiO 4 ), and (left) the entropy of the convective zone.  The model does not include rotation effects (next step when the model is relaxed). Awaits financial support.
Web Simulator ONLINE ! ,[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],[object Object],http://phoenix. ens-lyon . fr/simulator NOW OPEN!
TVLM513-46546 Hallinan et al. (ApJ 663, L25, 2007) Time series of the radio emission detected with the VLA from the  M9  dwarf TVLM 513-46546. Every  1.958 hrs  a periodic pulse is detected when extremely bright beams of radiation originating at the poles sweep Earth when the dwarf rotates. This dim dwarf is producing  radio emission which is thousands of times brighter  than any ever detected from the Sun. CREDIT: Hallinan et al., NRAO/AUI/NSF Animated gif of the radio emission from the  M9  dwarf TVLM 513-46546 detected with the VLA at  8.44 GHz . The time between each bright pulse corresponds to  1.958 hrs , which is the  period of rotation of the dwarf . CREDIT: Hallinan et al., NRAO/AUI/NSF
Maser radio emission of Jupiter ,[object Object],[object Object]

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Brazil1

  • 1. The evolution of brown dwarf's infrared spectroscopic properties IR and Sub-mm Spectroscopy - a New Tool for Studying Stellar Evolution SpS1, Session 8, Thursday Aug 6th, 9h-9h35 France Allard & Isabelle Barrafe Directrices de Recherche, CNRS Centre de Recherche Astrophysique de Lyon
  • 2. Burning: from VLM stars to planets stars brown dwarfs Planemos (planetary mass objects) = 3.5 10 6 K = 1 10 6 K = 2.4 10 6 K
  • 3.
  • 4.
  • 6.  
  • 7.  
  • 8. 2200K 1800K 1000K Teff from M ---> L -----> T dwarf Baraffe et al. ‘1998,2003; Chabrier et al. 2000 , Allard et al. 2001 Marley et al. 2000, 2002; Burrows et al. 2003, 2006 Formation and settling of « dust » in brown dwarf atmospheres
  • 9.  
  • 10.
  • 11. H 2 O temperature dependence
  • 12. 0.1 Myr log 10 g = 2.5 log 10 g = 3.0 H 2 ! Uncertainties at young ages!
  • 13. Clouds in brown dwarfs Fergley & Lodders, Astrophysics Update 2, edited by John W. Mason. ISBN 3-540-30312-X. Published by Springer Verlag, Heidelberg, Germany, 2006, p.1 http://arxiv.org/abs/ astro-ph/0601381
  • 14. Ruiz, Leggett & Allard (ApJ 491, L107, 1997)
  • 15.
  • 16. Effects of grains on atmosphere profiles: « green house » effect which heats up the outer layers
  • 17.  
  • 18.
  • 19.
  • 20. Dynamical Transport N 2 and CO is transported from inner/warmer regions of the atmosphere, depleting NH 3 (N 2 ) and CH 4 (CO) Saumon et al. (2003)
  • 21.
  • 22. 3D Radiation Hydrodynamics Freytag & Allard 2009 3D radiation hydrodynamical simulation of a brown dwarf (T eff =1500K, logg=5, type L) atmosphere cube (340 x 340 x 113 km 3 ). Runtime: 1.8 hours stellar time (about 3 months on 6 processors). Time step: 0.18 sec (6 hydro steps, 1 viscosity step, 1 source step, 1 radiation step). Color coded (right) is the dust concentration (Mg 2 SiO 4 ), and (left) the entropy of the convective zone. The model does not include rotation effects (next step when the model is relaxed). Awaits financial support.
  • 23.
  • 24. TVLM513-46546 Hallinan et al. (ApJ 663, L25, 2007) Time series of the radio emission detected with the VLA from the M9 dwarf TVLM 513-46546. Every 1.958 hrs a periodic pulse is detected when extremely bright beams of radiation originating at the poles sweep Earth when the dwarf rotates. This dim dwarf is producing radio emission which is thousands of times brighter than any ever detected from the Sun. CREDIT: Hallinan et al., NRAO/AUI/NSF Animated gif of the radio emission from the M9 dwarf TVLM 513-46546 detected with the VLA at 8.44 GHz . The time between each bright pulse corresponds to 1.958 hrs , which is the period of rotation of the dwarf . CREDIT: Hallinan et al., NRAO/AUI/NSF
  • 25.