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Activity, rotation and weather in Ultracool Dwarfs First NAHUAL meeting, La Gomera Eduardo L. Martín, IAC Outline • • • • • • Introduction on brown and ultracool dwarfs Rotation observations H observations X-ray and radio observations Weather observations Final Remarks The 1997 census of the solar neighborhood Henry 1998 in BDExp Martin et al. 2005, RevMex AA The 2004 census Martin et al. 1997,1998,1999; Kirkpatrick et al. 1999; 2000; Burgasser et al. 2000,2001; Leggett e al. 2001; Geballe et al. 2002; Cushing et al. 2002 Ultracool dwarfs (L, T) • Two new spectral classes have been defined for ultracool dwarfs. • The L class is characterized by weak or absent TiO, strong FeH, and huge alkali lines. Teff~2200K-1400K. • The T class is characterized by CH4. Teff<1400K. • A 35MJupiter evolves from M-type at 10 Myr to T type at 1 Gyr. Kumar 1963; D’Antona & Mazzitelli 1995; Saumon et al. 1996; Chabrier & Baraffe 2000 Brown dwarfs • A brown dwarf is defined primarily by its mass, irrespective of how it forms. • The low-mass limit of a star corresponds to the minimum mass for stable Hydrogen burning. • The HBMM depends on chemical composition and rotation. For solar abundances and no rotation the HBMM=0.075MSun=79MJupiter. • The lower limit of a brown dwarf mass is at the DBMM=0.012MSun=13MJupiter. Kippenhahn 1970; Martin et al. 1997; Basri et al. 2000; Reid et al. 2002. Rotation • Projected rotational velocities (vsini) have been measured in 40 field dwarfs M9-L6, using the rotational broadening of atomic and molecular lines with Keck/Hires. • Average vsini=21km/s, corresponding to Prot~6hr • Rotation makes the star more degenerate, and increases the HBMM. NIR high-resolution spectroscopy of a T dwarf. • Eps Ind B is the nearest T dwarf known (d=3.6 pc), Scholtz et al. 2003. • Smith et al. 2003 have obtained R=50,000 spectroscopy with Phoenix at Gemini South. • Many spectral features for accurate radial velocity and rotational broadening determination. Joergens et al. 2003 Evolution of rotational periods • Acceleration of the rotation of brown dwarfs due to contraction during the first 50-100 Myr. • Magnetic braking due to interaction with a disk may play a role. • Lack of efficient braking during most of dwarf’s evolution. Gizis et al. 2000; Zapatero Osorio et al. 2002 H activity • H is a diagnostic of hot plasma. It can be caused by a chromosphere or by an accretion boundary layer (CTTS activity). • The average H emission level in young BDs is higher than in the older counterparts of the solar vicinity. Accretion rates are very low. Field M,L,T Dwarfs • The general trend is that H activity level declines with decreasing temperature • A few very low-mass dwarfs have extraordinary persistent H emission • Interacting binaries? Liebert et al. 1999; Martin 1999; Reid et al. 2001; Martin & Ardila 2001 H flares • Duty cycle 1-3% • Sometimes HeI, KI, NaI, OI and CaII emission, and blue veiling • Energy release can be a few percent of bolometric luminosity Mohanty & Basri 2002; Meyer & Meyer-Hofmeister 1999 H-rotation connection breaks down • For SpT>M7 there is no connection between rotation and activity. • In the neutral atmospheres of L dwarfs the magnetic fields may be decoupled from convective motions. Fleming et al. 1993, 2000; Mokler & Stelzer 2002; Martin & Bouy 2002 Berger et al. 2001, Nature Radio Observations • Very Large Array observations at 8.5 GHz of LP944-20 • Quiescent and flaring emission • B~5G from synchrotron theory. • Duty cycle ~ 2.5% Guedel & Benz 1993 ApJ Violation of the Guedel-Benz Relation • Coronal activity in G,K,M stars LR~LX/1015.5 Hz-1 • Measured radio flux is at least 4 orders of magnitude higher than predicted. Berger 2002, ApJ Yet Another Surprise! • BRI0021-0214 is another inactive fast rotating dM9.5 with persistent and flaring radio emission. • It violates the GuedelBenz relation by a factor of >1700 Radio Emission in an L dwarf • 2MASS 0036+18, L3.5 • Unusual flare profile and variable persistent emission • No evidence of H emission Radio Activity does not Decline in Very Low-Mass Dwarfs • Contrary to H activity, there is not a clear decline of radio emission for spectral types cooler than M8. The decline may be shifted to cooler temperatures. • Radio emission requires magnetic fields B~5-20 G, similar to Jupiter’s Goldman et al. 2004 Weather observations • VLT/ISAAC and IRTF/Spex time series observations of late L and T dwarfs. • No variability detected larger than 5% Final Remarks • Coronal activity in brown dwarfs is scarce. Possibly less RV jitter. Weather may also not be a problem. • H activity dies off quickly for SpT>M8, with a few exceptions (interacting binaries?). NAHUAL can test this possibility. • Ultracool dwarfs tend to be fast rotators. Could this limit the RV accuracy? • Is activity switching from “stellar” to “planetary” mode in the ultracool dwarfs? NAHUAL could be used to measure zeeman splitting.