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AMI-LA radio continuum observations of low mass young stars: target sample for e-MERLIN legacy project

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Title: AMI-LA radio continuum observations of low mass young stars: target sample for e-MERLIN legacy project


1
AMI-LA radio continuum observations of low mass
young stars target sample for e-MERLIN legacy
project
  • Rachael Ainsworth
  • Dublin Institute for Advanced Studies
  • YERAC 2011

2
Introduction
  • 16 GHz radio continuum observations of target
    sample for the e-MERLIN legacy project on the
    morphology and time evolution of thermal jets
    associated with low mass young stars
    (Rodriguez).
  • I will draw correlations between the radio
    luminosity and a number of global properties for
    these systems.
  • These correlations along with the spectral
    indices for these sources will help place limits
    on the physical mechanisms responsible for the
    radio emission.
  • Future work e-MERLIN

3
Protostellar Evolution
  • Evolutionary Indicators (Hatchell 2007)
  • Bolometric temperature
  • Class 0 Tbol lt 70 K, Class I 70 lt Tbol lt 150 K
  • Ratio of submm to bolometric luminosity
  • Lbol/Lsmm gt 3000
  • Ratio of Spitzer IRAC to submm emission
  • F3.6/F850 gt 0.003

4
Bremsstrahlung
  • A form of thermal emission that comes from gas
    which has been ionized.
  • Atoms in the gas become ionized when their
    electrons become stripped or dislodged.
  • This results in charged particles moving around
    in an ionized gas.
  • As this happens, the electrons are accelerated by
    the charged particles, and the gas cloud emits
    radiation continuously.
  • Often called called "free-free" emission because
    it is produced by free electrons scattering off
    ions without being captured.

5
Spectral Indices
Partially optically thick
Optically thick
Optically thin
S? ?2
S? ?0.6
S? ?-0.1
6
Emission Mechanisms
  • Ionized spherical stellar winds (Panagia Felli
    1975)
  • Ionized collimated winds (Reynolds 1986)
  • Both models predict a correlation between the
    radio luminosity and the rate of stellar mass
    loss,
  • and a 0.6, where a is the spectral index
    defined as

7
The Sample
L1448, HH 7-11, L1551, L1527, HH 1-2, HH 26 IR,
HH 111, NGC 2264, Serpens, L723, L1251
8
L1448
9
HH 7-11
10
Results
11
Radio Luminosity with Bolometric Luminosity
  • (Scaife 2011)
  • logL1.8 cm (mJy kpc2) -(1.74 0.18)
    (0.510.26)logLbol(L?)
  • logL1.8 cm (mJy kpc2) -1.44
    0.60logLbol(L?)

12
Radio Luminosity withEnvelope Mass
  • (Scaife 2011)
  • logL1.8 cm (mJy kpc2) -(2.23 0.65)
    (0.680.62)logMenv(M?)
  • logL1.8 cm (mJy kpc2) -2.26
    1.21logMenv(M?)

13
e-MERLIN
  • Image the jet launch zone to look for clues as
    to how jets from young stars are generated.
  • Measure the strength and direction of the
    magnetic field in the jet launch zone.
  • Capabilities include
  • Observing bands at 1.3-1.8 GHz, 4-8 GHz, 22-24
    GHz
  • Resolution 10 to 150 mas
  • Total bandwidth 4 GHz
  • Sensitivity 1 µJy
  • Astrometry, polarimetry, spectroscopy
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