2013:reasearch
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| overlaid on the the 22 GHz continuum map imaged with the VLA (black image and white contours). | overlaid on the the 22 GHz continuum map imaged with the VLA (black image and white contours). | ||
| Colors denote line-of-sight velocities, with blue indicating blue-shifted emission and red indicating red-shifted emission. | Colors denote line-of-sight velocities, with blue indicating blue-shifted emission and red indicating red-shifted emission. | ||
| - | The sizes of the circles scale with the flux density. | + | The sizes of the circles scale with the flux density. The ellipses represent the disk planes surrounding the two young stars IRS1a and IRS1b, |
| - | The ellipses represent the disk planes surrounding the two young stars IRS1a and IRS1b, | + | |
| resolved by the EVN, with the solid lines indicating the near-side and the dashed lines the far-side of the disks. | resolved by the EVN, with the solid lines indicating the near-side and the dashed lines the far-side of the disks. | ||
| {{: | {{: | ||
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| + | Massive Star Forming Regions and Magnetic Fields | ||
| + | |||
| + | Gabriele Surcis, Huib Jan van Langevelde, and Ciriaco Goddi together with colleagues from Sweden, Spain, Mexico, | ||
| + | and South Korea observed the polarized emission of 22 GHz water masers around the massive young stellar objects (YSOs) | ||
| + | W75N-VLA2 and W75N-VLA1. The two massive YSOs are separated by just 1300 astronomical units and are at two | ||
| + | different evolutionary stages, i.e., VLA1 is the most evolved and VLA2 the least evolved. The interferometric | ||
| + | observations showed at 1~au scale that while the water masers distribution and the magnetic field around VLA1 have | ||
| + | not changed since 2005, the shell structure of the masers around VLA2 is still expanding and increasing its | ||
| + | ellipticity. Furthermore, | ||
| + | direction of the major-axis of the shell-like structure and it is now aligned with the magnetic field in VLA1. | ||
| + | This confirm that the water masers around VLA2 are tracing the evolution from a non-collimated to a collimated | ||
| + | outflow. | ||
| + | |||
| + | Gabriele Surcis and Huib Jan van Langevelde together with Wouter Vlemmings (Chalmers University of Technology), | ||
| + | Busaba Hutawarakorn Kramer (MPIfR), and Anna Bartkiewicz (Nicolaus Copernicus University) | ||
| + | continued their work on measuring magnetic fields morphology close to massive YSOs (au scale) by using 6.7 GHz | ||
| + | methanol masers. The group measured the magnetic field morphology towards eight new massive YSOs. These sources | ||
| + | are part of a large sample of massive YSOs, the so-called flux-limited sample, that is composed of 31 sources. | ||
| + | A preliminary statistical analysis of the results obtained from the first 19 sources reveals evidences that the | ||
| + | magnetic fields around massive YSOs are preferentially oriented along the molecular outflow. | ||
| + | Furthermore, | ||
| + | morphology of the magnetic field at au scale around the massive YSO IRAS20126+4104 by observing the polarized | ||
| + | emission of the 22 GHz water masers and the 6.7 GHz methanol masers. The orientation of the magnetic field | ||
| + | derived from the masers agrees with the S-shaped morphology on larger scale by using the dust-polarized emission | ||
| + | at 350~\mu~m. | ||
| + | |||
| + | --------------------------- | ||
| + | Figures captures. | ||
| + | |||
| + | figure_1a.eps, | ||
| + | and VLA2 (right panel). The reference position is $\alpha_{2000}=20^{\rm{h}}38^{\rm{m}}36^{\rm{s}}\!.435$ and | ||
| + | $\delta_{2000}=42^{\circ}37' | ||
| + | according to their peak flux density. The linear polarization vectors, scaled logarithmically according to | ||
| + | polarization fraction, are overplotted. In the bottom-right corner of both panels the error-weighted orientation | ||
| + | of the magnetic field ($\Phi_{\rm{B}}$) is also reported; the two dashed segments indicate the uncertainties. The | ||
| + | ellipse drawn in the right panel is the result of the best fit of the water masers. The estimated values of the | ||
| + | magnetic field strength are also shown in both panels next to the corresponding water maser. | ||
| + | |||
| + | figure_2a.eps, | ||
| + | the polarized dust emission at 350~$\mu$m, whose continuum emission is in the background. The white box indicates | ||
| + | the position of the right panel. | ||
| + | Right panel: methanol (triangles), | ||
| + | | ||
| + | $\delta_{2000}=41^{\circ}13' | ||
| + | $\sim$1000~au ($\rm{PA_{disk}}=53^{\circ}\pm7$\d. The red and blue lines indicate the red- and blue-shifted lobes | ||
| + | of the jet, respectively. The thick green segments represent the magnetic field direction determined from the | ||
| + | polarized methanol and water maser emissions. The green dashed segments represent the magnetic field direction | ||
| + | determined from the linearly polarized emission of OH masers (Edris et al. 2005, A&A, 434, 213). | ||
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| + | {{: | ||
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2013/reasearch.1415953829.txt.gz · Last modified: 2014/11/14 08:30 by paragi