Bibcode
Poidevin, F.; Ade, Peter A. R.; Angile, Francesco E.; Benton, Steven J.; Chapin, Edward L.; Devlin, Mark J.; Fissel, Laura M.; Fukui, Yasuo; Gandilo, Natalie N.; Gundersen, Joshua O.; Hargrave, Peter C.; Klein, Jeffrey; Korotkov, Andrei L.; Matthews, Tristan G.; Moncelsi, Lorenzo; Mroczkowski, Tony K.; Netterfield, Calvin B.; Novak, Giles; Nutter, David; Olmi, Luca; Pascale, Enzo; Savini, Giorgio; Scott, Douglas; Shariff, Jamil A.; Soler, Juan Diego; Tachihara, Kengo; Thomas, Nicholas E.; Truch, Matthew D. P.; Tucker, Carole E.; Tucker, Gregory S.; Ward-Thompson, Derek
Referencia bibliográfica
The Astrophysical Journal, Volume 791, Issue 1, article id. 43, 9 pp. (2014).
Fecha de publicación:
8
2014
Revista
Número de citas
10
Número de citas referidas
9
Descripción
Turbulence and magnetic fields are expected to be important for
regulating molecular cloud formation and evolution. However, their
effects on sub-parsec to 100 parsec scales, leading to the formation of
starless cores, are not well understood. We investigate the prestellar
core structure morphologies obtained from analysis of the Herschel-SPIRE
350 μm maps of the Lupus I cloud. This distribution is first compared
on a statistical basis to the large-scale shape of the main filament. We
find the distribution of the elongation position angle of the cores to
be consistent with a random distribution, which means no specific
orientation of the morphology of the cores is observed with respect to
the mean orientation of the large-scale filament in Lupus I, nor
relative to a large-scale bent filament model. This distribution is also
compared to the mean orientation of the large-scale magnetic fields
probed at 350 μm with the Balloon-borne Large Aperture Telescope for
Polarimetry during its 2010 campaign. Here again we do not find any
correlation between the core morphology distribution and the average
orientation of the magnetic fields on parsec scales. Our main conclusion
is that the local filament dynamics—including secondary filaments
that often run orthogonally to the primary filament—and possibly
small-scale variations in the local magnetic field direction, could be
the dominant factors for explaining the final orientation of each core.
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