%AStephens, Ian%AMyers, Philip%AZucker, Catherine%AJackson, James%AAndersson, B.-G.%ASmith, Rowan%ASoam, Archana%ABattersby, Cara%ASanhueza, Patricio%AHogge, Taylor%ASmith, Howard%ANovak, Giles%ASadavoy, Sarah%APillai, Thushara%ALi, Zhi-Yun%ALooney, Leslie%ASugitani, Koji%ACoudé, Simon%AGuzmán, Andrés%AGoodman, Alyssa%AKusune, Takayoshi%ASantos, Fábio%AZuckerman, Leah%AEncalada, Frankie%BJournal Name: The Astrophysical Journal Letters; Journal Volume: 926; Journal Issue: 1 %D2022%I %JJournal Name: The Astrophysical Journal Letters; Journal Volume: 926; Journal Issue: 1 %K %MOSTI ID: 10343966 %PMedium: X %TThe Magnetic Field in the Milky Way Filamentary Bone G47 %XAbstract Star formation primarily occurs in filaments where magnetic fields are expected to be dynamically important. The largest and densest filaments trace the spiral structure within galaxies. Over a dozen of these dense (∼10 4 cm −3 ) and long (>10 pc) filaments have been found within the Milky Way, and they are often referred to as “bones.” Until now, none of these bones has had its magnetic field resolved and mapped in its entirety. We introduce the SOFIA legacy project FIELDMAPS which has begun mapping ∼10 of these Milky Way bones using the HAWC+ instrument at 214 μ m and 18.″2 resolution. Here we present a first result from this survey on the ∼60 pc long bone G47. Contrary to some studies of dense filaments in the Galactic plane, we find that the magnetic field is often not perpendicular to the spine (i.e., the center line of the bone). Fields tend to be perpendicular in the densest areas of active star formation and more parallel or random in other areas. The average field is neither parallel nor perpendicular to the Galactic plane or the bone. The magnetic field strengths along the spine typically vary from ∼20 to ∼100 μ G. Magnetic fields tend to be strong enough to suppress collapse along much of the bone, but for areas that are most active in star formation, the fields are notably less able to resist gravitational collapse. %0Journal Article