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|Title:||Possible link between the power spectrum of interstellar filaments and the origin of the prestellar core mass function||Authors:||Roy, A.
Di Francesco, J.
ELIA, Davide Quintino
SPINOGLIO, Luigi Giuseppe Maria
|Issue Date:||2015||Journal:||ASTRONOMY & ASTROPHYSICS||Number:||584||First Page:||A111||Abstract:||A complete understanding of the origin of the prestellar core mass function (CMF) is crucial. Two major features of the prestellar CMF are 1) a broad peak below 1 M<SUB>☉</SUB>, presumably corresponding to a mean gravitational fragmentation scale, and 2) a characteristic power-law slope, very similar to the Salpeter slope of the stellar initial mass function (IMF) at the high-mass end. While recent Herschel observations have shown that the peak of the prestellar CMF is close to the thermal Jeans mass in marginally supercritical filaments, the origin of the power-law tail of the CMF/IMF at the high-mass end is less clear. In 2001, Inutsuka proposed a theoretical scenario in which the origin of the power-law tail can be understood as resulting from the growth of an initial spectrum of density perturbations seeded along the long axis of star-forming filaments by interstellar turbulence. Here, we report the statistical properties of the line-mass fluctuations of filaments in the Pipe, Taurus, and IC 5146 molecular clouds observed with Herschel for a sample of subcritical or marginally supercritical filaments using a 1D power spectrum analysis. The observed filament power spectra were fitted by a power-law function (P<SUB>true</SUB>(s) ∝ s<SUP>α</SUP>) after removing the effect of beam convolution at small scales. A Gaussian-like distribution of power-spectrum slopes was found, centered at α̅<SUB>corr</SUB> = -1.6 ± 0.3. The characteristic index of the observed power spectra is close to that of the 1D velocity power spectrum generated by subsonic Kolomogorov turbulence (-1.67). Given the errors, the measured power-spectrum slope is also marginally consistent with the power spectrum index of -2 expected for supersonic compressible turbulence. With such a power spectrum of initial line-mass fluctuations, Inutsuka's model would yield a mass function of collapsed objects along filaments approaching dN/dM ∝ M<SUP>- 2.3 ± 0.1</SUP> at the high-mass end (very close to the Salpeter power law) after a few free-fall times. An empirical correlation, P<SUP>0.5</SUP>(s<SUB>0</SUB>) ∝ ⟨N<SUB>H<SUB>2</SUB></SUB>⟩<SUP>1.4 ± 0.1</SUP>, was also found between the amplitude of each filament power spectrum P(s<SUB>0</SUB>) and the mean column density along the filament ⟨N<SUB>H<SUB>2</SUB></SUB>⟩. Finally, the dispersion of line-mass fluctuations along each filament σ<SUB>M<SUB>line</SUB></SUB> was found to scale with the physical length L of the filament roughly as σ<SUB>M<SUB>line</SUB></SUB> ∝ L<SUP>0.7</SUP>. Overall, our results are consistent with the suggestion that the bulk of the CMF/IMF results from the gravitational fragmentation of filaments. <P />Appendices are available in electronic form at <A href="http://www.aanda.org/10.1051/0004-6361/201526431/olm">http://www.aanda.org||Acknowledgments:||We are thankful to Prof. Shu-Ichiro Inutsuka for stimulating and enlightening discussions on filaments. We also acknowledge insightful discussions with Patrick Hennebelle and Gilles Chabrier about the origin of the CMF/IMF and the Press-Schechter formalism. This work has received support from the European Research Council under the European Union’s Seventh Framework Programme (ERC Advanced Grant Agreement No. 291294 – “ORISTARS”) and from the French National Research Agency (Grant No. ANR–11–BS56–0010 – “STARFICH”). SPIRE has been developed by a consortium of institutes led by Cardiff Univ. (UK) and including Univ. Lethbridge (Canada); NAOC (China); CEA, LAM (France); IFSI, Univ. Padua (Italy); IAC (Spain); Stockholm Observatory (Sweden); Imperial College London, RAL, UCL-MSSL, UKATC, Univ. Sussex (UK); Caltech, JPL, NHSC, Univ. Colorado (USA). This development has been supported by national funding agencies: CSA (Canada); NAOC (China); CEA, CNES, CNRS (France); ASI (Italy); MCINN (Spain); SNSB (Sweden); STFC (UK); and NASA (USA). PACS has been developed by a consortium of institutes led by MPE (Germany) and including UVIE (Austria); KUL, CSL, IMEC (Belgium); CEA, OAMP (France); MPIA (Germany); IFSI, OAP/AOT, OAA/CAISMI, LENS, SISSA (Italy); IAC (Spain). This development has been supported by the funding agencies BMVIT (Austria), ESA-PRODEX (Belgium), CEA/CNES (France), DLR (Germany), ASI (Italy), and CICT/MCT (Spain).||URI:||http://hdl.handle.net/20.500.12386/23755||URL:||https://www.aanda.org/articles/aa/abs/2015/12/aa26431-15/aa26431-15.html||ISSN:||0004-6361||DOI:||10.1051/0004-6361/201526431||Bibcode ADS:||2015A&A...584A.111R||Fulltext:||open|
|Appears in Collections:||1.01 Articoli in rivista|
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checked on Jun 21, 2021
checked on Jun 21, 2021
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