Abstract:Context. It is still largely debated whether magnetic fields play a key role in dynamically shaping the products of the star formation process. For example, in magnetized protostellar formation models, magnetic braking plays a major role in the regulation of the angular momentum transported from large envelope scales to the inner envelope, and is expected to be responsible for the resulting protostellar disk sizes. However, non-ideal magnetohydrodynamic effects that rule the coupling of the magnetic field to t… Show more
“…Such high values seem inconsistent with the fiducial value if the interstellar cosmic rays flux is responsible for the gas ionization, as it should be efficiently attenuated while penetrating into the dense cores (Padovani et al, 2018). The observations of Cabedo et al (2022) also show the CRs ionization rate is increasing at small envelope radii, toward the central protostellar embryo. Several theoretical works have investigated the role of shocks at the protostellar surface and magnetic mirroring within the jets as efficient forges to accelerate locally low-energy cosmic rays, and their role in increasing the ionization rate of the shielded protostellar material (Padovani et al, 2015;Silsbee et al, 2018;Fitz Axen et al, 2021;Padovani et al, 2021).…”
Section: Fraction Of Ionized Gasmentioning
confidence: 89%
“…The role of the magnetic field in setting the disk size in B335 has also been discussed in subsequent studies (Bjerkeli et al, 2019;Imai et al, 2019;Yen et al, 2019). However, new observations by Cabedo et al (2022) suggest that the gas at small envelope radii is strongly ionized in B335 and points toward conditions typical of ideal MHD. It may very well be that the star-disk building phase consists in a succession of non-ideal and ideal MHD conditions in the "life of the protostar."…”
Section: The Formation Of Disksmentioning
confidence: 96%
“…Caveats: the expected velocity drift is very difficult to measure at small scales typical of inner envelopes, as the velocity offset is expected to be of the order of the best spectral resolution currently available from typical instruments, and the velocity field is complex (Yen et al, 2018;Cabedo et al, 2022). The main limitation of this method is to ensure that the selected neutral and ion species trace the same gas or are affected by optical depth effects (Pratap et al, 1997;Jørgensen et al, 2004;Girart et al, 2005;Zinchenko et al, 2009).…”
Section: Ion To Neutral Velocity Driftmentioning
confidence: 99%
“…Such low values may suggest it is unlikely that the accretion through the disk to the central star could be driven by magneto-rotational instabilities. In Class 0 protostar B335, Cabedo et al (2022) used deuteration detected in molecular line emission maps to characterize the ionization of the gas at envelope radii ≲ 500 au (typical densities n H_{2} ~10 6 cm −3 ) and found a large cosmic ray ionization rate ζ between 10 -16 and 10 -14 s −1 . Such high values seem inconsistent with the fiducial value if the interstellar cosmic rays flux is responsible for the gas ionization, as it should be efficiently attenuated while penetrating into the dense cores (Padovani et al, 2018).…”
In this review article, we aim at providing a global outlook on the progresses made in the recent years to characterize the role of magnetic fields during the embedded phases of the star formation process. Thanks to the development of observational capabilities and the parallel progress in numerical models, capturing most of the important physics at work during star formation; it has recently become possible to confront detailed predictions of magnetized models to observational properties of the youngest protostars. We provide an overview of the most important consequences when adding magnetic fields to state-of-the-art models of protostellar formation, emphasizing their role to shape the resulting star(s) and their disk(s). We discuss the importance of magnetic field coupling to set the efficiency of magnetic processes and provide a review of observational works putting constraints on the two main agents responsible for the coupling in star-forming cores: dust grains and ionized gas. We recall the physical processes and observational methods, which allow to trace the magnetic field topology and its intensity in embedded protostars and review the main steps, success, and limitations in comparing real observations to synthetic observations from the non-ideal MHD models. Finally, we discuss the main threads of observational evidence that suggest a key role of magnetic fields for star and disk formation, and propose a scenario solving the angular momentum for star formation, also highlighting the remaining tensions that exist between models and observations.
“…Such high values seem inconsistent with the fiducial value if the interstellar cosmic rays flux is responsible for the gas ionization, as it should be efficiently attenuated while penetrating into the dense cores (Padovani et al, 2018). The observations of Cabedo et al (2022) also show the CRs ionization rate is increasing at small envelope radii, toward the central protostellar embryo. Several theoretical works have investigated the role of shocks at the protostellar surface and magnetic mirroring within the jets as efficient forges to accelerate locally low-energy cosmic rays, and their role in increasing the ionization rate of the shielded protostellar material (Padovani et al, 2015;Silsbee et al, 2018;Fitz Axen et al, 2021;Padovani et al, 2021).…”
Section: Fraction Of Ionized Gasmentioning
confidence: 89%
“…The role of the magnetic field in setting the disk size in B335 has also been discussed in subsequent studies (Bjerkeli et al, 2019;Imai et al, 2019;Yen et al, 2019). However, new observations by Cabedo et al (2022) suggest that the gas at small envelope radii is strongly ionized in B335 and points toward conditions typical of ideal MHD. It may very well be that the star-disk building phase consists in a succession of non-ideal and ideal MHD conditions in the "life of the protostar."…”
Section: The Formation Of Disksmentioning
confidence: 96%
“…Caveats: the expected velocity drift is very difficult to measure at small scales typical of inner envelopes, as the velocity offset is expected to be of the order of the best spectral resolution currently available from typical instruments, and the velocity field is complex (Yen et al, 2018;Cabedo et al, 2022). The main limitation of this method is to ensure that the selected neutral and ion species trace the same gas or are affected by optical depth effects (Pratap et al, 1997;Jørgensen et al, 2004;Girart et al, 2005;Zinchenko et al, 2009).…”
Section: Ion To Neutral Velocity Driftmentioning
confidence: 99%
“…Such low values may suggest it is unlikely that the accretion through the disk to the central star could be driven by magneto-rotational instabilities. In Class 0 protostar B335, Cabedo et al (2022) used deuteration detected in molecular line emission maps to characterize the ionization of the gas at envelope radii ≲ 500 au (typical densities n H_{2} ~10 6 cm −3 ) and found a large cosmic ray ionization rate ζ between 10 -16 and 10 -14 s −1 . Such high values seem inconsistent with the fiducial value if the interstellar cosmic rays flux is responsible for the gas ionization, as it should be efficiently attenuated while penetrating into the dense cores (Padovani et al, 2018).…”
In this review article, we aim at providing a global outlook on the progresses made in the recent years to characterize the role of magnetic fields during the embedded phases of the star formation process. Thanks to the development of observational capabilities and the parallel progress in numerical models, capturing most of the important physics at work during star formation; it has recently become possible to confront detailed predictions of magnetized models to observational properties of the youngest protostars. We provide an overview of the most important consequences when adding magnetic fields to state-of-the-art models of protostellar formation, emphasizing their role to shape the resulting star(s) and their disk(s). We discuss the importance of magnetic field coupling to set the efficiency of magnetic processes and provide a review of observational works putting constraints on the two main agents responsible for the coupling in star-forming cores: dust grains and ionized gas. We recall the physical processes and observational methods, which allow to trace the magnetic field topology and its intensity in embedded protostars and review the main steps, success, and limitations in comparing real observations to synthetic observations from the non-ideal MHD models. Finally, we discuss the main threads of observational evidence that suggest a key role of magnetic fields for star and disk formation, and propose a scenario solving the angular momentum for star formation, also highlighting the remaining tensions that exist between models and observations.
“…Finally, note that the models analyzed here implement nonideal MHD processes under ionization conditions that may not be prototypical at the smallest scales around protostars: for example, Cabedo et al (2022) estimated cosmic-ray ionization rates in B335 from observations probing the ∼ 100 − 500 au scales which are up to two orders of magnitude higher than the predicted ionization generated by external cosmic rays alone. If the ionization was indeed to be much stronger at small envelope radii due to locally accelerated cosmic rays, that would make the coupling of B fields to the local gas much more efficient and models that implement both ideal and nonideal MHD with realistic local ionization conditions would need to be explored in the future.…”
Section: Dust Polarized Emission: An Overall Good Tracer Of B-fields ...mentioning
Context. High-resolution millimeter and submillimeter (mm and submm) polarization observations have opened a new era in the understanding of how magnetic fields are organized in star forming regions, unveiling an intricate interplay between the magnetic fields and the gas in protostellar cores. However, to assess the role of the magnetic field in the process of solar-type star formation, it is important to understand to what extent these polarized dust emission are good tracers of the magnetic field in the youngest protostellar objects. Aims. In this paper, we present a thorough investigation of the fidelity and limitations of using dust polarized emission to map the magnetic field topologies in low-mass protostars. Methods. To assess the importance of these effects, we performed an analysis of magnetic field properties in 27 realizations of magnetohydrodynamics (MHD) models following the evolution of physical properties in star-forming cores. Assuming a uniform population of dust grains the sizes of which follow the standard MRN size distribution, we analyzed the synthetic polarized dust emission maps produced when these grains align with the local B-field because of radiative torques (B-RATs). Results. We find that mm and submm polarized dust emission is a robust tracer of the magnetic field topologies in inner protostellar envelopes and is successful at capturing the details of the magnetic field spatial distribution down to radii ∼ 100 au. Measurements of the line-of-sight-averaged magnetic field line orientation using the polarized dust emission are precise to < 15 • (typical of the error on polarization angles obtained with observations from large mm polarimetric facilities such as ALMA) in about 75% − 95% of the independent lines of sight that pass through protostellar envelopes. Large discrepancies between the integrated B-field mean orientation and the orientation reconstructed from the polarized dust emission are mostly observed in (i) lines of sight where the magnetic field is highly disorganized and (ii) those that probe large column densities. Our analysis shows that the high opacity of the thermal dust emission and low polarization fractions could be used to avoid using the small fraction of measurements affected by large errors.
We demonstrate for the first time that Galactic cosmic rays with energies as high as ∼10 10 eV can trigger a cascade of low-energy (<20 eV) secondary electrons that could be a significant contributor to the interstellar synthesis of prebiotic molecules whose delivery by comets, meteorites, and interplanetary dust particles may have kick-started life on Earth. For the energetic processing of interstellar ice mantles inside dark, dense molecular clouds, we explore the relative importance of low-energy (<20 eV) secondary electrons�agents of radiation chemistry�and lowenergy (<10 eV), nonionizing photons�instigators of photochemistry. Our calculations indicate fluxes of ∼10 2 electrons cm −2 s −1 for low-energy secondary electrons produced within interstellar ices due to attenuated Galactic cosmic-ray protons. Consequently, in certain star-forming regions where internal high-energy radiation sources produce ionization rates that are observed to be a thousand times greater than the typical interstellar Galactic ionization rate, the flux of low-energy secondary electrons should far exceed that of nonionizing photons. Because reaction cross sections can be several orders of magnitude larger for electrons than for photons, even in the absence of such enhancement, our calculations indicate that secondary low-energy (<20 eV) electrons are at least as significant as low-energy (<10 eV) nonionizing photons in the interstellar synthesis of prebiotic molecules. Most importantly, our results demonstrate the pressing need for explicitly incorporating low-energy electrons in current and future astrochemical simulations of cosmic ices. Such models are critically important for interpreting James Webb Space Telescope infrared measurements, which are currently being used to probe the origins of life by studying complex organic molecules found in ices near star-forming regions.
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