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The far-infrared (FIR) distribution at high Galactic latitudes, observed with Planck is filamentary with coherent structures in polarization. These structures are also closely related to filaments with coherent velocity structures. There is a long-standing debate about the physical nature of these structures. They are considered either as velocity caustics, fluctuations engraved by the turbulent velocity field or as cold three-dimensional density structures in the interstellar medium (ISM). We discuss different approaches to data analysis and interpretation in order to work out the differences. We considered mathematical preliminaries for the derivation of caustics that characterize filamentary structures in the ISM. Using the Hessian operator, we traced individual FIR filamentary structures in from channel maps as observed and alternatively from data that are provided by the velocity decomposition algorithm (VDA). VDA is claimed to separate velocity caustics from density effects. Based on the strict mathematical definition, the so-called velocity caustics are not actually caustics. These VDA data products may contain caustics in the same way as the original observations. Caustics derived by a Hessian analysis of both databases are nearly identical with a correlation coefficient of 98<!PCT!>. However, the VDA algorithm leads to a 30<!PCT!> increase in the alignment uncertainties when fitting FIR/ orientation angles. Thus, the VDA velocity crowding concept fails to explain the alignment of FIR/ filaments at $|b| > We used absorption data to constrain the physical nature of FIR/ filaments and determine spin temperatures and volume densities of FIR/ filaments. filaments exist as cold neutral medium (CNM) structures; outside the filaments no CNM absorption is detectable. The CNM in the diffuse ISM is exclusively located in filaments with FIR counterparts. These filaments at high Galactic latitudes exist as cold density structures; velocity crowding effects are negligible.
The far-infrared (FIR) distribution at high Galactic latitudes, observed with Planck is filamentary with coherent structures in polarization. These structures are also closely related to filaments with coherent velocity structures. There is a long-standing debate about the physical nature of these structures. They are considered either as velocity caustics, fluctuations engraved by the turbulent velocity field or as cold three-dimensional density structures in the interstellar medium (ISM). We discuss different approaches to data analysis and interpretation in order to work out the differences. We considered mathematical preliminaries for the derivation of caustics that characterize filamentary structures in the ISM. Using the Hessian operator, we traced individual FIR filamentary structures in from channel maps as observed and alternatively from data that are provided by the velocity decomposition algorithm (VDA). VDA is claimed to separate velocity caustics from density effects. Based on the strict mathematical definition, the so-called velocity caustics are not actually caustics. These VDA data products may contain caustics in the same way as the original observations. Caustics derived by a Hessian analysis of both databases are nearly identical with a correlation coefficient of 98<!PCT!>. However, the VDA algorithm leads to a 30<!PCT!> increase in the alignment uncertainties when fitting FIR/ orientation angles. Thus, the VDA velocity crowding concept fails to explain the alignment of FIR/ filaments at $|b| > We used absorption data to constrain the physical nature of FIR/ filaments and determine spin temperatures and volume densities of FIR/ filaments. filaments exist as cold neutral medium (CNM) structures; outside the filaments no CNM absorption is detectable. The CNM in the diffuse ISM is exclusively located in filaments with FIR counterparts. These filaments at high Galactic latitudes exist as cold density structures; velocity crowding effects are negligible.
The morphology and the characteristic scale of polarized structures provide crucial insights into the mechanisms that drive turbulence and maintain magnetic fields in magneto-ionic plasma. We aim to establish the efficacy of Minkowski functionals as quantitative statistical probes of filamentary morphology of polarized synchrotron emission resulting from fluctuation dynamo action. Using synthetic observations generated from magnetohydrodynamic simulations of fluctuation dynamos with varying driving scales (ℓ f) of turbulence in isothermal, incompressible, and subsonic media, we study the relation between different morphological measures and their connection to fractional polarization (p f). We find that Faraday depolarization at low frequencies gives rise to small-scale polarized structures that have higher filamentarity as compared to the intrinsic structures that are comparable to ℓ f. Above ∼3 GHz, the number of connected polarized structures per unit area (N CC,peak) is related to the mean p f (〈p f〉) of the emitting region as 〈 p f 〉 ∝ N CC , peak − 1 / 4 , provided the scale of the detectable emitting region is larger than ℓ f. This implies that N CC,peak represents the number of turbulent cells projected on the plane of the sky and can be directly used to infer ℓ f via the relation ℓ f ∝ N CC , peak − 1 / 2 . An estimate of ℓ f thus directly allows for pinning down the turbulence-driving mechanism in astrophysical systems. While the simulated conditions are mostly prevalent in the intracluster medium of galaxy clusters, the qualitative morphological features are also applicable in the context of interstellar medium in galaxies.
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