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REVIEW 2 major objections 4 minor 192 references

Cosmic Velocity Flows: from Theory to Observations

T0 review · 2 major / 4 minor · reviewed 2026-08-05 · deepseek-v4-flash

Pith's one-line read The thesis claims that cosmic filaments are hierarchically nested structures whose phase space shows coherent infall, multistreaming, and caustic-like features, recoverable from discrete tracers by Skeletor, a Voronoi-based hierarchical fil

desk verdict Sahyadri and the mock-calibration framework are real contributions, but the phase-space 'discovery' rests on defining Rv as the infall minimum and then scaling by Rv, so the headline features are built in. read the letter →

arxiv 2608.03530 v1 pith:JMBJJDVG submitted 2026-08-04 astro-ph.CO

classification astro-ph.CO
keywords cosmicwebfilamentsN-bodysimulationsVoronoitessellationphase-spacestructurehierarchicalformationlarge-scalepeculiarvelocities
verification ladder T0 review T1 audit T2 compute T3 formal

The pith

A machine-rendered reading of the paper's core claim, the machinery that carries it, and where it could break.

The reading

This thesis tries to establish that cosmic filaments—the dense threads of the cosmic web—can be identified reliably from discrete galaxy-like tracers, and that once identified they show a rich, ordered phase-space structure that two-point clustering statistics miss. It builds three things: the Sahyadri simulation suite, which resolves halos roughly 25 times lighter than the previous best parameter-varying suite; a calibration framework (FilGen/FilAPT) showing that filament curvature and spine-reconstruction noise bias measured profiles and can be corrected with optimized Fourier smoothing; and Skeletor, a Voronoi-based hierarchical filament finder. Applied to simulations, Skeletor splits filaments into nested sub-filaments and stacks their density and velocity profiles, revealing coherent radial infall, multistreaming, and caustic-like features near the filament edge. If right, these results give a physically motivated, dynamics-based way to define filament boundaries and a new observational handle on nonlinear structure formation.

What carries the argument

Skeletor is the central object: a Voronoi-based hierarchical filament finder. It quantifies local anisotropy from the Voronoi tessellation of tracer positions, selects filament-like cells, connects them into spines, orders the resulting network by a mass hierarchy, and optionally refines spines with dark-matter density while estimating filament radius Rv from the minimum of the radial infall velocity. Supporting it are the FilGen/FilAPT calibration tools, which create controlled mock filaments with known spines, and the Sahyadri N-body suite, whose seed-matched parameter variations and high mass resolution supply the tracer populations and the beyond-two-point statistics (VVF, kNN) that the

What would settle it

Recompute the stacked phase-space profiles using a filament radius defined independently of the velocity profile—say, from the density-gradient or tangential-velocity transition—and without the Rv>0.6 cut; if the coherent-infall and caustic features at r/Rv≈1 disperse, they were built in by the radius definition rather than discovered.

Watch

Extended reading notes

Core claim

The central discovery is that the phase space of cosmic filaments is organized and hierarchical. Using Skeletor, the thesis reconstructs filament spines directly from discrete tracers with a Voronoi tessellation, uses dark-matter information to refine the spine and to define each filament's radius Rv as the location of maximum radial infall, and classifies nested sub-filaments within parent filaments. Stacked profiles then show coherent anisotropic inflow toward the spine, a velocity transition at the inferred boundary, multistreaming inside, and localized caustic-like features—signatures expected from anisotropic gravitational collapse. The thesis also shows that sub-filaments are statistic

Load-bearing premise

The central premise is that every filament has a single coherent radial infall whose deepest point is its physical edge; filaments whose fitted infall profile shows a different inner minimum are cut out rather than analysed.

Editorial extensions

If this is right

  • Filament boundaries can be defined dynamically by the radius of maximum coherent infall, tying geometry directly to ongoing gravitational collapse.
  • Filament hierarchy matters: sub-filaments embedded in parent filaments have distinct density and velocity profiles, so stacked filament statistics should separate hierarchy levels.
  • Phase-space diagnostics such as infall, multistreaming, and caustics provide observables beyond the power spectrum for the quasi-linear and nonlinear regimes.
  • Optimized Fourier spine smoothing substantially improves the recovery of density and velocity profiles, reducing methodology-induced bias in filament studies.
  • Sahyadri's resolution enables VVF and kNN statistics at high tracer density with clear Omega_m sensitivity, supporting cosmological constraints from beyond-two-point statistics.

Reading between the lines

Editorial extensions of the paper, not claims the author makes directly.

  • A natural next step, not developed in the thesis, is to test whether the stacked phase-space profiles are universal across mass and redshift; the thesis frames universality as motivation, and the tools make it directly testable.
  • Because the Rv-scaled profiles may be partly built into the radius definition, the claimed features near r/Rv=1 should be checked against a radius defined independently of the velocity profile, for example from the density gradient.
  • The parent/sub-filament decomposition suggests that environment definitions for galaxy evolution studies may need to distinguish parent-filament from sub-filament membership, potentially affecting quenching and assembly-bias analyses.
  • Skeletor's inputs are only tracer positions and masses, so the same phase-space reconstruction could be attempted with spectroscopic galaxy surveys; the thesis's calibration framework could quantify how redshift-space distortions bias the inferred velocities.
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Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, and a circularity audit.

Referee Report

2 major / 4 minor

Summary. The thesis develops a set of numerical and methodological tools for studying the non-linear cosmic web, with emphasis on filamentary structure and velocity flows. It introduces the Sahyadri suite of high-resolution N-body simulations with systematic cosmological parameter variations; a calibration framework (FilGen/FilAPT) built on controlled filament realizations with known ground truth, including a Fourier-space smoothing technique; and Skeletor, a Voronoi-based hierarchical filament finder that reconstructs filament spines and sub-filaments from discrete tracers. These tools are then applied to study filament phase-space structure, reporting coherent radial infall, multistreaming, caustic-like features, and a hierarchy of sub-filaments. The central dynamical claims are that filaments have physically meaningful boundaries and that stacked phase-space profiles reveal a universal or quasi-universal structure.

Significance. The manuscript has several genuine strengths. The Sahyadri suite is carefully validated against Halofit and Tinker predictions (§2.4.2, Appendix A.3), and its improved mass resolution is quantified clearly. The FilGen/FilAPT calibration framework is a valuable contribution: it provides controlled realizations with known truth, and the optimized Fourier smoothing demonstrably reduces reconstruction biases (§3.3–3.4). Skeletor is a novel method that incorporates hierarchy in a principled way and does not require gridding of tracers. The public release of code and data products is also commendable. If the phase-space results were robust, the thesis would constitute a significant step toward a physical, dynamics-based description of filaments. However, as detailed below, the central phase-space claims currently rest on a radius definition that is partly circular, so the dynamical picture--coherent infall, filament boundaries, and the distinctiveness of sub-filaments--needs additional independent validation before those claims can be accepted.

major comments (2)
  1. [§4.3.6, Figs. 5.2, 6.6, 6.8] The comparison of alternative radius definitions in Fig. 6.8 is performed in bins of Rv after the sample has already been selected and scaled by Rv, so it does not break the circularity. An independent radius estimator (e.g., from density gradient or velocity dispersion) should be computed per filament, and the correlation between Rv and that estimator should be assessed without conditioning on Rv. Unless the phase-space features are shown to persist with an independently defined radius, the central claim of coherent infall and filament boundaries is not yet supported.
  2. [§6.3.4, Fig. 6.5] The same concern applies to the substructure analysis in Chapter 5, where parent and sub-filament profiles are compared using Rv-scaled radial distances (Fig. 5.2 and Fig. 4.10). The claim that sub-filaments are 'distinctly different' is based on the same velocity-defined radius and the same quality cuts. Please show whether the differences persist when profiles are compared in absolute radius or with a radius definition that does not rely on the infall minimum.
minor comments (4)
  1. [Appendix C.2] Typo in figure caption: 'panles' should be 'panels'. There are also several similar typographical and formatting issues throughout (e.g., 'wheras' in the Appendix C.4 caption, inconsistent spacing in 'er f'). A careful proofreading pass is needed.
  2. [§3.4.1] The description of the optimized Fourier smoothing is clear but the connection to the earlier FilAPT module could be made more explicit. In particular, the reader would benefit from a statement of how the optimization criterion behaves when the true profile is not known (as in real applications), and whether the method has been tested on mock filaments with a wide range of signal-to-noise.
  3. [Chapter 6] The phase-space plots (Fig. 6.10) and the interpretation in terms of multistreaming are interesting, but the figure labels are small and the text does not state the number of filaments used to produce the stacked distribution. Adding the sample size and the uncertainty on the median velocity would strengthen the presentation.
  4. [§2.4.1] The claim that 'Sahyadri resolves halos down to M_min = 3.2e9 h−1 M_sun' relies on a 40-particle threshold. The manuscript could state more explicitly how the results depend on this resolution threshold, particularly for the VVF and kNN statistics, since these are sensitive to the lowest-mass tracers.

Circularity Check

2 steps flagged · score 6.0 of 10

Phase-space 'boundary' and coherent-infall features are largely built into the Rv definition and the Rv cut; other results (multistreaming, density profiles) remain independent.

  1. self definitional [Ch. 4 §4.3.6 / Fig. 4.5 caption; Ch. 5 Fig. 5.2 caption]
    "The red curve shows the quadratic fit used to locate the velocity dip. The solid vertical line indicates the final filament radius Rv, defined by the location of largest radial infall. ... The radial distance is scaled by the radius of the filament, Rv."

    Because Rv is defined as the location of the vr dip, stacking profiles in units of r/Rv places the dip at r/Rv=1 by construction. The thesis then presents this dip as a discovered 'filament boundary' and 'coherent infall' feature. The existence of negative vr at small radii is an independent measurement, but the specific claim that the boundary/infall feature sits at r/Rv≈1 is a restatement of the definition, not an empirical discovery.

  2. fitted input called prediction [Ch. 6 Fig. 6.5 caption; Ch. 6 Figs. 6.6, 6.8]
    "The main population shows the expected positive correlation between filament radius and node mass, while a secondary population at low Rv arises from systems where the fitting procedure identifies an unphysical inner minimum in the radial velocity profile. The vertical dashed line marks the cut at Rv = 0.6 h−1Mpc adopted for the remainder of the analysis."

    The sample is cleaned by removing systems whose quadratic fit yields Rv < 0.6 h−1Mpc, described as an 'unphysical inner minimum'. These are precisely the objects that do not conform to the assumed single-infall profile used to define Rv. After this cut, the stacked profiles are presented as evidence of coherent infall and universal filament boundaries. The agreement with the assumed profile is therefore partly enforced by sample selection, so the 'prediction' of coherent infall is not independent of the fitted definition and cut.

full rationale

The central dynamical claim—that filament boundaries and coherent infall features appear at r/Rv≈1—is partially circular. Rv is defined as the location of maximum radial infall (the vr minimum) via a quadratic fit, and then all stacked phase-space profiles are scaled by Rv. This forces the infall dip to appear at r/Rv=1 by construction. The additional cut at Rv=0.6 h−1Mpc removes the secondary population whose fits show an 'unphysical inner minimum', i.e., the systems that most strongly violate the assumed single-infall profile; the cleaned sample is then used to report coherent inflow and boundary features, making the agreement with the assumed profile partly a selection effect. However, the thesis also contains genuinely independent content: the multistreaming and caustic-like phase-space features are not guaranteed by the radius definition, the density and dispersion profiles are measured without imposing the dip position, the substructure classification is geometric rather than velocity-based, and the Sahyadri suite is validated against external fitting functions (Halofit, Tinker). The optimized-smoothing claim is checked against known ground-truth profiles in the FilGen framework, so it is not circular despite its heuristic objective. No load-bearing self-citation chain or imported uniqueness theorem was found. Score 6 reflects partial circularity of the boundary/infall claim, not full circularity of the thesis.

Assumptions & free parameters 6 free parameters · 6 assumptions · 1 invented entities

The central claims rest on a moderate number of adjustable parameters, mostly in the mock generator, the filament finder's thresholds, and the radius definition. The most impactful free parameters are the Rv quality cut and the smoothing optimization target, because they shape the physical conclusions. The assumptions are standard CDM cosmology plus the paper-specific hierarchy and radius definitions, which are the main load-bearing premises.

free parameters (6)
  • FilGen velocity ansatz parameters (V0z, V0r, sigma0, a, b, c, u, g) = V0z=V0r=250 km/s, sigma0=300 km/s, a=0.125, b=2.5, c=15, u=8, g=0.5
    Chosen by hand to 'approximately match' the radial velocity profiles of [157] (Section 3.3.2.1). These set the ground truth in the calibration mocks, so the demonstrated biases and the performance of the smoothing method depend on them.
  • Anisotropy threshold alpha_th = 95th percentile of random-catalogue alpha distribution (default)
    Used in Skeletor to select filament-like Voronoi cells (Appendix C.3). Shifting this threshold changes the recovered filament population.
  • Connectivity parameter dcut = l_mean (mean inter-tracer spacing)
    Controls how filament segments are linked into spines (Appendix C.4). The length distribution and hierarchy collapse are sensitive to this choice.
  • Hierarchy mass thresholds = Mass bins used in the mass-thresholded hierarchy (Appendix C.2)
    Define parent and sub-filament levels. Sensitivity tests show little variation, but the classification is constructed from these thresholds.
  • Filament radius quality cut = Rv > 0.6 h^-1 Mpc
    Removes a 'secondary population' of filaments whose fitted radial velocity minima are deemed unphysical (Chapter 6, Figure 6.5). The reported phase-space trends depend on this cut.
  • Smoothing parameters in optimized Fourier/neighbour smoothing = Chosen per filament by minimizing the width of the inferred density profile
    The optimization objective assumes that the true density profile is narrow, which is part of the circularity concern; the selected smoothing scale affects all recovered profiles (Appendix B.5).
assumptions (6)
  • standard math FLRW background and Newtonian N-body dynamics for sub-horizon structure formation
    Invoked in Chapter 2 (Eqs. 1.1-2.3). The simulations and all analysis assume this framework.
  • domain assumption Cold dark matter with collisionless particles and no massive neutrinos
    Stated in Section 2.4.1: 'massive neutrinos are not included'. The Sahyadri simulations therefore probe a particular dark matter model.
  • ad hoc to paper The cosmic web has a hierarchical filament-in-filament structure that can be decomposed via mass thresholds
    Core to Skeletor and the sub-filament analysis (Chapters 4 and 5). The paper does not prove this decomposition is unique or physically preferred.
  • ad hoc to paper The location of maximum radial infall defines the 'true' filament radius
    Used to define Rv in Section 4.3.6 and throughout Chapter 6. This is a dynamical definition, not derived from first principles, and it creates the circularity with the stacked profiles.
  • domain assumption The analytic velocity ansatz in Eqs. 3.1-3.3 represents realistic cosmic filament kinematics
    The mock filament ground truth in Chapter 3 is built from this ansatz, so the calibration results measure how well the tools recover this particular model, not necessarily real filaments.
  • domain assumption Voronoi cell anisotropy is a faithful proxy for filamentary environment
    The motivating observation in Chapter 4 (Figure 4.1). If tracer bias makes Voronoi cells anisotropic for other reasons, the Skeletor selection would be contaminated.
invented entities (1)
  • Sub-filaments (filamentary substructures embedded within parent filaments)
    purpose: To classify nested filamentary systems and study their separate statistical and geometric properties (Chapters 4 and 5).
    Sub-filaments are defined by the mass-hierarchy classifier in Skeletor. No independent observable signature is provided that would distinguish a sub-filament from a parent filament in galaxy surveys.

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Cite this review

Pith. "Pith review of Cosmic Velocity Flows: from Theory to Observations." pith.science (2026). https://pith.science/paper/JMBJJDVG

@misc{pith2026260803530,
  author       = {Pith},
  title        = {Pith review of: Cosmic Velocity Flows: from Theory to Observations},
  year         = {2026},
  howpublished = {\url{https://pith.science/paper/JMBJJDVG}},
  note         = {Machine review of arXiv:2608.03530}
}
abstract

The Large-Scale Structure (LSS) of the Universe forms a complex network of nodes, filaments, sheets, and voids known as the Cosmic Web. As current and upcoming galaxy surveys increasingly probe the quasi-linear and non-linear regimes of structure formation, understanding its geometry and dynamics is essential for precision cosmology. In particular, cosmic filaments, which channel matter across the web, are central to these dynamical processes. This thesis develops numerical tools to study the non-linear cosmic web. First, the Sahyadri suite of high-resolution cosmological $N$-body simulations is introduced, providing a framework for precision studies of LSS and its cosmological dependence. A calibration framework for filament reconstruction is then developed using controlled filament realizations, enabling systematic investigation of reconstruction biases. The effects of filament curvature and reconstruction noise on inferred filament properties are quantified, and a novel Fourier-space smoothing approach is introduced to improve profile recovery. The thesis further presents Skeletor, a Voronoi-based filament finder that identifies filamentary structures directly from discrete tracers while explicitly incorporating the hierarchical nature of the cosmic web. A novel framework for classifying sub-filamentary structure is developed. Applying these tools to cosmological simulations reveals distinct properties of filament substructure and provides a detailed view of filament phase space, including coherent inflows, multistreaming, and caustic-like features. Together, these developments provide a framework for studying the geometry, hierarchy, and dynamics of the non-linear cosmic web. More broadly, they contribute to the ongoing effort to build a physically motivated understanding of the non-linear cosmic web beyond traditional measures of clustering.

Figures

Figures reproduced from arXiv: 2608.03530 by the authors.

Figure 1.1
Figure 1.1. Visualization of the large-scale galaxy and quasar distribution mapped by the DESI [PITH_FULL_IMAGE:figures/full_fig_p034_1_1.png] view at source ↗
Figure 1.2
Figure 1.2. Dark matter density fields illustrating the cosmic web at multiple scales, adapted [PITH_FULL_IMAGE:figures/full_fig_p037_1_2.png] view at source ↗
Figure 2.1
Figure 2.1. Stellar mass function using a stellar-to-halo mass relation and a conditional [PITH_FULL_IMAGE:figures/full_fig_p052_2_1.png] view at source ↗
Figures from the paper (47 more)
Figure 2.2
Figure 2.2. Figure 2.2: Comparison of the Sahyadri simulation suite with other large-scale structure simu￾lation efforts. Grey lines indicate simulations with constant particle number assuming Planck 2018 cosmology. Coloured points highlight suites with cosmology variations. The red (black)…
Figure 2.3
Figure 2.3. Figure 2.3: Visualization of the evolution of the dark matter density field as a function of redshift [PITH_FULL_IMAGE:figures/full_fig_p057_2_3.png]
Figure 2.4
Figure 2.4. Figure 2.4: Comparison between AbacusSummit-like and [PITH_FULL_IMAGE:figures/full_fig_p058_2_4.png]
Figure 2.5
Figure 2.5. Figure 2.5: Same as Figure [PITH_FULL_IMAGE:figures/full_fig_p059_2_5.png]
Figure 2.6
Figure 2.6. Figure 2.6: Visualizations of single-cell slices of the tessellated density field at [PITH_FULL_IMAGE:figures/full_fig_p060_2_6.png]
Figure 2.7
Figure 2.7. Figure 2.7: Variation of the matter power spectrum as a function of [PITH_FULL_IMAGE:figures/full_fig_p061_2_7.png]
Figure 2.8
Figure 2.8. Figure 2.8: Comparison of the halo power spectrum (Phh) for different tracers, Ωmvalues, and redshifts. The top panels show Phh for two tracer populations with different number densities, thresholded on Vpeak(see text for details). Solid lines correspond to the fiducial cosmolog…
Figure 2.9
Figure 2.9. Figure 2.9: Variation of the mass function as a function of [PITH_FULL_IMAGE:figures/full_fig_p063_2_9.png]
Figure 2.10
Figure 2.10. Figure 2.10: Same as Figure [PITH_FULL_IMAGE:figures/full_fig_p063_2_10.png]
Figure 2.11
Figure 2.11. Figure 2.11: Same as Figure [PITH_FULL_IMAGE:figures/full_fig_p064_2_11.png]
Figure 2.12
Figure 2.12. Figure 2.12: Spearman rank correlations between halo environment and internal properties, as a [PITH_FULL_IMAGE:figures/full_fig_p066_2_12.png]
Figure 2.13
Figure 2.13. Figure 2.13: Redshift dependence of correlations for the fiducial cosmology. The panels are the [PITH_FULL_IMAGE:figures/full_fig_p066_2_13.png]
Figure 3.1
Figure 3.1. Figure 3.1: Plots showing number density projections of the fiducial filament along the three [PITH_FULL_IMAGE:figures/full_fig_p076_3_1.png]
Figure 3.2
Figure 3.2. Figure 3.2: Various profiles for the fiducial filament model. The left (right) panels show longitudi [PITH_FULL_IMAGE:figures/full_fig_p079_3_2.png]
Figure 3.3
Figure 3.3. Figure 3.3: Projected number density for the thick filament. The panels are the same as Figure [PITH_FULL_IMAGE:figures/full_fig_p080_3_3.png]
Figure 3.4
Figure 3.4. Figure 3.4: Radial and longitudinal density and velocity profiles for the thick filament. The [PITH_FULL_IMAGE:figures/full_fig_p081_3_4.png]
Figure 3.5
Figure 3.5. Figure 3.5: Effect of sampling of the spine on the density and velocity profiles. The panels are [PITH_FULL_IMAGE:figures/full_fig_p084_3_5.png]
Figure 3.6
Figure 3.6. Figure 3.6: Effect of error in spine extraction on the estimated density and velocity profiles. [PITH_FULL_IMAGE:figures/full_fig_p085_3_6.png]
Figure 3.7
Figure 3.7. Figure 3.7: Comparison of optimized and constant smoothing and curvature segregation on the [PITH_FULL_IMAGE:figures/full_fig_p086_3_7.png]
Figure 3.8
Figure 3.8. Figure 3.8: PDFs of lengths lfil of the DisPerSE inferred spines in units of the length lf of the actual spine. Pink colour represents the unsmoothed case, while green and purple colours represent the spines after applying a constant neighbour smoothing and optimized Fourier smo…
Figure 3.9
Figure 3.9. Figure 3.9: Distribution of the parameters of the filaments, [PITH_FULL_IMAGE:figures/full_fig_p089_3_9.png]
Figure 3.10
Figure 3.10. Figure 3.10: Illustration of need for optimized smoothing for a diverse filament set. The left panel [PITH_FULL_IMAGE:figures/full_fig_p089_3_10.png]
Figure 3.11
Figure 3.11. Figure 3.11: Effect of redshift space distortions on the density profiles of straight filaments with [PITH_FULL_IMAGE:figures/full_fig_p091_3_11.png]
Figure 4.1
Figure 4.1. Figure 4.1: Illustration of the geometric motivation behind [PITH_FULL_IMAGE:figures/full_fig_p101_4_1.png]
Figure 4.2
Figure 4.2. Figure 4.2: Schematic overview of the Skeletor algorithm. scales. At each hierarchy level, the most massive halos act as nodes, whereas the filamentary structures connecting them are traced by lower-mass halos arranged along the spine like beads on a string. Progressively loweri…
Figure 4.3
Figure 4.3. Figure 4.3: Distribution of the anisotropy parameter [PITH_FULL_IMAGE:figures/full_fig_p106_4_3.png]
Figure 4.4
Figure 4.4. Figure 4.4: Example of the dipole-minimization smoothing procedure. The radial density profile [PITH_FULL_IMAGE:figures/full_fig_p109_4_4.png]
Figure 4.5
Figure 4.5. Figure 4.5: Example illustrating the estimation of the filament radius. The plot shows the radial [PITH_FULL_IMAGE:figures/full_fig_p110_4_5.png]
Figure 4.6
Figure 4.6. Figure 4.6: Reconstruction of the prominent filament shown in Figure [PITH_FULL_IMAGE:figures/full_fig_p112_4_6.png]
Figure 4.7
Figure 4.7. Figure 4.7: Comparison of filament networks identified by [PITH_FULL_IMAGE:figures/full_fig_p113_4_7.png]
Figure 4.8
Figure 4.8. Figure 4.8: Length distribution of filaments identified by [PITH_FULL_IMAGE:figures/full_fig_p114_4_8.png]
Figure 4.9
Figure 4.9. Figure 4.9: Average radial density (left) and radial velocity (right) profiles of filaments identified [PITH_FULL_IMAGE:figures/full_fig_p115_4_9.png]
Figure 4.10
Figure 4.10. Figure 4.10: Comparison between the stacked radial profiles of parent (black) and sub-filaments [PITH_FULL_IMAGE:figures/full_fig_p116_4_10.png]
Figure 5.1
Figure 5.1. Figure 5.1: Left panel: Distribution of the total node mass, log(M1+M2). Right panel: Distribution of the corresponding node mass ratio, M1/M2. Parent filaments are shown in black and sub￾filaments in red. Node masses are reported in units of M⊙/h. we perform a second comparison…
Figure 5.2
Figure 5.2. Figure 5.2: Comparison of the radial density and velocity profiles of parent filaments (solid curves) [PITH_FULL_IMAGE:figures/full_fig_p123_5_2.png]
Figure 6.1
Figure 6.1. Figure 6.1: Stacked radial phase-space profiles in ten percentile bins of filament curvature, [PITH_FULL_IMAGE:figures/full_fig_p132_6_1.png]
Figure 6.2
Figure 6.2. Figure 6.2: Illustration of filament curvature. The figure shows the projection of a filament [PITH_FULL_IMAGE:figures/full_fig_p133_6_2.png]
Figure 6.3
Figure 6.3. Figure 6.3: Stacked density and radial velocity profiles in ten percentile bins of filament length. [PITH_FULL_IMAGE:figures/full_fig_p133_6_3.png]
Figure 6.4
Figure 6.4. Figure 6.4: Stacked phase-space profiles in ten percentile bins of the total node mass, [PITH_FULL_IMAGE:figures/full_fig_p135_6_4.png]
Figure 6.5
Figure 6.5. Figure 6.5: Two-dimensional distribution of the velocity-defined filament radius, [PITH_FULL_IMAGE:figures/full_fig_p135_6_5.png]
Figure 6.6
Figure 6.6. Figure 6.6: Stacked phase-space profiles in ten percentile bins of the velocity-defined filament [PITH_FULL_IMAGE:figures/full_fig_p136_6_6.png]
Figure 6.7
Figure 6.7. Figure 6.7: Two-dimensional distribution of the velocity-defined filament radius, [PITH_FULL_IMAGE:figures/full_fig_p137_6_7.png]
Figure 6.8
Figure 6.8. Figure 6.8: Comparison of different filament radius definitions relative to the velocity-defined [PITH_FULL_IMAGE:figures/full_fig_p138_6_8.png]
Figure 6.9
Figure 6.9. Figure 6.9: Individual filament profiles for two representative primary filaments (red and blue). [PITH_FULL_IMAGE:figures/full_fig_p139_6_9.png]
Figure 6.10
Figure 6.10. Figure 6.10: (left panel:) Schematic illustrating the construction of the filament phase-space distribution. The solid black line represents the filament spine made up of discrete segments, with cylinders of radius Rv centred on individual spine segments and oriented perpendicul…
Figure 6.11
Figure 6.11. Figure 6.11: Examples of (x,vx) phase-space diagrams for three individual parent filaments. In all cases, coherent infall towards the filament spine is followed by multistreaming, and eventually a sharp broadening of the velocity distribution in the central regions. Localized en…
Figure 6.12
Figure 6.12. Figure 6.12: Radial velocity distributions, P(vr), at three neighbouring cylindrical radii for a representative parent filament. The left, centre, and right panels correspond to regions dominated by coherent infall, multistreaming, and the central dynamically mixed region, respe…

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