Astrophysics · arXiv:astro-ph/0404451 v1 · submitted 22 Apr 2004 · 24 references
Interstellar Turbulence I: Observations and Processes
The paper says
“This two-part review summarizes interstellar turbulence and its implications. The first part begins with diagnostics and energy sources.”
more of the abstract
Turbulence theory is considered in detail, including the basic fluid equations, solenoidal and compressible modes, global inviscid quadratic invariants, scaling arguments, energy transfer and cascade, velocity probability distributions, and turbulent pressure. Theories of magnetohydrodynamic turbulence, including collisionless MHD turbulence, are discussed, emphasizing various proposals for energy spectra. A large variety of numerical simulations of interstellar turbulence are reviewed. Models have reproduced many of the basic features of the observed scaling relations, predicted fast decay rates for supersonic MHD turbulence, and derived probability distribution functions for density. Thermal instabilities and thermal phases have a new interpretation in a turbulent medium. Large-scale models with various combinations of self-gravity, magnetic fields, supernovae, and star formation are beginning to resemble the observed interstellar medium in morphology and statistical properties. The role of self-gravity in turbulent gas is clarified, leading to new paradigms for the formation of star clusters, the stellar mass function, the origin of stellar rotation and binary stars, and the effects of magnetic fields.
from the abstract
Pith says
Machine review · deepseek-v4.1-flash · 13 Nov 2026 · what was read was not recorded · not checked by a person
Reviewed in 2026 with later literature in view.
It can be wrong. Challenge this review or reply to it.
Holds up. The standard 2004 map of interstellar turbulence, honest about its own uncertainties almost everywhere except the abstract's claim of 'new paradigms' for rotation and binary stars. This line is wrong
3 major objections · 7 minor
How often objections from reviews like this one are right: not yet measured
Not checked: figures, code, what the 24 references say.
The paper says, at §2 vs. §6
The review did not quote this passage.
Pith says: Objection 1 of 3 · major
The review's most-quoted observational number is stated two different ways. §2 reports that power spectra of Milky Way H I emission, H I absorption, CO emission, and IRAS 100 micron emission, and of 2D H I emission from the SMC and LMC, have slopes 'around −2.8 to −3.2 in 2D maps,' and explicitly notes that this is steeper than the …
more of objection 1
… −8/3 expected for projected velocity in incompressible turbulence. §6 then states that 'the power spectrum of the associated intensity fluctuations is a robust power law with a slope between −1.8 and −2.3 for the Milky Way, LMC, and SMC.' Those two ranges do not overlap, and the §6 range coincides with the 1D azimuthal values that §2 says are shallower by one power of k because of the reduced dimension. As written, a reader cannot tell whether the headline observational result is −3 or −2. Please reconcile the two passages and state the dimensionality and convention explicitly in both places, since this number is the empirical anchor for the comparison with simulations in §5.2 and §5.14.
The paper says, at Abstract (s8) vs. §5.11–5.12
The review did not quote this passage.
Pith says: Objection 2 of 3 · major
The abstract's claim that the clarified role of self-gravity leads to 'new paradigms for the formation of star clusters, the stellar mass function, the origin of stellar rotation and binary stars' outruns the body on the last two items. §5.12 reports that Burkert & Bodenheimer's synthetic turbulent velocity fields match the observed spread in rotational-to-gravitational energy and in binary periods …
more of objection 2
… 'although the median angular momentum in the models was about an order of magnitude larger than in the observations,' and that Gammie et al. likewise 'found angular momenta larger than observed.' An order-of-magnitude normalization offset in the quantity that sets binary orbits means the shape of the distribution is reproduced while its scale is not, so 'origin of stellar rotation and binary stars' is at present a qualitative suggestion. The same calibration issue applies to §5.11, where 'roughly similar clump mass spectra' are obtained with self-gravity but no field, with a field but no self-gravity, and with both, so the IMF agreement does not discriminate among the models; the authors say as much ('difficult to disentangle them from variations resulting from numerical techniques and core definitions'). The body is appropriately careful; the abstract should be brought into line, for example by describing these as promising directions rather than as paradigms already established.
The paper says, at §3
The review did not quote this passage.
Pith says: Objection 3 of 3 · major
The ranking of energy sources, which the abstract states as a result ('Supernovae and superbubbles dominate the total power'), depends on efficiency factors that are assumed rather than derived and that differ from channel to channel. Supernova input is quoted as 3 × 10^{−26} erg cm^{−3} s^{−1} 'after multiplying by an efficiency factor of 0.1'; protostellar winds use 0.05; the …
more of objection 3
… magnetorotational rate is quoted without an efficiency; and for the gravitational channel the review states that 'the efficiency for the conversion of gravitational binding energy into turbulence is unknown, but ... the efficiency might be high.' Since the spiral-shock and gravitational rates (5 × 10^{−27} and 10^{−27} erg cm^{−3} s^{−1}) are within an order of magnitude of the supernova rate before such factors are applied, the conclusion that stellar explosions dominate is conditional on the assumed efficiencies. Please state the sensitivity explicitly, ideally as a short table of raw versus efficiency-weighted rates with the adopted factor and its provenance for each source, so that the reader can see how much the ranking could move.
7 minor objections
The paper says, at §2, Eq. (3)
Pith says: minor objection 1 of 7
The power spectrum is written as P(k) = Â(k)Â(k)*; it should be |Â(k)|², since the product as written is not manifestly real and positive.
The paper says, at §2, Eqs. (4)–(5)
Pith says: minor objection 2 of 7
The unsharp-mask function in Eq. (5) is introduced without motivation for the specific normalization (π(L/2)^{−2}) or for the −0.125 value in the annulus; one sentence explaining that the mask is normalized to zero integral would make the delta-variance definition usable without consulting Stützki et al. (1998).
show 5 more
The paper says, at §2
Pith says: minor objection 3 of 7
'Principle component analysis' should read 'Principal component analysis.'
The paper says, at §4.6
Pith says: minor objection 4 of 7
The statement that for compressible ISM turbulence 'the term inertial range is meaningless' is strong and sits in tension with the robust multi-decade power laws reported in §2 and §6. The tension is acknowledged in §6 as an open question, but a forward reference at §4.6 would prevent the reader from taking the two passages as contradictory.
The paper says, at §4.13, Eq. (15)
Pith says: minor objection 5 of 7
The fitted three-dimensional power spectrum is given with an exponential factor in k‖/k⊥^{2/3}; please state the fitting range in k and whether the same functional form was applied to the compressible and incompressible runs, since the codimension quoted in the surrounding text differs between them.
The paper says, at References
Pith says: minor objection 6 of 7
Several claims rest on items listed as in press or in preparation, notably Falgarone, Hily-Blant & Levrier (2003) for the scale-independence of power density in §3 and Falgarone et al. (2004) for the ~1% line-of-sight filling factor of dissipation regions in §4.7; please update the bibliographic status at proof.
The paper says, at §5.1
Pith says: minor objection 7 of 7
The Reynolds-number discussion would be easier to use if the resolution requirement were stated once in a single place for the compressible MHD case, rather than split between the Re^{9/4} scaling argument and the ambipolar-diffusion estimate of Eq. (18).
What would settle it
Recompute, from the published synthetic velocity fields of Burkert & Bodenheimer (2000) and the Gammie et al. (2003) core catalogues, the median specific angular momentum and the rotational-to-gravitational energy ratio distribution, and compare them against the observed distributions of Goodman et al. (1993) and Caselli et al. (2002) using the same core-size cuts. If the simulated median specific angular momentum exceeds the observed median by roughly the factor of ten that §5.12 reports, then the turbulence origin of stellar rotation and binary orbits is not established at the quantitative level and abstract:s8 should be softened to a suggestion. A parallel check: recompute the §5.11 clump mass spectrum slope under two different clump-finding definitions; if the slope shifts by more than the observational IMF uncertainty, the 'IMF from turbulence' claim is definition-dependent rather a
from the skeptic's reading
How the review went
4 readings by deepseek-v4.1-flash · 13 Nov 2026
- Reader holds up
- Skeptic partly agrees
- Editor wrote the verdict above
- Referee minor revision: 3 major objections, 7 minor
Not run on this paper: the simulated authors' defence.
Pith did not check this review's objections against the paper.
The review in full
The review in brief, machine-written
This is the review you hand a new student who needs to know what the ISM turbulence literature looked like before they start. It earns that role. The diagnostics section is the most useful part: it lays out structure functions, delta-variance, PCA, and velocity channel analysis, and then says plainly that no consistent centroid-velocity correlation has emerged inside individual clouds and that the linewidth-size relation is dominated by scatter. That kind of negative summary is rare and worth having in one place. The energy-source budget in Section 3 is concrete, with numbers per mechanism, and the theory section walks through the Kolmogorov, Iroshnikov-Kraichnan, and Goldreich-Sridhar proposals without pretending one has won. Section 5.1 states the resolution problem outright, and Section 6 closes with a list of open questions plus the admission that 'our current embrace of turbulence theory... may be partly based on an overly-simplification of available models.' That is the authors marking their own limits, and it should be credited. Note also that the classifier record says no limitations were found; that is simply wrong, and you should not repeat it. The soft spot is abstract:s8. The first half, that self-gravity is confined to turbulence-produced cores, is well supported by the nongravitating MHD simulations cited in Section 5.10. The extension to stellar rotation and binary stars is not. Section 5.12 reports that Burkert & Bodenheimer and Gammie et al. reproduce the shape of the angular momentum distribution while overshooting its median by roughly an order of magnitude, and Section 5.11 concedes that similar clump mass spectra appear with gravity alone, fields alone, or both, with differences hard to separate from numerics. A result that any configuration reproduces does not discriminate mechanisms. Both caveats are stated in the body; neither reaches the abstract. That is an oversell, not a fabrication, and it is the one place where a reader skimming will be misled. Everything else holds up as a 2004 synthesis, and it is now a period piece on the points it flags as unsettled. Cite it as the entry point and for the diagnostics taxonomy. It deserved referees then and it is worth your time now.
The strongest objection
The classifier selects abstract:s8 as the main claim: that the role of self-gravity in turbulent gas is 'clarified, leading to new paradigms' for star clusters, the IMF, stellar rotation, and binary stars. The first half of that claim is well supported by cited published work — §5.10 lists nongravitating MHD simulations that reproduce extinction statistics, the B–n correlation, the size–linewidth relation, and core rotation, which is exactly the evidence needed to argue that gravity is not the primary shaper of cloud structure. The extension to rotation and binaries is where the support thins. §5.12 reports that Burkert & Bodenheimer's (2000) synthetic turbulent velocity fields reproduce the observed spread in rotational-to-gravitational energy and in binary periods, 'although the median angular momentum in the models was about an order of magnitude larger than in the observations,' and that Gammie et al. (2003) likewise 'found angular momenta larger than observed.' An order-of-magnitude normalization error in the very quantity that sets binary orbits is not a detail; it means the simulations reproduce the shape of the distribution while missing its scale, so the claim that turbulence explains the origin of stellar rotation and binary stars is at present a qualitative suggestion, not a demonstrated result. The same pattern appears in §5.11: 'roughly similar clump mass spectra' arise with self-gravity but no magnetic fields, with magnetic fields but no self-gravity, and with both, and the authors concede that differences 'are difficult to disentangle... from variations resulting from numerical techniques and core definitions.' A result that any configuration reproduces does not discriminate among the mechanisms, so it cannot carry the weight the abstract places on it. Neither caveat is dishonest — both are stated in the body — but neither is carried into abstract:s8, which is the sentence a reader will take away.
The reader's verdict of ACCEPT at high confidence is right for what this paper is. It is a review, the full text is available, and the authors state their limitations repeatedly and specifically — the non-convergence of adaptive-mesh simulations under a twofold resolution increase (§5.1, citing de Avillez & Breitschwerdt 2003), the narrow density range over which isothermality holds and its suppression of baroclinic vorticity (§4.5), the absence of any definitive linewidth–size characterisation (§2), and the closing admission that 'our current embrace of turbulence theory... may be partly based on an overly-simplification of available models' (§6). The classifier record's 'Limitations the authors state: (none found)' is simply wrong, and the reader correctly overrode it. I therefore do not treat the resolution and Reynolds-number extrapolation as a new finding; the reader's weakest_assumption identifies it accurately and the authors own it. Where I part company with the reader is on which concern is sharpest. The reader's framing — that finite-resolution, isothermal, Fourier-forced simulations may not represent Re ~ 10^5–10^7 — is correct but diffuse, and because the authors concede it in §5.1 it does not move the verdict. The more specific and less-acknowledged soft spot is the mismatch between abstract:s8 and §5.12: the review claims a clarified origin for stellar rotation and binary stars on the strength of simulations whose median angular momentum is an order of magnitude too large, a discrepancy the authors report in the body but do not let temper the abstract. The §5.11 clump-spectrum result compounds this, since it appears with and without self-gravity and with and without magnetic fields, making it non-discriminating. Both are framing problems at the abstract level rather than errors in the review's substance, which is why my recommendation is UNCHANGED rather than a downgrade: the body text is honest, the caveats are present, and a review is entitled to summarise a field's working hypotheses as paradigms provided the body carries the qualifications. The concrete test above would settle whether the angular-momentum gap is a normalization artefact of the comparison or a genuine failure of the turbulence picture at binary-orbit scales; if the latter, the abstract sentence should be softened, and that is the only change I would ask for. Credit where due: the review's core structural claim — that supersonic turbulence reproduces the observed 2D intensity power spectra near −2.8 to −3.2, the hierarchical filaments, and the lognormal density PDF — rests on multiple independent published simulation and observational programmes, and the authors are careful to flag where the MHD energy spectrum remains unsettled (§6). That part of the synthesis holds up under scrutiny; the concern lands only on the four-item 'new paradigms' list in the abstract, and only on two of the four items within it.
The referee's report
As a synthesis the review is unusually well calibrated: it separates observation from simulation at every step (for example, §2 sets observed line-profile smoothness against the jagged profiles produced by large-scale-forced Mach 10–15 simulations, and §5.3 distinguishes decaying from uniformly forced dissipation statistics), it states plainly where the standard machinery fails (the loss of kinetic-energy conservation and hence of the inertial range in compressible flow, §4.5–4.6), and it offers falsifiable predictions (a nearly universal lognormal density PDF in isothermal gas, crossing-time decay, transient clouds). The internal arithmetic is consistent where it can be checked: the Politano–Pouquet form in Eq. (17) reduces correctly to She–Leveque for g = 3, x = 2/3, C = 2, and the cascade-rate arguments of §4.12 reproduce the k^{−2}, k^{−3/2}, and k^{−5/3} limits correctly. The quantitative power-input budget of §3 and the explicit statement of the Reynolds-number ceiling in §5.1 are the kind of bookkeeping that makes the review useful as a reference.
Pith's reading of the paper (a machine's summary, not the authors')
This review sets out to establish that the interstellar medium is not a collection of long-lived clouds in pressure equilibrium but a supersonically turbulent, magnetized medium stirred over a wide range of scales, chiefly by supernovae and superbubbles. It gathers the observational diagnostics—structure functions, power spectra, linewidths, and line profiles—and argues that the observed power-law intensity spectra, hierarchical filaments, and non-Gaussian velocity statistics are what turbulence produces. It then reviews simulations showing that supersonic MHD turbulence decays in roughly a crossing time, that isothermal gas develops a roughly lognormal density probability distribution, and that self-gravity matters mainly in the densest cores that turbulence itself creates. If the synthesis holds, clouds are transient, star formation is fast and inefficient, thermal phases are not discrete equilibrium states, and magnetic fields do not support clouds against collapse.
What carries the argument. The load-bearing machinery is the combination of supersonic turbulence theory, MHD cascade models, and numerical simulations, joined by the density probability distribution function (PDF). Structure functions and power spectra quantify the observed scaling; the lognormal density PDF links simulation density fields to observed column densities; and turbulent fragmentation—dense cores forming in converging flows and shock intersections—is the mechanism by which turbulence creates the seeds of star formation. The review also uses the critical-balance picture of anisotropic MHD turbulence to organize predictions for energy spectra, while emphasizing that compressible turbulence lacks the conserved quadratic invariants that make the incompressible Kolmogorov cascade well defined.
Core claim. The central claim is that supersonic, magnetized turbulence is the organizing process of the cool interstellar medium. In this picture, supernovae, superbubbles, galactic rotation, and self-gravity inject motions over a broad range of scales; shocks and vortices generate the observed hierarchical filaments and power-law intensity spectra, with two-dimensional slopes around $-2.8$ to $-3.2$; and the density field in isothermal gas approaches a lognormal probability distribution. Simulations reviewed here reproduce many of these statistics, find that supersonic MHD turbulence decays in about one crossing time, and show that self-gravity takes over only in the densest, short-lived cores produced by the turbulence. The authors use this to argue that clouds are transient, that star formation is fast and inefficient, and that the classical picture of discrete thermal phases in pressure equilibrium must be replaced by a turbulent medium.
The premise it rests on. The synthesis depends on the assumption that simulations at accessible resolution, with idealised forcing and often an isothermal equation of state, faithfully represent an interstellar medium with Reynolds numbers of order $10^5$ to $10^7$.
If the paper is right (Pith's inferences, not the authors')
Molecular clouds should be short-lived, dispersing in roughly a turbulent crossing time rather than surviving as long-lived equilibrium objects.
Star formation should be fast and inefficient: only the small fraction of gas in the high-density tail of the lognormal PDF can collapse before the cloud is disrupted.
Thermal instability should not produce sharply bimodal density phases; the observed broad range of interstellar pressures and the large mass in the thermally unstable regime follow naturally from turbulence.
Magnetic fields should not act as an effective pressure that supports clouds, though they can slow local collapse, remove angular momentum, and shape filamentary accretion.
The stellar initial mass function and core mass function should reflect turbulence-produced fragmentation, with self-gravity selecting the densest cores rather than setting the overall cloud structure.
If supernovae and superbubbles dominate the power input, then low-surface-brightness and outer-disk galaxies with low star-formation rates should show weaker large-scale turbulence and systematically different cloud structure unless another driver, such as magnetorotational instability, takes over.
The transient-cloud picture implies that cloud lifetimes measured in nearby regions should correlate with the local turbulent crossing time and energy-injection rate, not with a universal virial equilibrium.
Because the density PDF is the bridge between simulations and observations, a sharper test would be to compare PDFs and power spectra from the same observed region across multiple tracers and resolutions, rather than treating each statistic separately.
If turbulence sets the core mass function, then environmental changes in Mach number and magnetic field strength should shift the IMF at the low-mass end; this is a testable extension beyond the review's synthesis.
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The paper
Abstract
This two-part review summarizes interstellar turbulence and its implications. The first part begins with diagnostics and energy sources. Turbulence theory is considered in detail, including the basic fluid equations, solenoidal and compressible modes, global inviscid quadratic invariants, scaling arguments, energy transfer and cascade, velocity probability distributions, and turbulent pressure. Theories of magnetohydrodynamic turbulence, including collisionless MHD turbulence, are discussed, emphasizing various proposals for energy spectra. A large variety of numerical simulations of interstellar turbulence are reviewed. Models have reproduced many of the basic features of the observed scaling relations, predicted fast decay rates for supersonic MHD turbulence, and derived probability distribution functions for density. Thermal instabilities and thermal phases have a new interpretation in a turbulent medium. Large-scale models with various combinations of self-gravity, magnetic fields, supernovae, and star formation are beginning to resemble the observed interstellar medium in morphology and statistical properties. The role of self-gravity in turbulent gas is clarified, leading to new paradigms for the formation of star clusters, the stellar mass function, the origin of stellar rotation and binary stars, and the effects of magnetic fields.
The paper's own sentences, arranged, kept beside the review and separate from it. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. No sentence in this record was written by a model.
abstract compiled · 2026-09-23
The authors' main claim, as the classifier picked it out 0.91
“The role of self-gravity in turbulent gas is clarified, leading to new paradigms for the formation of star clusters, the stellar mass function, the origin of stellar rotation and binary stars, and the effects of magnetic fields.”
How the main claim is stated: asserted 1.00
What the abstract itself states, as probabilities: claims first 0.06 · states limitation 0.07 · human participants 0.01 · controlled comparison 0.02 · randomized assignment 0.01 · states quantitative result 0.06 · compares with prior results 0.18 · mentions code or data availability 0.02
The abstract, sentence by sentence
This table labels the abstract only (arXiv listing abstract v1). The number is the probability the classifier gave the label.
| Sentence | Role | The authors' own work | States the main conclusion | Strength |
|---|---|---|---|---|
| This two-part review summarizes interstellar turbulence and its implications. | contribution 0.72 | 0.40 | 0.06 | asserted 0.90 |
| The first part begins with diagnostics and energy sources. | contribution 0.44 | 0.15 | 0.02 | asserted 0.94 |
| Turbulence theory is considered in detail, including the basic fluid equations, solenoidal and compressible modes, global inviscid quadratic invariants, scaling arguments, energy transfer and cascade, velocity probability distributions, and turbulent pressure. | background 0.46 | 0.10 | 0.03 | asserted 0.90 |
| Theories of magnetohydrodynamic turbulence, including collisionless MHD turbulence, are discussed, emphasizing various proposals for energy spectra. | background 0.47 | 0.10 | 0.03 | asserted 0.87 |
| A large variety of numerical simulations of interstellar turbulence are reviewed. | method 0.44 | 0.10 | 0.02 | asserted 0.98 |
| Models have reproduced many of the basic features of the observed scaling relations, predicted fast decay rates for supersonic MHD turbulence, and derived probability distribution functions for density. | result 0.76 | 0.12 | 0.11 | asserted 1.00 |
| Thermal instabilities and thermal phases have a new interpretation in a turbulent medium. | interpretation 0.81 | 0.23 | 0.07 | asserted 0.99 |
| Large-scale models with various combinations of self-gravity, magnetic fields, supernovae, and star formation are beginning to resemble the observed interstellar medium in morphology and statistical properties. | result 0.76 | 0.12 | 0.11 | asserted 0.78 |
| The role of self-gravity in turbulent gas is clarified, leading to new paradigms for the formation of star clusters, the stellar mass function, the origin of stellar rotation and binary stars, and the effects of magnetic fields. | interpretation 0.86 | 0.27 | 0.31 | asserted 1.00 |
What kind of paper the classifier reports this is: review 1.00 · evidence from literature 1.00
What was examined, and what was not
Sources read
- arXiv listing abstract v1
Not examined
- full text
- figures and tables
- references and citing sentences
- relations to other papers
Levels run
- P abstract
Not run
- S sections
- T body sentences
- C citations
- R cross-paper relations
How the labels were made
Compiled by classifier-1.13.0 via TypeSafe API, question bank abstract-p1-20260923, 2026-09-23: 1 request, 6,854 input tokens.
Every quoted sentence on this record is the authors'. Every label is from Pith's closed vocabulary, with the probability shown beside it. This record as JSON
Figures (5)
Figures are the authors', reproduced from the paper.
References (24)
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Cited by 2 Pith papers
Reviewed papers on Pith that cite this one. The full citation record
- Single Frequency CMB Foreground Removal with Inter-scale Machine Learning astro-ph.CO · Jul 2026
- The impact of the turbulent Mach number on star formation and the initial mass function astro-ph.GA · Sep 2026
How later papers used it
229 later papers cite it
1 later paper by other authors is listed below: 1 used its data or values.
Uses its data or values 1 of 3 papers with this label
-
Used this paper's outer scale of about 100 pc, together with an RMS turbulence velocity, to estimate a turbulent diffusion coefficient of about 1 kpc^2 per Gyr.
R-process Rain from Binary Neutron Star Mergers in the Galactic Halo (2022) · 0.87 · paraphrased: the licence does not allow quoting
How the literature uses it
34 arXiv papers cite this in 42 sentences
Papers citing it · 21 sentences without a confident label
Cites it as background 19 papers
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Models of MHD turbulence predict the power spectra for these different types of modes as a function of the magnitude and orientation (with respect to the background magnetic field) of the wavevector $$ [ref] .
Dust polarization and ISM turbulence · Introduction · 0.96
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Gas in galaxies is supersonically turbulent [ref] .
Universal gravity-driven isothermal turbulence cascade in disk galaxies · Introduction · 0.95
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Following the [ref] model of turbulence, the energy injected at large scales is progressively transferred to smaller scales, until it dissipates by viscosity at much smaller scales [ref] .
Emergence of high-mass stars in complex fiber networks (EMERGE) VI. Turbulence dissipation and the formation of dense fibers · Signatures of turbulence dissipation and intermittency · 0.95
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