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arxiv: 2605.17004 · v1 · pith:FCAG2NVQnew · submitted 2026-05-16 · ❄️ cond-mat.stat-mech

Model of Simplicial Complexes with dimension-wise preferential attachment

Pith reviewed 2026-05-19 19:05 UTC · model grok-4.3

classification ❄️ cond-mat.stat-mech
keywords simplicial complexespreferential attachmenthigher-order networkspower-law distributionsgenerative modelsgeneralized degreegrowing networks
0
0 comments X

The pith

A simplicial complex grows when new vertices attach to existing simplexes through independent preferential attachment rules at each dimension.

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

The paper develops a generative model for growing simplicial complexes that applies preferential attachment separately for simplexes of each dimension. Attachment probabilities depend on the generalized degree within that dimension alone, without extra coupling between dimensions. This produces power-law distributions in the generalized degrees for every dimension. A reader would care because the model offers a straightforward way to create higher-order structures that match the heterogeneous connectivity seen in real systems such as social or biological networks. If the claim holds, dimension-independent rules are enough to generate scale-free properties across multiple interaction orders.

Core claim

The authors define a growing simplicial complex by beginning with a seed structure and iteratively adding new vertices that form simplexes of chosen dimensions; the probability that a new k-simplex attaches to an existing one is proportional to the current generalized degree of that existing k-simplex, and the rule operates independently for each k.

What carries the argument

Dimension-wise preferential attachment: the attachment probability for simplexes of dimension k depends solely on their own generalized degree at that dimension.

If this is right

  • Generalized degree distributions for simplexes of every dimension follow power-law tails.
  • The model generates higher-order networks whose connectivity is heterogeneous at multiple interaction orders.
  • Scale-free properties emerge across dimensions from rules that do not mix information between dimensions.
  • The construction can be used to study dynamical processes on simplicial complexes with tunable higher-order structure.

Where Pith is reading between the lines

These are editorial extensions of the paper, not claims the author makes directly.

  • Real-world many-body systems might exhibit independent scaling exponents for interactions of different orders.
  • The framework could be tested against temporal datasets that record the order of added simplexes.
  • Extensions might add rules that occasionally couple dimensions while preserving the core power-law behavior.

Load-bearing premise

Preferential attachment can be applied independently in each dimension without needing coupling terms that link different dimensions.

What would settle it

Simulations of the model produce generalized degree distributions that are not power laws, or empirical higher-order networks require measurable cross-dimensional dependencies to fit observed data.

Figures

Figures reproduced from arXiv: 2605.17004 by Diego Febbe, Duccio Fanelli, Timoteo Carletti.

Figure 1
Figure 1. Figure 1: FIG. 1: Representation of a simplex (panel a) and a simplicial complex (panel b) together [PITH_FULL_IMAGE:figures/full_fig_p006_1.png] view at source ↗
Figure 2
Figure 2. Figure 2: FIG. 2: Growing process for the simplicial complex. With probability [PITH_FULL_IMAGE:figures/full_fig_p010_2.png] view at source ↗
Figure 3
Figure 3. Figure 3: FIG. 3: Examples of various simplex generations, by varying the parameters [PITH_FULL_IMAGE:figures/full_fig_p012_3.png] view at source ↗
Figure 4
Figure 4. Figure 4: FIG. 4: Panel (a): Degree evolution of the nodes over building time for various values of [PITH_FULL_IMAGE:figures/full_fig_p013_4.png] view at source ↗
Figure 5
Figure 5. Figure 5: FIG. 5: Spectral dimensions [PITH_FULL_IMAGE:figures/full_fig_p017_5.png] view at source ↗
Figure 6
Figure 6. Figure 6: FIG. 6: Tetrahedron, basis of the new 4-dimensional structure that will be created. Here, [PITH_FULL_IMAGE:figures/full_fig_p023_6.png] view at source ↗
Figure 7
Figure 7. Figure 7: FIG. 7: The objective is to understand how to express the sum of the degrees of the links [PITH_FULL_IMAGE:figures/full_fig_p025_7.png] view at source ↗
Figure 8
Figure 8. Figure 8: FIG. 8: Here we want to express the sum of the degrees of all triangles that include node [PITH_FULL_IMAGE:figures/full_fig_p028_8.png] view at source ↗
Figure 9
Figure 9. Figure 9: FIG. 9: Here we want to express how the degree [PITH_FULL_IMAGE:figures/full_fig_p029_9.png] view at source ↗
Figure 10
Figure 10. Figure 10: FIG. 10: When a new tetrahedron is formed, three new links (dashed in the figure) appear. [PITH_FULL_IMAGE:figures/full_fig_p030_10.png] view at source ↗
Figure 11
Figure 11. Figure 11: FIG. 11: Numerical simulation results for the values of [PITH_FULL_IMAGE:figures/full_fig_p031_11.png] view at source ↗
Figure 12
Figure 12. Figure 12: FIG. 12: Plot of [PITH_FULL_IMAGE:figures/full_fig_p037_12.png] view at source ↗
read the original abstract

Network science is a powerful framework allowing to model complex systems, it is capable to describe and take into account the intricate web of connections existing among the constituting basic element of the system. Recently scholars have brought to the fore the relevance of higher-order networks, namely structures allowing to encode for many-body interaction, differently from the pairwise case handled by networks. This novel research field opens new avenues of research with applications ranging from neurosciences to social sciences; there is thus a need for generative models of higher-order network capable to reproduce features present in empirical data. In this work we present a model for growing simplicial complex rooted on a preferential attachment process acting dimension-wise, i.e., returning a power law distribution for the generalized degree of simplexes of different dimension.

Editorial analysis

A structured set of objections, weighed in public.

Desk editor's note, referee report, simulated authors' rebuttal, and a circularity audit. Tearing a paper down is the easy half of reading it; the pith above is the substance, this is the friction.

Referee Report

2 major / 2 minor

Summary. The manuscript introduces a generative model for simplicial complexes that grows by successively adding simplices of varying dimensions according to a dimension-wise preferential attachment rule. The central claim is that this process produces power-law distributions for the generalized degrees of simplices in each dimension separately.

Significance. If the power-law result can be derived rigorously, the model would supply a minimal, parameter-light mechanism for generating higher-order networks with scale-free generalized-degree statistics across dimensions. Such a construction could serve as a useful benchmark for empirical simplicial data in statistical mechanics and complex-systems modeling, especially given the explicit dimension-wise separation.

major comments (2)
  1. [Abstract and model definition] Abstract and model section: the claim that dimension-wise preferential attachment yields power-law generalized-degree distributions is asserted without any rate equation, mean-field closure, or stationary-solution derivation. The central result therefore rests on an unshown calculation.
  2. [Model definition] Model construction: attaching a d-simplex necessarily augments the generalized degrees of all its (d-1)-faces. The manuscript treats each dimension’s attachment probability as independent, yet provides no argument showing that the resulting topological correlations factor out or average to zero in the mean-field limit. This coupling is load-bearing for the independence of the per-dimension power laws.
minor comments (2)
  1. [Results/figures] The manuscript should include at least one figure comparing simulated generalized-degree histograms against the claimed power-law form, with the theoretical exponent indicated.
  2. [Notation] Notation for generalized degree and simplex incidence should be defined once at first use and used consistently thereafter.

Simulated Author's Rebuttal

2 responses · 0 unresolved

We thank the referee for their careful reading of the manuscript and for the constructive comments, which help clarify the presentation of the analytic results and the treatment of inter-dimensional effects. We address each major comment below and have revised the manuscript to incorporate the requested derivations and arguments.

read point-by-point responses
  1. Referee: [Abstract and model definition] Abstract and model section: the claim that dimension-wise preferential attachment yields power-law generalized-degree distributions is asserted without any rate equation, mean-field closure, or stationary-solution derivation. The central result therefore rests on an unshown calculation.

    Authors: We agree that the submitted version did not include an explicit derivation of the power-law distributions. The manuscript relied on numerical simulations to illustrate the emergence of power laws across dimensions. To address this, we have added a new subsection deriving the rate equations for the generalized degree of simplices in each dimension d, applying a mean-field approximation to close the equations, and solving the resulting stationary master equation to obtain the power-law form with exponent 1 + 1/α_d, where α_d is the attachment parameter for dimension d. revision: yes

  2. Referee: [Model definition] Model construction: attaching a d-simplex necessarily augments the generalized degrees of all its (d-1)-faces. The manuscript treats each dimension’s attachment probability as independent, yet provides no argument showing that the resulting topological correlations factor out or average to zero in the mean-field limit. This coupling is load-bearing for the independence of the per-dimension power laws.

    Authors: This observation correctly identifies a potential source of coupling. In the revised manuscript we have inserted a paragraph explaining that, within the mean-field limit, the expected increment to the generalized degree of a (d-1)-face arising from the attachment of a new d-simplex is proportional to the current generalized degree of that face in dimension d-1. Because the attachment probability for dimension d is itself linear in the generalized degrees of d-simplices, this contribution factors into the existing preferential-attachment term for dimension d-1 and does not introduce additional dimension-dependent correlations beyond those already captured by the per-dimension rate equations. The argument is supported by an explicit averaging step over the uniform random choice of the new simplex’s faces. revision: yes

Circularity Check

0 steps flagged

No significant circularity: power-law result derived from attachment rule via rate equations

full rationale

The paper defines a generative growth process with dimension-wise preferential attachment and derives the stationary power-law form for generalized degrees from the resulting mean-field rate equations. This is a forward derivation from the model rules rather than a re-statement of fitted inputs or self-referential definitions. No load-bearing step reduces to a self-citation chain, an ansatz smuggled via prior work, or a uniqueness theorem imported from the same authors. The topological coupling concern raised in the skeptic note pertains to the validity of the mean-field closure, not to circularity in the derivation chain itself. The model is self-contained against external benchmarks for this class of preferential-attachment constructions.

Axiom & Free-Parameter Ledger

1 free parameters · 1 axioms · 0 invented entities

The model rests on a single core attachment rule and at least one tunable parameter controlling attachment strength per dimension; no new particles or forces are postulated.

free parameters (1)
  • dimension-specific attachment probability
    Controls the strength of preferential attachment within each dimension and must be chosen to match desired exponents.
axioms (1)
  • domain assumption Preferential attachment acts independently on each dimension of the simplicial complex.
    Invoked as the defining mechanism that produces the claimed power-law distributions.

pith-pipeline@v0.9.0 · 5658 in / 1083 out tokens · 35032 ms · 2026-05-19T19:05:40.251706+00:00 · methodology

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Reference graph

Works this paper leans on

55 extracted references · 55 canonical work pages · 1 internal anchor

  1. [1]

    Emergence of scaling in random networks.science, 286(5439):509–512, 1999

    Albert-L´ aszl´ o Barab´ asi and R´ eka Albert. Emergence of scaling in random networks.science, 286(5439):509–512, 1999

  2. [2]

    Exploring complex networks.nature, 410(6825):268–276, 2001

    Steven H Strogatz. Exploring complex networks.nature, 410(6825):268–276, 2001

  3. [3]

    Statistical mechanics of complex networks.Reviews of modern physics, 74(1):47, 2002

    R´ eka Albert and Albert-L´ aszl´ o Barab´ asi. Statistical mechanics of complex networks.Reviews of modern physics, 74(1):47, 2002. 18

  4. [4]

    Oxford university press, 2010

    Mark EJ Newman.Networks: An introduction. Oxford university press, 2010

  5. [5]

    Albert-L´ aszl´ o Barabasi and Zoltan N. Oltvai. Network biology: understanding the cell’s functional organization.Nature Reviews Genetics, 5(2):101–113, 2004

  6. [6]

    Comparative analysis of existing models for power- grid synchronization.New Journal of Physics, 17(1):015012, 2015

    Takashi Nishikawa and Adilson E Motter. Comparative analysis of existing models for power- grid synchronization.New Journal of Physics, 17(1):015012, 2015

  7. [7]

    Chaos and synchronization in the ujt relaxation oscillator

    Diego Febbe, Angelo Di Garbo, Riccardo Mannella, Riccardo Meucci, and Duccio Fanelli. Chaos and synchronization in the ujt relaxation oscillator. In2024 IEEE Workshop on Com- plexity in Engineering (COMPENG), pages 1–7. IEEE, 2024

  8. [8]

    Inferring cell cycle phases from a partially temporal network of protein interactions.Cell Reports Methods, 3(2), 2023

    Maxime Lucas, Arthur Morris, Alex Townsend-Teague, Laurent Tichit, Bianca Habermann, and Alain Barrat. Inferring cell cycle phases from a partially temporal network of protein interactions.Cell Reports Methods, 3(2), 2023

  9. [9]

    Neu- roscience needs network science.Journal of Neuroscience, 43(34):5989–5995, 2023

    D´ aniel L Barab´ asi, Ginestra Bianconi, Ed Bullmore, Mark Burgess, SueYeon Chung, Tina Eliassi-Rad, Dileep George, Istv´ an A Kov´ acs, Hern´ an Makse, Thomas E Nichols, et al. Neu- roscience needs network science.Journal of Neuroscience, 43(34):5989–5995, 2023

  10. [10]

    Robustness and resilience of complex networks.Nature Reviews Physics, 6(2):114–131, 2024

    Oriol Artime, Marco Grassia, Manlio De Domenico, James P Gleeson, Hern´ an A Makse, Giuseppe Mangioni, Matjaˇ z Perc, and Filippo Radicchi. Robustness and resilience of complex networks.Nature Reviews Physics, 6(2):114–131, 2024

  11. [11]

    Epidemic spreading in scale-free net- works.Physical review letters, 86(14):3200, 2001

    Romualdo Pastor-Satorras and Alessandro Vespignani. Epidemic spreading in scale-free net- works.Physical review letters, 86(14):3200, 2001

  12. [12]

    Financial stability through the lens of complex systems.Journal of Financial Stability, 71:101228, 2024

    Grzegorz Ha laj, Serafin Martinez-Jaramillo, and Stefano Battiston. Financial stability through the lens of complex systems.Journal of Financial Stability, 71:101228, 2024

  13. [13]

    Will you take the knee? italian twitter echo chambers’ genesis during euro 2020

    Chiara Buongiovanni, Roswita Candusso, Giacomo Cerretini, Diego Febbe, Virginia Morini, and Giulio Rossetti. Will you take the knee? italian twitter echo chambers’ genesis during euro 2020. InInternational Conference on Complex Networks and Their Applications, pages 29–40. Springer, 2022

  14. [14]

    Evolution of networks with aging of sites.Physical Review E, 62(2):1842, 2000

    Sergey N Dorogovtsev and Jos´ e Fernando F Mendes. Evolution of networks with aging of sites.Physical Review E, 62(2):1842, 2000

  15. [15]

    Connectivity of growing random networks.Physical review letters, 85(21):4629, 2000

    Paul L Krapivsky, Sidney Redner, and Francois Leyvraz. Connectivity of growing random networks.Physical review letters, 85(21):4629, 2000

  16. [16]

    Networks beyond pairwise interactions: Struc- 19 ture and dynamics.Physics reports, 874:1–92, 2020

    Federico Battiston, Giulia Cencetti, Iacopo Iacopini, Vito Latora, Maxime Lucas, Alice Pata- nia, Jean-Gabriel Young, and Giovanni Petri. Networks beyond pairwise interactions: Struc- 19 ture and dynamics.Physics reports, 874:1–92, 2020

  17. [17]

    The physics of higher-order interactions in complex systems.Nature physics, 17(10):1093–1098, 2021

    Federico Battiston, Enrico Amico, Alain Barrat, Ginestra Bianconi, Guilherme Ferraz de Ar- ruda, Benedetta Franceschiello, Iacopo Iacopini, Sonia K´ efi, Vito Latora, Yamir Moreno, et al. The physics of higher-order interactions in complex systems.Nature physics, 17(10):1093–1098, 2021

  18. [18]

    What are higher-order networks?SIAM review, 65(3):686–731, 2023

    Christian Bick, Elizabeth Gross, Heather A Harrington, and Michael T Schaub. What are higher-order networks?SIAM review, 65(3):686–731, 2023

  19. [19]

    Mill´ an, Hanlin Sun, Lorenzo Giambagli, Riccardo Muolo, Timoteo Carletti, Joaqu´ ın J

    Ana P. Mill´ an, Hanlin Sun, Lorenzo Giambagli, Riccardo Muolo, Timoteo Carletti, Joaqu´ ın J. Torres, Filippo Radicchi, J¨ urgen Kurths, and Ginestra Bianconi. Topology shapes dynamics of higher-order networks.Nature Physics, pages 1–9, 2025

  20. [20]

    Two’s company, three (or more) is a simplex: Algebraic-topological tools for understanding higher-order structure in neural data

    Chad Giusti, Robert Ghrist, and Danielle S Bassett. Two’s company, three (or more) is a simplex: Algebraic-topological tools for understanding higher-order structure in neural data. Journal of computational neuroscience, 41(1):1–14, 2016

  21. [21]

    Simplicial activity driven model.Physical review letters, 121(22):228301, 2018

    Giovanni Petri and Alain Barrat. Simplicial activity driven model.Physical review letters, 121(22):228301, 2018

  22. [22]

    Simplicial contagion in temporal higher-order networks.Journal of Physics: Complexity, 2(3):035019, 2021

    Sandeep Chowdhary, Aanjaneya Kumar, Giulia Cencetti, Iacopo Iacopini, and Federico Battis- ton. Simplicial contagion in temporal higher-order networks.Journal of Physics: Complexity, 2(3):035019, 2021

  23. [23]

    Simplicial models of social contagion.Nature communications, 10(1):2485, 2019

    Iacopo Iacopini, Giovanni Petri, Alain Barrat, and Vito Latora. Simplicial models of social contagion.Nature communications, 10(1):2485, 2019

  24. [24]

    Weisfeiler and leman go neural: Higher-order graph neural networks

    Christopher Morris, Martin Ritzert, Matthias Fey, William L Hamilton, Jan Eric Lenssen, Gaurav Rattan, and Martin Grohe. Weisfeiler and leman go neural: Higher-order graph neural networks. InProceedings of the AAAI conference on artificial intelligence, volume 33, pages 4602–4609, 2019

  25. [25]

    Spectral higher-order neural networks.arXiv preprint arXiv:2603.28420, 2026

    Gianluca Peri, Timoteo Carletti, Duccio Fanelli, and Diego Febbe. Spectral higher-order neural networks.arXiv preprint arXiv:2603.28420, 2026

  26. [26]

    Turing patterns in systems with high-order interactions.Chaos, Solitons & Fractals, 166:112912, 2023

    Riccardo Muolo, Luca Gallo, Vito Latora, Mattia Frasca, and Timoteo Carletti. Turing patterns in systems with high-order interactions.Chaos, Solitons & Fractals, 166:112912, 2023

  27. [27]

    Turing patterns on discrete topologies: from networks to higher-order structures

    Riccardo Muolo, Lorenzo Giambagli, Hiroya Nakao, Duccio Fanelli, and Timoteo Carletti. Turing patterns on discrete topologies: from networks to higher-order structures. InProceed- 20 ings A, volume 480, page 20240235. The Royal Society, 2024

  28. [28]

    Diffusion-driven instability of topological signals coupled by the dirac operator.Physical Review E, 106(6):064314, 2022

    Lorenzo Giambagli, Lucille Calmon, Riccardo Muolo, Timoteo Carletti, and Ginestra Bian- coni. Diffusion-driven instability of topological signals coupled by the dirac operator.Physical Review E, 106(6):064314, 2022

  29. [29]

    Dirac signal processing of higher- order topological signals.New Journal of Physics, 25(9):093013, 2023

    Lucille Calmon, Michael T Schaub, and Ginestra Bianconi. Dirac signal processing of higher- order topological signals.New Journal of Physics, 25(9):093013, 2023

  30. [30]

    Stability of synchroniza- tion in simplicial complexes.Nature communications, 12(1):1255, 2021

    Lucia Valentina Gambuzza, Francesca Di Patti, Luca Gallo, Stefano Lepri, Miguel Romance, Regino Criado, Mattia Frasca, Vito Latora, and Stefano Boccaletti. Stability of synchroniza- tion in simplicial complexes.Nature communications, 12(1):1255, 2021

  31. [31]

    Synchronization induced by directed higher-order interactions.Communi- cations Physics, 5(1):263, 2022

    Luca Gallo, Riccardo Muolo, Lucia Valentina Gambuzza, Vito Latora, Mattia Frasca, and Timoteo Carletti. Synchronization induced by directed higher-order interactions.Communi- cations Physics, 5(1):263, 2022

  32. [32]

    Global topological synchroniza- tion on simplicial and cell complexes.Physical Review Letters, 130(18):187401, 2023

    Timoteo Carletti, Lorenzo Giambagli, and Ginestra Bianconi. Global topological synchroniza- tion on simplicial and cell complexes.Physical Review Letters, 130(18):187401, 2023

  33. [33]

    Hamiltonian control to desynchronize kuramoto oscillators with higher-order interactions.Physical Review E, 111(4):044307, 2025

    Martin Moriam´ e, Maxime Lucas, and Timoteo Carletti. Hamiltonian control to desynchronize kuramoto oscillators with higher-order interactions.Physical Review E, 111(4):044307, 2025

  34. [34]

    Cambridge University Press, 2021

    Ginestra Bianconi.Higher-order networks. Cambridge University Press, 2021

  35. [35]

    Springer, 2010

    Leo J Grady and Jonathan R Polimeni.Discrete calculus: Applied analysis on graphs for computational science, volume 3. Springer, 2010

  36. [36]

    Hodge laplacians on graphs.Siam Review, 62(3):685–715, 2020

    Lek-Heng Lim. Hodge laplacians on graphs.Siam Review, 62(3):685–715, 2020

  37. [37]

    Network geometry with flavor: from complexity to quantum geometry.Physical Review E, 93(3):032315, 2016

    Ginestra Bianconi and Christoph Rahmede. Network geometry with flavor: from complexity to quantum geometry.Physical Review E, 93(3):032315, 2016

  38. [38]

    Exponential random simplicial com- plexes.Journal of Physics A: Mathematical and Theoretical, 48(46):465002, 2015

    Konstantin Zuev, Or Eisenberg, and Dmitri Krioukov. Exponential random simplicial com- plexes.Journal of Physics A: Mathematical and Theoretical, 48(46):465002, 2015

  39. [39]

    Dorogovtsev and P

    SN Dorogovtsev and PL Krapivsky. Deterministic simplicial complexes.arXiv preprint arXiv:2507.07402, 2025

  40. [40]

    Ahorn: A Dataset of Higher-Order Networks

    Ahorn Project (RWTH Aachen University). Ahorn: A Dataset of Higher-Order Networks. https://ahorn.rwth-aachen.de/dataset

  41. [41]

    Emergent com- plex network geometry.Scientific reports, 5(1):10073, 2015

    Zhihao Wu, Giulia Menichetti, Christoph Rahmede, and Ginestra Bianconi. Emergent com- plex network geometry.Scientific reports, 5(1):10073, 2015

  42. [42]

    Emergent hyperbolic network geometry.Scientific 21 reports, 7(1):41974, 2017

    Ginestra Bianconi and Christoph Rahmede. Emergent hyperbolic network geometry.Scientific 21 reports, 7(1):41974, 2017

  43. [43]

    Simplicial complexes: higher-order spectral dimen- sion and dynamics.Journal of Physics: Complexity, 1(1):015002, 2020

    Joaqu´ ın J Torres and Ginestra Bianconi. Simplicial complexes: higher-order spectral dimen- sion and dynamics.Journal of Physics: Complexity, 1(1):015002, 2020

  44. [44]

    Generalized network structures: The configuration model and the canonical ensemble of simplicial complexes.Physical Review E, 93(6):062311, 2016

    Owen T Courtney and Ginestra Bianconi. Generalized network structures: The configuration model and the canonical ensemble of simplicial complexes.Physical Review E, 93(6):062311, 2016. [45]https://github.com/diegofebbe/Random_walk_on_simplicial_complexes/tree/ master

  45. [45]

    Complex network geometry and frustrated synchronization.Scientific reports, 8(1):9910, 2018

    Ana P Mill´ an, Joaqu´ ın J Torres, and Ginestra Bianconi. Complex network geometry and frustrated synchronization.Scientific reports, 8(1):9910, 2018

  46. [46]

    Synchronization in network geome- tries with finite spectral dimension.Physical Review E, 99(2):022307, 2019

    Ana P Mill´ an, Joaqu´ ın J Torres, and Ginestra Bianconi. Synchronization in network geome- tries with finite spectral dimension.Physical Review E, 99(2):022307, 2019

  47. [47]

    Explosive higher-order kuramoto dynamics on simplicial complexes.Physical Review Letters, 124(21):218301, 2020

    Ana P Mill´ an, Joaqu´ ın J Torres, and Ginestra Bianconi. Explosive higher-order kuramoto dynamics on simplicial complexes.Physical Review Letters, 124(21):218301, 2020

  48. [48]

    Topological thermal in- stability and length of proteins.Proteins: Structure, Function, and Bioinformatics, 55(3):529– 535, 2004

    Raffaella Burioni, Davide Cassi, Fabio Cecconi, and Angelo Vulpiani. Topological thermal in- stability and length of proteins.Proteins: Structure, Function, and Bioinformatics, 55(3):529– 535, 2004

  49. [49]

    Random Walks Across Dimensions: Exploring Simplicial Complexes

    Diego Febbe, Duccio Fanelli, and Timoteo Carletti. Random walks across dimensions: Ex- ploring simplicial complexes.arXiv preprint arXiv:2601.16086, 2026

  50. [50]

    Cambridge University Press, 2016

    Albert-L´ aszl´ o Barab´ asi.Network Science. Cambridge University Press, 2016. [52]https://github.com/diegofebbe/Random_walk_on_simplicial_complexes/tree/ master

  51. [51]

    Networks of scientific papers: The pattern of bibliographic references indicates the nature of the scientific research front.Science, 149(3683):510–515, 1965

    Derek J De Solla Price. Networks of scientific papers: The pattern of bibliographic references indicates the nature of the scientific research front.Science, 149(3683):510–515, 1965. Appendix A: Number of paths fromdtoD−1 In this section, we count the number of paths from ad-dimensional simplexσ (d) i to a (D−1)-dimensional simplexσ (D−1) i , which serves...

  52. [52]

    Since the node degree given by Eq. (B5) increases monotonically, the number of nodes having degree greater than a givenk (0) i is determined byt i =T 2 ki 1/β ,as at each time step a new node enters the simplicial complex, withTindicating the total construction time. Therefore, the probability of picking a node with degree lower thank i is P(k) = 1− 2 ki ...

  53. [53]

    General case From Secs. B 1, B 2, and B 3, we now derive a general formula describing the evolution of structures of dimensiondin cases in which simplicial complexes of dimensionDare built by settingp D = 1 in Eq. (22), withD > d. By summarizing the methods previously presented, in order to write a solvable equation for the degreek (d) i , it is crucial t...

  54. [54]

    (37) only applies to nodes that already belong to at least one triangle

    Lower degree included The two terms growth mechanisms derived from Eq. (37) only applies to nodes that already belong to at least one triangle. If a nodeiis introduced at timet i0 without being part of any triangle, thenP e∋i k(1) e = 0 for allt > t i0, and the triangle-driven growth channel is effectively suppressed. In the following, we consider a modif...

  55. [55]

    General case We now consider the general case in which simplices of different dimensions can enter the network. The evolution of the node degree can be written as dk(0) i dt = DX d=1 pd P σ(d−1)∋i k(d−1) σ P σ(d−1) k(d−1) σ .(C21) where we used the notationσ (d−1) ∋ito denote the fact that the sum is restricted to (d−1)-simplexes containing nodei. As in t...