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Hartmann R, Singh PK, Pearce P, Mok R, Song B, Díaz-Pascual F, Dunkel J, and Drescher K, 2018.
Emergence of three-dimensional order and structure in growing biofilms, Nat. Phys. 15: 251–256
Harvey CW, Alber M, Tsimring LS, and Aranson IS, 2013. Continuum modeling of myxobacteria
clustering, New J. Phys. 15: 035029
Haupt M and Hauser MJB, 2020. Effective mixing due to oscillatory laminar flow in tubular networks of plasmodial slime moulds, New J. Phys. 22: 053007
Helbing D and Molnár P, 1995. Social force model for pedestrian dynamics, Phys. Rev. E 51:
4282–4286
Helbing D, Farkas I, and Vicsek T, 2000. Simulating dynamical features of escape panic, Nature
407: 487–490
Herant M and Dembo M, 2010. Form and function in cell motility: from fibroblasts to keratocytes,
Biophys. J. 98: 1408–1417
Herrera-Perez R and Kasza KE, 2019. Manipulating the Patterns of Mechanical Forces That Shape
Multicellular Tissues, Physiology 34: 381–391
Hoffman BD, Grashoff C, and Schwartz MA, 2011. Dynamic molecular processes mediate cellular
mechanotransduction, Nature 475: 316–323
Hofhuis H, . . . , Hay A (15 coauthors), 2016. Morphomechanical Innovation Drives Explosive Seed
Dispersal, Cell 166: 222–233
Hofmeister WFB, 1868. Allgemeine Morphologie der Gewächse, Handbuch der Physiologischen
Botanik 1: 394–553, Engelmann, Leipzig
Hohenberg PC and B. I. Halperin PI, 1977. Theory of Dynamic Critical Phenomena, Rev. Mod.
Phys. 49: 435 –479
Hohng S, Zhou R, Nahas MK, Yu J, Schulten K, Lilley DMJ, and Ha T, 2007. Fluorescence-force
spectroscopy maps two-dimensional reaction landscape of the Holliday junction, Science 318:
279–283
Holmes WR and Edelstein-Keshet L, 2012. A comparison of computational models for eukaryotic
cell shape and motility, PLoS Comput. Biol. 8: e1002793
Holtfreter JF, 1988. A New Look at Spemann’s Organizer, Developmental Biology, ed. Browder
LW, 5: 127–150, Plenum Press, New York
Howard J, 2001. Mechanics of Motor Proteins and the Cytoskeleton, Sinauer Associates, Sunderland MA
Hu J, Yang M, Gompper G, and Winkler RG, 2015. Modelling the mechanics and hydrodynamics
of swimming E. coli, Soft Matter, 11: 7867–7876
Huang C, Lv J-a, Tian X, Wang Y, Yu Y, and Jie Liu J, 2015. Miniaturized Swimming Soft Robot
with Complex Movement Actuated and Controlled by Remote Light Signals, Sci. Rep. 5: 17414
Ibrahim Y and Liverpool TB, 2016. How walls affect the dynamics of self-phoretic microswimmers,
Eur. Phys. J. Spec. Top. 225: 1843–1874
Ideses Y, Brill-Karniely Y, Haviv L, Ben-Shaul A, and Bernheim-Groswasser A, 2008. Arp2/3
Branched Actin Network Mediates Filopodia-Like Bundles Formation In Vitro, PLos One 3: e3297
Ideses Y, Erukhimovitch V, Brand R, Jourdain D, Salmeron Hernandez J, Gabinet UR, Safran
SA, Kruse K, and Bernheim-Groswasser A, 2018. Spontaneous buckling of contractile poroelastic
actomyosin sheets, Nat. Commun. 9: 2461
Ihle T, 2011. Kinetic Theory of Flocking: Derivation of Hydrodynamic Equations, Phys. Rev. E 83:
030901
209
Hartmann R, Singh PK, Pearce P, Mok R, Song B, Díaz-Pascual F, Dunkel J, and Drescher K, 2018.
Emergence of three-dimensional order and structure in growing biofilms, Nat. Phys. 15: 251–256
Harvey CW, Alber M, Tsimring LS, and Aranson IS, 2013. Continuum modeling of myxobacteria
clustering, New J. Phys. 15: 035029
Haupt M and Hauser MJB, 2020. Effective mixing due to oscillatory laminar flow in tubular networks of plasmodial slime moulds, New J. Phys. 22: 053007
Helbing D and Molnár P, 1995. Social force model for pedestrian dynamics, Phys. Rev. E 51:
4282–4286
Helbing D, Farkas I, and Vicsek T, 2000. Simulating dynamical features of escape panic, Nature
407: 487–490
Herant M and Dembo M, 2010. Form and function in cell motility: from fibroblasts to keratocytes,
Biophys. J. 98: 1408–1417
Herrera-Perez R and Kasza KE, 2019. Manipulating the Patterns of Mechanical Forces That Shape
Multicellular Tissues, Physiology 34: 381–391
Hoffman BD, Grashoff C, and Schwartz MA, 2011. Dynamic molecular processes mediate cellular
mechanotransduction, Nature 475: 316–323
Hofhuis H, . . . , Hay A (15 coauthors), 2016. Morphomechanical Innovation Drives Explosive Seed
Dispersal, Cell 166: 222–233
Hofmeister WFB, 1868. Allgemeine Morphologie der Gewächse, Handbuch der Physiologischen
Botanik 1: 394–553, Engelmann, Leipzig
Hohenberg PC and B. I. Halperin PI, 1977. Theory of Dynamic Critical Phenomena, Rev. Mod.
Phys. 49: 435 –479
Hohng S, Zhou R, Nahas MK, Yu J, Schulten K, Lilley DMJ, and Ha T, 2007. Fluorescence-force
spectroscopy maps two-dimensional reaction landscape of the Holliday junction, Science 318:
279–283
Holmes WR and Edelstein-Keshet L, 2012. A comparison of computational models for eukaryotic
cell shape and motility, PLoS Comput. Biol. 8: e1002793
Holtfreter JF, 1988. A New Look at Spemann’s Organizer, Developmental Biology, ed. Browder
LW, 5: 127–150, Plenum Press, New York
Howard J, 2001. Mechanics of Motor Proteins and the Cytoskeleton, Sinauer Associates, Sunderland MA
Hu J, Yang M, Gompper G, and Winkler RG, 2015. Modelling the mechanics and hydrodynamics
of swimming E. coli, Soft Matter, 11: 7867–7876
Huang C, Lv J-a, Tian X, Wang Y, Yu Y, and Jie Liu J, 2015. Miniaturized Swimming Soft Robot
with Complex Movement Actuated and Controlled by Remote Light Signals, Sci. Rep. 5: 17414
Ibrahim Y and Liverpool TB, 2016. How walls affect the dynamics of self-phoretic microswimmers,
Eur. Phys. J. Spec. Top. 225: 1843–1874
Ideses Y, Brill-Karniely Y, Haviv L, Ben-Shaul A, and Bernheim-Groswasser A, 2008. Arp2/3
Branched Actin Network Mediates Filopodia-Like Bundles Formation In Vitro, PLos One 3: e3297
Ideses Y, Erukhimovitch V, Brand R, Jourdain D, Salmeron Hernandez J, Gabinet UR, Safran
SA, Kruse K, and Bernheim-Groswasser A, 2018. Spontaneous buckling of contractile poroelastic
actomyosin sheets, Nat. Commun. 9: 2461
Ihle T, 2011. Kinetic Theory of Flocking: Derivation of Hydrodynamic Equations, Phys. Rev. E 83:
030901