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collective dynamics of swimming bacteria, Phys. Rev. Lett. 98: 158102
Sokolov A, Apodacac MM, Grzybowski BA, and Aranson IS, 2010. Swimming bacteria power
microscopic gears, Proc. Natl. Acad. Sci. USA 107: 969–974
Solon J, Kaya-Copur A, Colombelli J and Brunner D, 2009. Pulsed forces timed by a ratchet-like
mechanism drive directed tissue movement during dorsal closure, Cell 137: 1331–1342
Solon AP, Caussin JB, Bartolo D, Chat/’e H, and Tailleur J, 2015. Pattern formation in flocking
models: A hydrodynamic description, Phys. Rev. E 92: 062111
Solon AP, Chat/’e H, and Tailleur J, 2015. From Phase to Micro-Phase Separation in Flocking
Models:The Essential Role of Non-Equilibrium Fluctuations, Phys. Rev. Lett. 114: 068101
Solon AP, Fily Y, Baskaran A, Cates ME, Kafri Y, Kadar M, and Tailleur J, 2015. Pressure is not a
state function for generic active fluids, Nat. Phys. 11: 673–678
Son K, Guasto JS and Stocker R, 2013. Bacteria can exploit a flagellar buckling instability to change
direction, Nat. Phys. 9: 494–498
Sowa Y, Rowe AD, Leake MC, Yakushi T, Homma M, Ishijima A, Berry RM, 2005. Direct observation of steps in rotation of the bacterial flagellar motor, Nature 437: 916–919
Spedding G, 2011. The cost of flight in flocks, Nature 474: 458–459
Spemann H and Mangold H, 1924. Induction of embryonic primordia by implantation of organizers
from a different species. Roux’s Arch. Entw. Mech. 100: 599–638
Stanton MM, Simmchen J, Ma X, Miguel-López A, and Sánchez S, 2016. Biohybrid janus motors
driven by Escherichia coli, Adv. Mater. Interf. 3: 1500505
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Stewart PS and Franklin MJ, 2008. Physiological heterogeneity in biofilms. Nat. Rev. Microbiol. 6:
199–210
Streichan SJ, Lefebvre MF, Noll N, Wieschaus EF, and Shraiman BI, 2018. Global Morphogenetic
Flow Is Accurately Predicted by the Spatial Distribution of Myosin Motors, eLife 7: e27454
Strömbom D, Siljestam M, Park J, and Sumpter DJT, 2015. The shape and dynamics of local
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Stürmer J, Seyrich M, and Stark H, 2019. Chemotaxis in a binary mixture of active and passive
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Sumino Y and Yoshikawa K, 2014. Amoeba-like motion of an oil droplet, Eur. Phys. J. Spec. Top.
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Sun L, Chen Z, Bian F, and Zhao Y, 2020. Bioinspired Soft Robotic Caterpillar with Cardiomyocyte
Drivers, Adv. Funct. Mater. 30: 1907820
Suzuki R and Bausch AR, 2017. The emergence and transient behaviour of collective motion in
active filament systems, Nat. Commun. 8: 41
Taber LA, 2009. Towards a unified theory for morphomechanics, Phil. Trans. R. Soc. A 367: 3555–
3583
Taber LA, Shi Y, Yang L, and Bayly PV, 2011. Poroelastic Model For Cell Crawling Including
Mechanical Coupling between Cytoskeletal Contraction and Actin Polymerization, J. Mech. Mater.
Struct. 6: 569–589
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219
Sokolov A, Aranson IS, Kessler JO and Goldstein RE, 2007. Concentration dependence of the
collective dynamics of swimming bacteria, Phys. Rev. Lett. 98: 158102
Sokolov A, Apodacac MM, Grzybowski BA, and Aranson IS, 2010. Swimming bacteria power
microscopic gears, Proc. Natl. Acad. Sci. USA 107: 969–974
Solon J, Kaya-Copur A, Colombelli J and Brunner D, 2009. Pulsed forces timed by a ratchet-like
mechanism drive directed tissue movement during dorsal closure, Cell 137: 1331–1342
Solon AP, Caussin JB, Bartolo D, Chat/’e H, and Tailleur J, 2015. Pattern formation in flocking
models: A hydrodynamic description, Phys. Rev. E 92: 062111
Solon AP, Chat/’e H, and Tailleur J, 2015. From Phase to Micro-Phase Separation in Flocking
Models:The Essential Role of Non-Equilibrium Fluctuations, Phys. Rev. Lett. 114: 068101
Solon AP, Fily Y, Baskaran A, Cates ME, Kafri Y, Kadar M, and Tailleur J, 2015. Pressure is not a
state function for generic active fluids, Nat. Phys. 11: 673–678
Son K, Guasto JS and Stocker R, 2013. Bacteria can exploit a flagellar buckling instability to change
direction, Nat. Phys. 9: 494–498
Sowa Y, Rowe AD, Leake MC, Yakushi T, Homma M, Ishijima A, Berry RM, 2005. Direct observation of steps in rotation of the bacterial flagellar motor, Nature 437: 916–919
Spedding G, 2011. The cost of flight in flocks, Nature 474: 458–459
Spemann H and Mangold H, 1924. Induction of embryonic primordia by implantation of organizers
from a different species. Roux’s Arch. Entw. Mech. 100: 599–638
Stanton MM, Simmchen J, Ma X, Miguel-López A, and Sánchez S, 2016. Biohybrid janus motors
driven by Escherichia coli, Adv. Mater. Interf. 3: 1500505
Stavans J, 1993.The evolution of cellular structures, Rep. Prop. Phys. 56: 733–789
Stewart PS and Franklin MJ, 2008. Physiological heterogeneity in biofilms. Nat. Rev. Microbiol. 6:
199–210
Streichan SJ, Lefebvre MF, Noll N, Wieschaus EF, and Shraiman BI, 2018. Global Morphogenetic
Flow Is Accurately Predicted by the Spatial Distribution of Myosin Motors, eLife 7: e27454
Strömbom D, Siljestam M, Park J, and Sumpter DJT, 2015. The shape and dynamics of local
attraction, Eur. Phys. J. Spec. Top. 224: 3311–3323
Stürmer J, Seyrich M, and Stark H, 2019. Chemotaxis in a binary mixture of active and passive
particles J. Chem. Phys.Ê150: 214901
Sumino Y and Yoshikawa K, 2014. Amoeba-like motion of an oil droplet, Eur. Phys. J. Spec. Top.
223: 1345–1352
Sun L, Chen Z, Bian F, and Zhao Y, 2020. Bioinspired Soft Robotic Caterpillar with Cardiomyocyte
Drivers, Adv. Funct. Mater. 30: 1907820
Suzuki R and Bausch AR, 2017. The emergence and transient behaviour of collective motion in
active filament systems, Nat. Commun. 8: 41
Taber LA, 2009. Towards a unified theory for morphomechanics, Phil. Trans. R. Soc. A 367: 3555–
3583
Taber LA, Shi Y, Yang L, and Bayly PV, 2011. Poroelastic Model For Cell Crawling Including
Mechanical Coupling between Cytoskeletal Contraction and Actin Polymerization, J. Mech. Mater.
Struct. 6: 569–589
Tambe DT, . . . , Trepat X (12 coauthors) 2011. Collective cell guidance by cooperative intercellular
forces, Nat. Mater. 10: 469–475