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Brownian dynamics simulations demonstrating chemotactic performance
a–c Simulated trajectories of a non-motile cell, a Haloferax sp. Boulby Mine (HXBM) cell, and an E. coli cell (respectively) in a chemical gradient. d Effects of modulating τrun for chemotactic strategies as indicated. Drift speed increases until τrun ~ 10 s for bipolar and run-lengthening modes. In run-shortening mode, the optimal run duration is around τrun ~ 20 s. Error bars represent s.e.m. (standard error of the mean). e Mean-squared displacements per unit time for simulated cells. Series represent HXBM unless otherwise indicated. Molecular diffusivities are given to the right, for comparison. S.e.m. is <0.02% of the values for all but the purely diffusive case and so have been omitted. f Fractional chemotactic drift speed of HXBM. The fractional drift speed increases at low v0 before saturating at around vx ≈ 0.1v0. Error bars represent s.e.m., and the series are coloured according to the swimming modes as in panel d. g Swimming efficiency (ε) multiplied by the friction coefficient (γ), showing a broad decline in efficiency at higher speeds, consistent with the results in panel f. Error bars represent s.e.m., and the series are coloured according to the swimming modes as in panel d.

Brownian dynamics simulations demonstrating chemotactic performance a–c Simulated trajectories of a non-motile cell, a Haloferax sp. Boulby Mine (HXBM) cell, and an E. coli cell (respectively) in a chemical gradient. d Effects of modulating τrun for chemotactic strategies as indicated. Drift speed increases until τrun ~ 10 s for bipolar and run-lengthening modes. In run-shortening mode, the optimal run duration is around τrun ~ 20 s. Error bars represent s.e.m. (standard error of the mean). e Mean-squared displacements per unit time for simulated cells. Series represent HXBM unless otherwise indicated. Molecular diffusivities are given to the right, for comparison. S.e.m. is <0.02% of the values for all but the purely diffusive case and so have been omitted. f Fractional chemotactic drift speed of HXBM. The fractional drift speed increases at low v0 before saturating at around vx ≈ 0.1v0. Error bars represent s.e.m., and the series are coloured according to the swimming modes as in panel d. g Swimming efficiency (ε) multiplied by the friction coefficient (γ), showing a broad decline in efficiency at higher speeds, consistent with the results in panel f. Error bars represent s.e.m., and the series are coloured according to the swimming modes as in panel d.

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Archaea have evolved to survive in some of the most extreme environments on earth. Life in extreme, nutrient-poor conditions gives the opportunity to probe fundamental energy limitations on movement and response to stimuli, two essential markers of living systems. Here we use three-dimensional holographic microscopy and computer simulations to reve...

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