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As described in Ref. (see also supplemental material), C is renormalized to a smaller value by bending fluctuations. We use C calculated from the torque measured in the experiment, which gives its renormalized value.
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As described in Ref. (see also supplemental material), C is renormalized to a smaller value by bending fluctuations. We use C calculated from the torque measured in the experiment, which gives its renormalized value.
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70350527907
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See EPAPS Document No. E-PLEEE8-80-R06910 for supplemental material. For more information on EPAPS, see
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See EPAPS Document No. E-PLEEE8-80-R06910 for supplemental material. For more information on EPAPS, see http://www.aip.org/pubservs/epaps.html.
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70350549088
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The language of phase coexistence is approximate in that the finite barrier to nucleation in one-dimensional systems precludes a true (sharp) phase transition.
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The language of phase coexistence is approximate in that the finite barrier to nucleation in one-dimensional systems precludes a true (sharp) phase transition.
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We have also explored increasing the entropic repulsion by a constant factor of up to 3. Though this does bring the torques closer to the experiment, the only other significant change is a decrease in F0 (data not shown)-specifically, this does not change the discussed discrepancies between the simulation and experiment.
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We have also explored increasing the entropic repulsion by a constant factor of up to 3. Though this does bring the torques closer to the experiment, the only other significant change is a decrease in F0 (data not shown)-specifically, this does not change the discussed discrepancies between the simulation and experiment.
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70350526175
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Though the 4.2 kbp z0 data alone would be arguably consistent with the model predictions, the 2.2 kbp data highlights the discrepancy at small applied forces.
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Though the 4.2 kbp z0 data alone would be arguably consistent with the model predictions, the 2.2 kbp data highlights the discrepancy at small applied forces.
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