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Executive Summary Final - the Center for Nanoscale Science - an ...

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IRG2: Powered Motion at <strong>the</strong> <strong>N<strong>an</strong>oscale</strong><br />

A third area of research has been <strong>the</strong> optical<br />

control of motor behavior: <strong>the</strong> combined<br />

operation of cyclic chemical reactions <strong>an</strong>d<br />

propulsive motion in coupled populations of Ag/<br />

AgCl particles that engage in periodic clumping<br />

<strong>an</strong>d explosion in a complex non-linear fashion,<br />

with nearby clusters dynamically triggering <strong>the</strong><br />

explosions of nearby clusters in novel reaction<br />

waves of a mixed character: part homogeneous<br />

solution <strong>an</strong>d part particle-surface mediated. The<br />

figure at right – which depicts <strong>the</strong> probability that<br />

a cluster will explode given that a cluster has<br />

previously exploded a dist<strong>an</strong>ce R away at <strong>the</strong><br />

specified time in <strong>the</strong> past, provides proof of<br />

cluster-cluster interaction: <strong>the</strong> peak <strong>for</strong> a 0.2 s delay at around 20 microns clearly indicates<br />

cluster-cluster correlations. The overlap of ion gradients of nearby particles produces a<br />

particularly strong motor-motor coupling in <strong>the</strong>se systems, with enticing prospects to exhibit<br />

collective behaviors including particle-reaction waves, bistability, etc.<br />

In <strong>the</strong> catalytic motor are as a whole, in 2010 we have discovered <strong>the</strong> first examples of n<strong>an</strong>o/<br />

micro-objects outside living systems that move autonomously by converting chemical energy<br />

into mech<strong>an</strong>ical <strong>for</strong>ces. With very little “in<strong>for</strong>mation” input (in <strong>the</strong> <strong>for</strong>m of gradients), <strong>the</strong>se<br />

objects begin to display emergent collective behavior that were thought to lie solely in <strong>the</strong> realm<br />

of biology. Freed of usual biological constraints, we now have <strong>the</strong> unprecedented opportunity to<br />

probe <strong>the</strong> ultimate limits of self-org<strong>an</strong>ization in <strong>the</strong>se dynamic systems that operate far from<br />

equilibrium. Our eventual goal is to develop “intelligent” n<strong>an</strong>o/microbots that c<strong>an</strong> sense <strong>the</strong>ir<br />

environment, communicate <strong>the</strong> in<strong>for</strong>mation to o<strong>the</strong>r bots, <strong>an</strong>d induce swarming behavior in<br />

heterogeneous populations of <strong>the</strong>se bots to produce pre-determined functional outcomes.<br />

At smaller length scales, molecular motors designed to exhibit controlled mech<strong>an</strong>ical motions<br />

on <strong>the</strong> molecular scale present promising possibilities of building novel functional materials <strong>an</strong>d<br />

to extend ideas of catalytically-powered motion – already developed in solution on <strong>the</strong> singlemolecule<br />

level in <strong>the</strong> work described above – to molecular systems that are harnessed to<br />

substrates or within active materials. Our research in molecular motors aims towards assembling<br />

various single-molecule motors in well-defined n<strong>an</strong>oscale assemblies on surfaces to induce<br />

controlled motion with light, electrons, <strong>an</strong>d ions, <strong>an</strong>d to harness <strong>the</strong>se motions towards<br />

applications in n<strong>an</strong>o-electro-mech<strong>an</strong>ical systems <strong>an</strong>d n<strong>an</strong>ophotonics.<br />

As with catalytic motors, we have had several signific<strong>an</strong>t accomplishments in molecular motors<br />

project over <strong>the</strong> past year. First, we have discovered that <strong>the</strong> structure of specially designed<br />

rotax<strong>an</strong>e molecules c<strong>an</strong> be ch<strong>an</strong>ged reversibly between two (or more) stable states by employing<br />

a redox reaction. We used <strong>the</strong> n<strong>an</strong>oscale motion induced within <strong>the</strong> molecule to generate<br />

microscale motions by arr<strong>an</strong>ging <strong>the</strong>m to work in unison. In order to control <strong>the</strong> motion <strong>an</strong>d<br />

orientation, we also studied <strong>the</strong> con<strong>for</strong>mational ch<strong>an</strong>ges in rotax<strong>an</strong>es at <strong>the</strong> single-molecule level<br />

<strong>an</strong>d observed that con<strong>for</strong>mational ch<strong>an</strong>ges correlate with <strong>the</strong> known redox states of rotax<strong>an</strong>es.

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