TY - JOUR
T1 - Dislocation reactions, grain boundaries, and irreversibility in two-dimensional lattices using topological tweezers
AU - Irvine, William T.M.
AU - Hollingsworth, Andrew D.
AU - Grier, David G.
AU - Chaikin, Paul M.
PY - 2013/9/24
Y1 - 2013/9/24
N2 - Dislocations, disclinations, and grain boundaries are topological excitations of crystals that play a key role in determining outof- equilibrium material properties. In this article we study the kinetics, creation, and annihilation processes of these defects in a controllable way by applying topological tweezers, an array of weak optical tweezers which strain the lattice by weakly pulling on a collection of particles without grabbing them individually. We use topological tweezers to deterministically control individual dislocations and grain boundaries, and reversibly create and destroy dislocation pairs in a 2D crystal of charged colloids. Starting from a perfect lattice, we exert a torque on a finite region and follow the complete step-by-step creation of a disoriented grain, from the creation of dislocation pairs through their reactions to form a grain boundary and their reduction of elastic energy. However, when the grain is rotated back to its original orientation the dislocation reactions do not retrace. Rather, the process is irreversible; the grain boundary expands instead of collapsing.
AB - Dislocations, disclinations, and grain boundaries are topological excitations of crystals that play a key role in determining outof- equilibrium material properties. In this article we study the kinetics, creation, and annihilation processes of these defects in a controllable way by applying topological tweezers, an array of weak optical tweezers which strain the lattice by weakly pulling on a collection of particles without grabbing them individually. We use topological tweezers to deterministically control individual dislocations and grain boundaries, and reversibly create and destroy dislocation pairs in a 2D crystal of charged colloids. Starting from a perfect lattice, we exert a torque on a finite region and follow the complete step-by-step creation of a disoriented grain, from the creation of dislocation pairs through their reactions to form a grain boundary and their reduction of elastic energy. However, when the grain is rotated back to its original orientation the dislocation reactions do not retrace. Rather, the process is irreversible; the grain boundary expands instead of collapsing.
KW - Colloidal crystal
KW - Holographic trapping
KW - Topological defect
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U2 - 10.1073/pnas.1300787110
DO - 10.1073/pnas.1300787110
M3 - Article
C2 - 24009341
AN - SCOPUS:84884636613
SN - 0027-8424
VL - 110
SP - 15544
EP - 15548
JO - Proceedings of the National Academy of Sciences of the United States of America
JF - Proceedings of the National Academy of Sciences of the United States of America
IS - 39
ER -