2020
DOI: 10.21468/scipostphys.8.4.065
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On duality between Cosserat elasticity and fractons

Abstract: We present a dual formulation of the Cosserat theory of elasticity. In this theory a local element of an elastic body is described in terms of local displacement and local orientation. Upon the duality transformation these degrees of freedom map onto a coupled theory of a vector-valued one-form gauge field and an ordinary U (1) gauge field. We discuss the degrees of freedom in the corresponding gauge theories, the defect matter and coupling to the curved space.

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Cited by 45 publications
(27 citation statements)
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“…For example, in certain fracton models, the restricted mobility of excitations can formally be understood as a consequence of the fact that the many-body dynamics conserves not only the total charge density of fractons, but also the total dipole moment (or higher multipole moment) associated with this charge [50][51][52]. Systems with such conservation laws naturally couple to symmetric tensor gauge theories [53][54][55], just like theories of classical or quantum elasticity [56][57][58][59][60][61][62][63][64][65][66][67]. Other fracton models are understood by duality to systems with subsystem symmetries [68].…”
Section: Introductionmentioning
confidence: 99%
“…For example, in certain fracton models, the restricted mobility of excitations can formally be understood as a consequence of the fact that the many-body dynamics conserves not only the total charge density of fractons, but also the total dipole moment (or higher multipole moment) associated with this charge [50][51][52]. Systems with such conservation laws naturally couple to symmetric tensor gauge theories [53][54][55], just like theories of classical or quantum elasticity [56][57][58][59][60][61][62][63][64][65][66][67]. Other fracton models are understood by duality to systems with subsystem symmetries [68].…”
Section: Introductionmentioning
confidence: 99%
“…This connection is made precise via a duality transformation, often referred to as "fracton-elasticity duality," which maps the elasticity theory of crystals onto a symmetric tensor gauge theory [9]. We discuss this duality in detail in Section V, along with its various generalizations [41][42][43][44][45][46][47]. For example, the duality can be extended to three-dimensional elasticity theory, giving rise to the concept of fractonic lines, i.e line-like excitations without the ability to move [41].…”
mentioning
confidence: 99%
“…Using Eqs. (6.4), (6.5), we can solve the dynamical Ehrenfest constrain (6.6) by introducing an additional u(1) gauge field b µ [69,73]…”
Section: Vortex Crystalmentioning
confidence: 99%
“…Moreover, a disclination dipole is equivalent to a dislocation, with the Burgers vector perpendicular to the dipole moment. The duality has been generalized in several different directions and was used to revisit the melting transition in quantum crystals [70][71][72][73]. It was also generalized to three spatial dimensions [74] and to quantum smectic phases [75], that are dual to more general multipole theories studied in [76][77][78].…”
Section: Introductionmentioning
confidence: 99%