A formalism for nemato-elasticity enforces Saint Venant compatibility via a helical basis, yielding direction-selective criticality and defect-induced random fields as universal features of crystalline systems.
Compatible Instability: Gauge Constraints of Elasticity Inherited by Electronic Nematic Criticality
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abstract
Electronic nematicity is widely observed in quantum materials with varying degrees of electronic correlation, manifesting through charge, spin, orbital, or superconducting degrees of freedom. A phenomenological model capable of describing this broad set of systems must also account for nemato-elasticity, by which nematic and elastic degrees of freedom become intertwined. However, being a tensor gauge field theory, elasticity must satisfy the compatibility relations which guarantee the integrability of lattice deformations. Here, we develop a formalism for nemato-elasticity that manifestly respects the elastic compatibility relations. We show that these constraints bifurcate the phase space of nematic fluctuations into two orthogonal sectors: one compatible and thus critical, the other incompatible and therefore gapped. The suppression of the latter leads to universal direction-selective nematic criticality in any crystal lattice. Moreover, the critical nematic modes are protected from pinning effects induced by microscopic defect strains, which necessarily induce both longitudinal and transverse correlated random fields. Finally, our results also reconcile seemingly contradictory nematic phenomena, such as the mean-field character of the nematic transition and the widespread presence of domain formation.
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Nematic order competes with d-wave superconductivity via a first-order transition but coexists with s-wave pairing in a 2D electron gas with quadrupolar interactions, producing mixed phases at finite temperature.
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Theory of Electronic Nematic Criticality Constrained by Elastic Compatibility
A formalism for nemato-elasticity enforces Saint Venant compatibility via a helical basis, yielding direction-selective criticality and defect-induced random fields as universal features of crystalline systems.
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Competition and coexistence of superconductivity and nematic order in a two-dimensional electron gas with quadrupolar interactions
Nematic order competes with d-wave superconductivity via a first-order transition but coexists with s-wave pairing in a 2D electron gas with quadrupolar interactions, producing mixed phases at finite temperature.