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Self-interaction in Bopp-Podolsky electrodynamics: Spacetimes with angular defects of a charge at rest for the spacetimes with topological defects of two types: for the axially symmetric
COMPLEX DYNAMICS OF THE CASCADE OF KINK-ANTIKINK INTERACTIONS IN A LINEAR DEFECT OF THE ELECTROCONVECTIVE STRUCTURE OF A NEMATIC LIQUID CRYSTAL, the linear defect with the topological charge S = −1 begins to oscillate and decays into an odd number
COMPLEX DYNAMICS OF THE CASCADE OF KINK-ANTIKINK INTERACTIONS IN A LINEAR DEFECT OF THE ELECTROCONVECTIVE STRUCTURE OF A NEMATIC LIQUID CRYSTAL, the linear defect with the topological charge S = −1 begins to oscillate and decays into an odd number
Towards comprehension of the surface state properties in the intrinsic magnetic topological insulators topological insulators are far from being fully understood. Motivated by recent controversial ARPES results
To the Intrinsic Magnetism of the Bi108 Sn0.02 Sb0.9 Te2 S Topological Insulator, originating from the nonmagnetic structural defects of Bi1.08Sn0.02Sb0.9Te2S topological insulator form
A multidimensional global monopole and nonsingular cosmology strength, the monopole is shown to be asymptotically flat up to a solid angle defect. In the range d - 1
Response evolution of a tetrachiral metamaterial unit cell under architectural transformations. This architectural transformation is considered as a topological defect, which enhances the twisting effect
On structural defect generation induced by thermal fluctuations in materials with a perfect lattice under dynamic loadingThe possibility of structural defect generation induced by thermal fluctuations in single cryctals
Self-action in gravity, topological defects, and wormholes.
Nickel-p-block metal mixed chalcogenides based on AuCu3-type fragments: Iodine-assisted synthesis as a way of obtaining new structures-centered nickel cuboctahedra, alternating along the c axis with defective Cu2Sb-type nickel-chalcogen ones. Both
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