1989
DOI: 10.1109/20.42340
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The algebraic topology of Bloch points

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Cited by 27 publications
(16 citation statements)
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“…It can be seen that the points with M ( r )= 0 correspond to the hedgehog or antihedgehog of n ( r ) with the effective magnetic charge ( S is the surface enclosing the singularity), namely the emergent magnetic monopole and antimonople (see Fig. 1c and also Supplementary Note 1 ) 6 7 8 9 10 11 12 21 22 23 . Therefore, the strong correlation limit produces the non-trivial topological classification of the spin configurations and the topological phase transition as well.…”
Section: Resultsmentioning
confidence: 99%
See 1 more Smart Citation
“…It can be seen that the points with M ( r )= 0 correspond to the hedgehog or antihedgehog of n ( r ) with the effective magnetic charge ( S is the surface enclosing the singularity), namely the emergent magnetic monopole and antimonople (see Fig. 1c and also Supplementary Note 1 ) 6 7 8 9 10 11 12 21 22 23 . Therefore, the strong correlation limit produces the non-trivial topological classification of the spin configurations and the topological phase transition as well.…”
Section: Resultsmentioning
confidence: 99%
“…A real-space geometric arrangement of spins affects charge transport by exerting an additional quantum phase on the itinerant electrons, called Berry phase 5 , which acts as the effective magnetic field. Among topological spin orders, hedgehogs and antihedgehogs play the roles of sources or sinks of emergent field, that is, emergent monopoles or antimonopoles 6 7 . These hedgehog spin structures have been indeed realized as topological defects such as Bloch points 8 9 10 11 and singular points where magnetic skyrmions coalesce with or split from one another 12 .…”
mentioning
confidence: 99%
“…In the present paper, we use the word, (anti) monopole, to express the topological defect on the skyrmion string. Kotiuga 31,32 described the topological nature of (anti)monopole by the Hopf extension theorem of algebraic topology. (The references 33,34 give a more extensive discussion on the group theoretical description of topological matters.)…”
Section: Openmentioning
confidence: 99%
“…Thus, a BP cannot appear alone within a continuous structure: either it is created in a pair, or it enters into the sample from the boundary. 3 Experimental proofs of the existence of BP's are not numerous, but exist. Lorentz imaging of nickel thin films with an asymmetric Bloch-wall structure showed polarity reversals that imply the presence of a BP.…”
Section: Introductionmentioning
confidence: 99%