Matches in SemOpenAlex for { <https://semopenalex.org/work/W2969794872> ?p ?o ?g. }
- W2969794872 abstract "We present a $4'/m'$-respecting crisscross AFM model in 2D and 3D, both belonging to the $Z_2$ classification and exhibiting interesting magnetic high-order topological insulating (HOTI) phases. The topologically nontrivial phase in the 2D model is characterized by the fractional charge localized around the corners and the quantized charge quadrupole moment. Moreover, our 2D model also exhibits the quantized magnetic quadrupole moment, which is a unique feature compared with previous studies. The 3D system stacked from layers of the 2D model possesses the HOTI phase holding chiral 1D metallic states on the hinge, which corresponds to the Wannier center flow between the valence and conduction bands. The novel transport properties such as the half-quantum spin-flop pumping phenomena on the side surfaces of the HOTI phase is also discussed." @default.
- W2969794872 created "2019-08-29" @default.
- W2969794872 creator A5012757489 @default.
- W2969794872 creator A5067905077 @default.
- W2969794872 creator A5089117299 @default.
- W2969794872 date "2019-12-23" @default.
- W2969794872 modified "2023-10-14" @default.
- W2969794872 title "Higher-order topological insulators in a crisscross antiferromagnetic model" @default.
- W2969794872 cites W1904914631 @default.
- W2969794872 cites W1983970619 @default.
- W2969794872 cites W1988579412 @default.
- W2969794872 cites W1989250610 @default.
- W2969794872 cites W1991577814 @default.
- W2969794872 cites W2001755358 @default.
- W2969794872 cites W2013282079 @default.
- W2969794872 cites W2020332193 @default.
- W2969794872 cites W2060130140 @default.
- W2969794872 cites W2077013831 @default.
- W2969794872 cites W2078822726 @default.
- W2969794872 cites W2088198211 @default.
- W2969794872 cites W2102074887 @default.
- W2969794872 cites W2117734893 @default.
- W2969794872 cites W2149260107 @default.
- W2969794872 cites W2154383866 @default.
- W2969794872 cites W2528872749 @default.
- W2969794872 cites W2595688496 @default.
- W2969794872 cites W2611523917 @default.
- W2969794872 cites W2743972233 @default.
- W2969794872 cites W2745740700 @default.
- W2969794872 cites W2746713678 @default.
- W2969794872 cites W2750111109 @default.
- W2969794872 cites W2785331841 @default.
- W2969794872 cites W2786992009 @default.
- W2969794872 cites W2790098368 @default.
- W2969794872 cites W2810574886 @default.
- W2969794872 cites W2810585930 @default.
- W2969794872 cites W2883874761 @default.
- W2969794872 cites W2884871106 @default.
- W2969794872 cites W2886358572 @default.
- W2969794872 cites W2886583066 @default.
- W2969794872 cites W2889025743 @default.
- W2969794872 cites W2897502354 @default.
- W2969794872 cites W2898913837 @default.
- W2969794872 cites W2901854059 @default.
- W2969794872 cites W2921026673 @default.
- W2969794872 cites W2923485233 @default.
- W2969794872 cites W2952781775 @default.
- W2969794872 cites W3098093725 @default.
- W2969794872 cites W3103140239 @default.
- W2969794872 cites W3103618868 @default.
- W2969794872 cites W3121845213 @default.
- W2969794872 cites W3121964595 @default.
- W2969794872 cites W326669990 @default.
- W2969794872 doi "https://doi.org/10.1103/physrevb.100.235137" @default.
- W2969794872 hasPublicationYear "2019" @default.
- W2969794872 type Work @default.
- W2969794872 sameAs 2969794872 @default.
- W2969794872 citedByCount "7" @default.
- W2969794872 countsByYear W29697948722020 @default.
- W2969794872 countsByYear W29697948722021 @default.
- W2969794872 countsByYear W29697948722022 @default.
- W2969794872 crossrefType "journal-article" @default.
- W2969794872 hasAuthorship W2969794872A5012757489 @default.
- W2969794872 hasAuthorship W2969794872A5067905077 @default.
- W2969794872 hasAuthorship W2969794872A5089117299 @default.
- W2969794872 hasBestOaLocation W29697948722 @default.
- W2969794872 hasConcept C114614502 @default.
- W2969794872 hasConcept C121332964 @default.
- W2969794872 hasConcept C128911142 @default.
- W2969794872 hasConcept C149298590 @default.
- W2969794872 hasConcept C155355069 @default.
- W2969794872 hasConcept C184720557 @default.
- W2969794872 hasConcept C188082385 @default.
- W2969794872 hasConcept C26873012 @default.
- W2969794872 hasConcept C33923547 @default.
- W2969794872 hasConcept C39984356 @default.
- W2969794872 hasConcept C44280652 @default.
- W2969794872 hasConcept C45646460 @default.
- W2969794872 hasConcept C54553102 @default.
- W2969794872 hasConcept C62520636 @default.
- W2969794872 hasConcept C84114770 @default.
- W2969794872 hasConceptScore W2969794872C114614502 @default.
- W2969794872 hasConceptScore W2969794872C121332964 @default.
- W2969794872 hasConceptScore W2969794872C128911142 @default.
- W2969794872 hasConceptScore W2969794872C149298590 @default.
- W2969794872 hasConceptScore W2969794872C155355069 @default.
- W2969794872 hasConceptScore W2969794872C184720557 @default.
- W2969794872 hasConceptScore W2969794872C188082385 @default.
- W2969794872 hasConceptScore W2969794872C26873012 @default.
- W2969794872 hasConceptScore W2969794872C33923547 @default.
- W2969794872 hasConceptScore W2969794872C39984356 @default.
- W2969794872 hasConceptScore W2969794872C44280652 @default.
- W2969794872 hasConceptScore W2969794872C45646460 @default.
- W2969794872 hasConceptScore W2969794872C54553102 @default.
- W2969794872 hasConceptScore W2969794872C62520636 @default.
- W2969794872 hasConceptScore W2969794872C84114770 @default.
- W2969794872 hasFunder F4320321001 @default.
- W2969794872 hasFunder F4320335777 @default.
- W2969794872 hasIssue "23" @default.
- W2969794872 hasLocation W29697948721 @default.