{"@context":{"@vocab":"https://cir.nii.ac.jp/schema/1.0/","rdfs":"http://www.w3.org/2000/01/rdf-schema#","dc":"http://purl.org/dc/elements/1.1/","dcterms":"http://purl.org/dc/terms/","foaf":"http://xmlns.com/foaf/0.1/","prism":"http://prismstandard.org/namespaces/basic/2.0/","cinii":"http://ci.nii.ac.jp/ns/1.0/","datacite":"https://schema.datacite.org/meta/kernel-4/","ndl":"http://ndl.go.jp/dcndl/terms/","jpcoar":"https://github.com/JPCOAR/schema/blob/master/2.0/"},"@id":"https://cir.nii.ac.jp/crid/1360004234992495872.json","@type":"Article","productIdentifier":[{"identifier":{"@type":"DOI","@value":"10.1103/physrevb.98.115150"}},{"identifier":{"@type":"URI","@value":"https://link.aps.org/article/10.1103/PhysRevB.98.115150"}},{"identifier":{"@type":"URI","@value":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevB.98.115150/fulltext"}},{"identifier":{"@type":"DOI","@value":"10.48550/arxiv.1807.01091"}}],"resourceType":"学術雑誌論文(journal article)","dc:title":[{"@value":"Unified understanding of symmetry indicators for all internal symmetry classes"}],"description":[{"notation":[{"@value":"The interplay between symmetry and topology in electronic band structures has been one of the central subjects in condensed-matter physics. Recently, it has been getting clear that a wide variety of useful information about the band topology can be extracted by focusing the symmetry representations of valence bands without computing Wilson loops. In this work, we extend the previous studies on this subject to all 10 Altland-Zirnbauer symmetry classes in each of 230 space groups. We derive various general statements that should be useful in the search for topological superconductors and topological semimetals."}]},{"notation":[{"@value":"11 pages, 4 figures, 5 tables; v3: minor changes"}]}],"creator":[{"@id":"https://cir.nii.ac.jp/crid/1380004234992495872","@type":"Researcher","foaf:name":[{"@value":"Seishiro Ono"}]},{"@id":"https://cir.nii.ac.jp/crid/1420282801184439552","@type":"Researcher","personIdentifier":[{"@type":"KAKEN_RESEARCHERS","@value":"20785323"},{"@type":"NRID","@value":"1000020785323"},{"@type":"CINII_AUTHOR_ID","@value":"DA20007159"},{"@type":"URI","@value":"https://ci.nii.ac.jp/author/DA20007159#entity"},{"@type":"URI","@value":"https://viaf.org/viaf/NII%7CDA20007159"},{"@type":"NRID","@value":"9000398812316"},{"@type":"NRID","@value":"9000404799263"},{"@type":"NRID","@value":"9000017709967"},{"@type":"NRID","@value":"9000404803675"},{"@type":"NRID","@value":"9000239645588"},{"@type":"NRID","@value":"9000326254893"},{"@type":"NRID","@value":"9000404799242"},{"@type":"NRID","@value":"9000415054269"},{"@type":"RESEARCHMAP","@value":"https://researchmap.jp/harukiwatanabe"}],"foaf:name":[{"@value":"Haruki Watanabe"}]}],"publication":{"publicationIdentifier":[{"@type":"PISSN","@value":"24699950"},{"@type":"EISSN","@value":"24699969"}],"prism:publicationName":[{"@value":"Physical Review B"}],"dc:publisher":[{"@value":"American Physical Society (APS)"}],"prism:publicationDate":"2018-09-25","prism:volume":"98","prism:number":"11","prism:startingPage":"115150"},"reviewed":"false","dc:rights":["https://link.aps.org/licenses/aps-default-license"],"url":[{"@id":"https://link.aps.org/article/10.1103/PhysRevB.98.115150"},{"@id":"http://harvest.aps.org/v2/journals/articles/10.1103/PhysRevB.98.115150/fulltext"}],"createdAt":"2018-09-25","modifiedAt":"2018-09-25","foaf:topic":[{"@id":"https://cir.nii.ac.jp/all?q=Superconductivity%20(cond-mat.supr-con)","dc:title":"Superconductivity (cond-mat.supr-con)"},{"@id":"https://cir.nii.ac.jp/all?q=Condensed%20Matter%20-%20Materials%20Science","dc:title":"Condensed Matter - Materials Science"},{"@id":"https://cir.nii.ac.jp/all?q=Condensed%20Matter%20-%20Strongly%20Correlated%20Electrons","dc:title":"Condensed Matter - Strongly Correlated Electrons"},{"@id":"https://cir.nii.ac.jp/all?q=Strongly%20Correlated%20Electrons%20(cond-mat.str-el)","dc:title":"Strongly Correlated Electrons (cond-mat.str-el)"},{"@id":"https://cir.nii.ac.jp/all?q=Condensed%20Matter%20-%20Superconductivity","dc:title":"Condensed Matter - Superconductivity"},{"@id":"https://cir.nii.ac.jp/all?q=Materials%20Science%20(cond-mat.mtrl-sci)","dc:title":"Materials Science (cond-mat.mtrl-sci)"},{"@id":"https://cir.nii.ac.jp/all?q=FOS:%20Physical%20sciences","dc:title":"FOS: Physical sciences"}],"project":[{"@id":"https://cir.nii.ac.jp/crid/1040282256950690944","@type":"Project","projectIdentifier":[{"@type":"KAKEN","@value":"17K17678"},{"@type":"JGN","@value":"JP17K17678"},{"@type":"URI","@value":"https://kaken.nii.ac.jp/grant/KAKENHI-PROJECT-17K17678/"}],"notation":[{"@language":"ja","@value":"空間群の対称性や電子数に基づいたトポロジカル半金属や量子スピン液体の一般的理解"},{"@language":"en","@value":"Unified understanding of topological semimetals and quantum spin liquids based on spatial symmetries and electronic filling"}]}],"relatedProduct":[{"@id":"https://cir.nii.ac.jp/crid/1050566774916954368","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Symmetry and Topology in Non-Hermitian Physics"}]},{"@id":"https://cir.nii.ac.jp/crid/1050576347193754624","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@language":"en","@value":"Symmetry-Based Approach to Superconducting Nodes: Unification of Compatibility Conditions and Gapless Point Classifications"}]},{"@id":"https://cir.nii.ac.jp/crid/1360004235937253376","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Structure and topology of band structures in the 1651 magnetic space groups"}]},{"@id":"https://cir.nii.ac.jp/crid/1360005519934035968","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Appearance of hinge states in second-order topological insulators via the cutting procedure"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011144237660672","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Surface State Magnetization and Chiral Edge States on Topological Insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011144282918272","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Robust doubly charged nodal lines and nodal surfaces in centrosymmetric systems"}]},{"@id":"https://cir.nii.ac.jp/crid/1360011145265105024","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Diagnosis for Nonmagnetic Topological Semimetals in the Absence of Spin-Orbital Coupling"}]},{"@id":"https://cir.nii.ac.jp/crid/1360013172519110144","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi mathvariant=\"double-struck\">Z</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>\n-enriched symmetry indicators for topological superconductors in the 1651 magnetic space groups"}]},{"@id":"https://cir.nii.ac.jp/crid/1360290617652629504","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Theory of inversion-\n<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi mathvariant=\"double-struck\">Z</mml:mi><mml:mn>4</mml:mn></mml:msub></mml:math>\n protected topological chiral hinge states and its applications to layered antiferromagnets"}]},{"@id":"https://cir.nii.ac.jp/crid/1360290617758876160","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Second-order topological non-Hermitian skin effects"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292618696471424","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mrow><mml:mo stretchy=\"false\">(</mml:mo><mml:mi>d</mml:mi><mml:mo>−</mml:mo><mml:mn>2</mml:mn><mml:mo stretchy=\"false\">)</mml:mo></mml:mrow></mml:math>\n-Dimensional Edge States of Rotation Symmetry Protected Topological States"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292619589026176","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Odd-Parity Topological Superconductors: Theory and Application to<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:msub><mml:mi>Cu</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mi>Bi</mml:mi><mml:mn>2</mml:mn></mml:msub><mml:msub><mml:mi>Se</mml:mi><mml:mn>3</mml:mn></mml:msub></mml:math>"}]},{"@id":"https://cir.nii.ac.jp/crid/1360292620238345856","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Classification of topological insulators and superconductors in three spatial dimensions"}]},{"@id":"https://cir.nii.ac.jp/crid/1360294643701759616","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Non-Hermitian band topology with generalized inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360294647472413696","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Symmetry indicator in non-Hermitian systems"}]},{"@id":"https://cir.nii.ac.jp/crid/1360565166776159104","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Symmetry-based indicators of band topology in the 230 space groups"}]},{"@id":"https://cir.nii.ac.jp/crid/1360565167769067264","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>Z</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>topology in nonsymmorphic crystalline insulators: Möbius twist in surface states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360566399835736320","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Magnetic Response of Majorana Kramers Pairs Protected by \\(\\mathbb{Z}_{2}\\) Invariants"}]},{"@id":"https://cir.nii.ac.jp/crid/1360567185013295104","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Symmetry Indicators and Anomalous Surface States of Topological Crystalline Insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1360568469972060160","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Symmetry indicators for topological superconductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1360574094030997888","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Refined symmetry indicators for topological superconductors in all space groups"}]},{"@id":"https://cir.nii.ac.jp/crid/1360576118678478592","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Discriminant indicators with generalized inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360581935562024704","@type":"Article","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Hybrid Higher-Order Skin Topological Modes in the Two-Dimensional Su–Schrieffer–Heeger Model with Nonreciprocal Hoppings"}]},{"@id":"https://cir.nii.ac.jp/crid/1360588380160718976","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Classification of time-reversal symmetric topological superconducting phases for conventional pairing symmetries"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659922993024","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Connecting higher-order topological insulators to lower-dimensional topological insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1360848659923419904","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Topological classification under nonmagnetic and magnetic point group symmetry: Application of real-space Atiyah-Hirzebruch spectral sequence to higher-order topology"}]},{"@id":"https://cir.nii.ac.jp/crid/1360855571060530816","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological quantum chemistry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861288362648704","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Rotoinversion-symmetric bulk-hinge correspondence and its applications to higher-order Weyl semimetals"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861707123985408","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:msub><mml:mi>Z</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math>\n Dirac points with topologically protected multihelicoid surface states"}]},{"@id":"https://cir.nii.ac.jp/crid/1360861707393005056","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Discriminant indicator with generalized rotational symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1360865816812000256","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Effects of first- and second-order topological phases on equilibrium crystal shapes"}]},{"@id":"https://cir.nii.ac.jp/crid/1361131419925632384","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Bulk-edge and bulk-hinge correspondence in inversion-symmetric insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137043881877120","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological Insulators in Magnetic Fields: Quantum Hall Effect and Edge Channels with a Nonquantized<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\" display=\"inline\"><mml:mi>θ</mml:mi></mml:math>Term"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137046210614656","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Compactly supported Wannier functions and algebraic<mml:math xmlns:mml=\"http://www.w3.org/1998/Math/MathML\"><mml:mi>K</mml:mi></mml:math>-theory"}]},{"@id":"https://cir.nii.ac.jp/crid/1361137046434969344","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological Crystalline Insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1361412894817147520","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Glide-symmetric magnetic topological crystalline insulators with inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418518758675328","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Quantitative mappings between symmetry and topology in solids"}]},{"@id":"https://cir.nii.ac.jp/crid/1361418521474006272","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Higher-order topological insulators and superconductors protected by inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1361699995753587584","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Reflection-Symmetric Second-Order Topological Insulators and Superconductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1362262944631307008","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological insulators and superconductors: tenfold way and dimensional hierarchy"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544418447622400","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Filling-enforced quantum band insulators in spin-orbit coupled crystals"}]},{"@id":"https://cir.nii.ac.jp/crid/1362544418835474816","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Higher-order topological insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1362825896305175936","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological odd-parity superconductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107368532019968","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"<i>Colloquium</i>: Topological insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369195749248","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Second-order topological insulators and superconductors with an order-two crystalline symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107369740393728","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Twisted Equivariant Matter"}]},{"@id":"https://cir.nii.ac.jp/crid/1363107370622629376","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Antiferromagnetic topological insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388844983571840","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological Classification of Crystalline Insulators through Band Structure Combinatorics"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388845242560000","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Inversion-symmetric topological insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1363388845672934528","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological insulators and superconductors"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319149177088","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Weyl and Dirac semimetals in three-dimensional solids"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670319213439616","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Bulk topological invariants in noninteracting point group symmetric insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/1363670320138823040","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Topological insulators with inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1363951794754824192","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Quantized response and topology of magnetic insulators with inversion symmetry"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233268604994176","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"Nonstandard symmetry classes in mesoscopic normal-superconducting hybrid structures"}]},{"@id":"https://cir.nii.ac.jp/crid/1364233270145850752","@type":"Article","relationType":["references"],"jpcoar:relatedTitle":[{"@value":"The space group classification of topological band-insulators"}]},{"@id":"https://cir.nii.ac.jp/crid/2050307417130022400","@type":"Article","resourceType":"学術雑誌論文(journal article)","relationType":["isReferencedBy"],"jpcoar:relatedTitle":[{"@value":"Topological gapless points in superconductors : from the viewpoint of symmetry"}]}],"dataSourceIdentifier":[{"@type":"CROSSREF","@value":"10.1103/physrevb.98.115150"},{"@type":"KAKEN","@value":"PRODUCT-22158210"},{"@type":"OPENAIRE","@value":"doi_dedup___::5203c9dea26e95d825c99d6efc10e746"},{"@type":"CROSSREF","@value":"10.1103/physrevb.101.115120_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.7566/jpsj.89.043703_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1093/ptep/ptab124_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.2.043274_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.102.241202_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.103.205205_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1126/sciadv.aaz8367_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.1.013012_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.105.085109_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.104.035424_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.3.023086_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.7566/jpsj.93.064702_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.109.214502_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.98.205129_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.99.085127_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevx.9.041015_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.105.115119_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.4.033170_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevx.12.011021_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.105.214103_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.107.245148_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevresearch.2.013300_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"},{"@type":"CROSSREF","@value":"10.1103/physrevb.100.165202_references_DOI_PaJBEH1IzsI3kkiqxJ4t7QdgbR5"}]}