about
Type-II Weyl semimetalsExperimental evidence of hourglass fermion in the candidate nonsymmorphic topological insulator KHgSb.Strong anisotropy of Dirac cones in SrMnBi2 and CaMnBi2 revealed by angle-resolved photoemission spectroscopy.Evidence of topological surface state in three-dimensional Dirac semimetal Cd3As2.Discovery of a three-dimensional topological Dirac semimetal, Na3Bi.A stable three-dimensional topological Dirac semimetal Cd3As2.Landau level splitting in Cd3As2 under high magnetic fields.Quasiparticle interference of the Fermi arcs and surface-bulk connectivity of a Weyl semimetal.Two-dimensional chiral topological superconductivity in Shiba latticesGraph theory data for topological quantum chemistry.The chiral anomaly and thermopower of Weyl fermions in the half-Heusler GdPtBi.Distinguishing a Majorana zero mode using spin-resolved measurements.Time-Reversal-Breaking Weyl Fermions in Magnetic Heusler Alloys.Observation of topological superconductivity on the surface of an iron-based superconductor.Beyond Dirac and Weyl fermions: Unconventional quasiparticles in conventional crystals.Composite Icosahedron/Cube Endohedral Clusters in Rh2Cd15.MoTe_{2}: A Type-II Weyl Topological Metal.Higher-order topological insulators.Dirac semimetal and topological phase transitions inA3Bi (A=Na, K, Rb)Three-dimensional Dirac semimetal and quantum transport in Cd3As2Topological Dirac semimetal phase in Pd and Pt oxidesHigher-Order Topology in BismuthTopological quantum chemistryHourglass fermionsHigh-resolution studies of the Majorana atomic chain platformImaging electronic states on topological semimetals using scanning tunneling microscopyUniversal signatures of Fermi arcs in quasiparticle interference on the surface of Weyl semimetalsA gap-protected zero-Hall effect state in the quantum limit of the non-symmorphic metal KHgSbBand connectivity for topological quantum chemistry: Band structures as a graph theory problemBuilding blocks of topological quantum chemistry: Elementary band representationsDouble crystallographic groups and their representations on the Bilbao Crystallographic ServerMultiple topological states in iron-based superconductorsTopological phases in the TaSe3 compoundTopology of Disconnected Elementary Band RepresentationsWallpaper fermions and the nonsymmorphic Dirac insulatorChiral anomaly factory: Creating Weyl fermions with a magnetic fieldCrystal growth and stoichiometry-dependent properties of the ferromagnetic Weyl semimetal ZrCo2−xSnElectronic structure, Dirac points and Fermi arc surface states in three-dimensional Dirac semimetal Na3Bi from angle-resolved photoemission spectroscopyTopological Insulators from Group CohomologyInteraction-induced quantum anomalous Hall phase in (111) bilayer ofLaCoO3
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Q28270263-CEE8D32F-3C54-4270-B8CC-E85C510EE1B9Q33643524-B57F2F3D-2451-4F3F-AC39-29C0D9302FF1Q33781253-B8E45C8A-1014-44F5-9632-2E228D358DC9Q34068138-17FEBA23-F6AA-424A-9DAC-6896037F4F37Q34398510-71D65D92-9A0F-496B-970A-782BB773C5A1Q34421287-1448AC3D-9744-4CD5-BFA1-C39BC828712BQ35878364-5D7C7410-7812-4633-B1A3-CCDCE3D15776Q35953357-4A25B070-0DCB-4151-ADFF-1D8790115787Q37153624-6063F25F-2E05-4EF1-9155-656286102D4EQ47671277-0415845E-9D40-4908-8D9B-0807C6CF1A80Q48053743-DC1F87C2-9582-4659-8640-101AD99DCCBEQ48196242-D2E7B7FD-EB74-415D-AA9C-FC8642CC7789Q51007453-FB97FD98-F48E-4D2E-A75B-1EEFA815D3BBQ51556918-A656BD69-66A6-4D69-80CB-1E006C3C649BQ53057429-B70C45E1-7D1A-4339-BB36-C03966434445Q53746523-A817A367-F846-47F3-A3E7-96F12559AE17Q53936269-D55468F9-418D-46D6-B8C8-B76CBC9B1529Q55280643-E110DB09-4A5E-47F0-B4C7-6881B20AA888Q56622372-12EF4433-8A73-4E46-A402-75D391F2BC3BQ56622377-5EF8F0F0-9A8B-475F-B154-C3B0E1F0B7BCQ57662078-F8A3DD54-E37B-4265-8A0E-70B2741216B2Q57822933-CD8DE98B-B038-443C-A2F3-16545E890CAFQ59066613-0787D07C-C45F-42B9-B37B-BDBD91A59CA9Q59067156-86A32592-1F37-44F6-988E-8F097942DBB7Q59457854-85875FA6-6100-422F-8E19-092A450BE202Q59457858-7DDCBE76-2A61-40DA-8D24-E7FF69155D2CQ59457860-A65CF273-2D19-456A-BD85-C83F1C31291BQ62581716-EC80F2C8-2224-4F98-9BB5-0F35B0F34CCCQ62641789-EF4CE1B3-521F-4CE4-950E-26AF77554A6FQ62641790-D18926B3-EEDC-4F8C-98AB-066D303A1812Q62641838-C0051F7B-92DF-428A-91E7-7E2A4FDCC65BQ62645332-54CE21BC-8BED-4E12-B5BD-73719F2AE752Q62645336-B9F3BEEF-0D9B-4D85-9724-3E4B974205B9Q62645338-7F98D0BC-A9F7-4AFC-950B-D2734047F68FQ62645342-25E4A3EB-71EF-4552-BA9D-2988AE09BFC0Q62645343-32064735-3AF9-47C0-8E56-4560604CC67EQ62645345-EDCF3172-840D-41B6-A5B8-D6C5A353E113Q62645349-AB4EAB86-8D7E-4D17-B44B-229FDA070843Q62645351-8AF0DF7E-77E4-4F1C-AD37-C65972513B42Q62645353-3702FA63-EED6-40E8-896A-EC6595537CB7
P50
description
onderzoeker
@nl
researcher
@en
հետազոտող
@hy
name
Zhijun Wang
@ast
Zhijun Wang
@en
Zhijun Wang
@es
Zhijun Wang
@nl
type
label
Zhijun Wang
@ast
Zhijun Wang
@en
Zhijun Wang
@es
Zhijun Wang
@nl
prefLabel
Zhijun Wang
@ast
Zhijun Wang
@en
Zhijun Wang
@es
Zhijun Wang
@nl
P106
P31
P496
0000-0003-2169-8068