activity
20092021
most citedSpin fluctuation induced Weyl semimetal state in the paramagnetic phase of EuCdAs

193 citations · 789 across the 18 of their papers we have counts for

collaborators

18 papers

cond-mat.str-el2021★ 8 cited

Revealing a charge-density-wave gap in the predicted weak topological insulator HoSbTe

J. L. Liu, R. Liu, M. Yang +7

HoSbTe was predicted to be a weak topological insulator, whose spin-orbit coupling (SOC) gaps are reported to be as large as hundreds of meV. Utilizing infrared spectroscopy, we fi…

cond-mat.mtrl-sci2021★ 18 cited

Inherited Weak Topological Insulator Signatures in Topological Hourglass Semimetal Nb3XTe6 (X = Si, Ge)

Q. Wan, T. Y. Yang, S. Li +17

Using spin-resolved and angle-resolved photoemission spectroscopy and first-principles calculations, we have identified bulk band inversion and spin polarized surface state evolved…

cond-mat.str-el2019★ 193 cited

Spin fluctuation induced Weyl semimetal state in the paramagnetic phase of EuCdAs

J. -Z. Ma, S. M. Nie, C. J. Yi +22

Weyl fermions as emergent quasiparticles can arise in Weyl semimetals (WSMs) in which the energy bands are nondegenerate, resulting from inversion or time-reversal symmetry breakin…

cond-mat.str-el2019★ 51 cited

Observation of multiple types of topological fermions in PdBiSe

B. Q. Lv, Z. -L. Feng, J. -Z. Zhao +12

Topological semimetals with different types of band crossings provide a rich platform to realize novel fermionic excitations, known as topological fermions. In particular, some fer…

cond-mat.str-el2019★ 17 cited

Magnetic competition induced colossal magnetoresistance in n-type HgCr2Se4 under high pressures

J. P. Sun, Y. Y. Jiao, C. J. Yi +7

The n-type HgCr2Se4 exhibits a sharp semiconductor-to-metal transition (SMT) in resistivity accompanying the ferromagnetic order at TC = 106 K. Here, we investigate the effects of…

cond-mat.str-el2018★ 10 cited

Evidence for ground state and defect-induced spin glass behaviour in the pyrochlore osmate YOsO

N. R. Davies, C. V. Topping, H. Jacobsen +14

We present AC and DC magnetometry, heat capacity, muon spin relaxation (SR) and resonant inelastic X-ray scattering (RIXS) studies of the pyrochlore osmate YOsO. We…

cond-mat.supr-con2017★ 6 cited

Magneto-elastic coupling in Fe-based superconductors

S. -F. Wu, W. -L. Zhang, V. K. Thorsmølle +12

We used polarization-resolved Raman scattering to study the magneto-elastic coupling in the parent compounds of several families of Fe-based superconductors (BaFe2As2, EuFe2As2, Na…

cond-mat.str-el2017★ 18 cited

Crossover from itinerant to localized magnetic excitations through the metal-insulator transition in NaOsO

J. G. Vale, S. Calder, C. Donnerer +8

NaOsO undergoes a metal-insulator transition (MIT) at 410 K, concomitant with the onset of antiferromagnetic order. The excitation spectra have been investigated throu…

cond-mat.mtrl-sci2017★ 4 cited

Robustness of topological states to lattice instability in non-symmorphic topological insulator KHgSb

D. Chen, T. T. Zhang, C. J. Yi +8

We report a polarized Raman scattering study of non-symmorphic topological insulator KHgSb with hourglass-like electronic dispersion. Supported by theoretical calculations, we show…

cond-mat.supr-con2016★ 8 cited

Disentangling the surface and bulk electronic structures of LaOFeAs

P. Zhang, J. Ma, T. Qian +7

We performed a comprehensive angle-resolved photoemission spectroscopy study of the electronic band structure of LaOFeAs single crystals. We found that samples cleaved at low tempe…

cond-mat.supr-con2016★ 10 cited

Commensurate lattice distortion in the layered titanium oxypnictides NaTiO ( As, Sb) determined by X-ray diffraction

N. R. Davies, R. D. Johnson, A. J. Princep +12

We report single crystal X-ray diffraction measurements on NaTiO ( = As, Sb) which reveal a charge superstructure that appears below the density wave transition…

cond-mat.supr-con2016★ 9 cited

New phase transition in NaTiAsO revealed by Raman scattering

D. Chen, T. T. Zhang, Z. -D. Song +8

We performed a Raman scattering study of NaTiAsO. We identified a symmetry breaking structural transition at around K, which matches a large bump in the ele…

cond-mat.supr-con2015★ 23 cited

Penetration depth measurements of K2Cr3As3 and Rb2Cr3As3

G. M. Pang, M. Smidman, W. B. Jiang +10

The newly discovered superconductors A2Cr3As3 (A = K, Rb, Cs), with a quasi-one-dimensional crystal structure have attracted considerable interest. The crystal structure consists o…

cond-mat.str-el2015★ 57 cited

Giant spin-phonon-electronic coupling in a 5d oxide

S. Calder, J. H. Lee, M. B. Stone +8

Enhanced coupling of material properties offers new fundamental insights and routes to multifunctional devices. In this context 5d oxides provide new paradigms of cooperative inter…

cond-mat.str-el2012★ 21 cited

Magnetic structure determination of CaLiOsO using neutron and x-ray scattering

S. Calder, M. D. Lumsden, V. O. Garlea +5

We present a neutron and x-ray scattering investigation of CaLiOsO, a material predicted to host magnetic ordering solely through an extended superexchange pathway involvin…

cond-mat.str-el2012★ 140 cited

Magnetically driven metal-insulator transition in NaOsO3

S. Calder, V. O. Garlea, D. F. McMorrow +10

The metal-insulator transition (MIT) is one of the most dramatic manifestations of electron correlations in materials. Various mechanisms producing MITs have been extensively consi…

cond-mat.supr-con2010★ 64 cited

Large decrease in the critical temperature of superconducting LaFeAsO0.85 compounds doped with 3% atomic weight of nonmagnetic Zn impurities

Y. F. Guo, Y. G. Shi, S. Yu +10

We observed a large decrease of Tc by no more than 3 at.% of Zn doped to the optimized superconductor LaFeAsO0.85 (Tc = 26 K), confirmed by measurements of electrical resistivity,…

cond-mat.str-el2009★ 132 cited

Continuous metal-insulator transition of the antiferromagnetic perovskite NaOsO3

Y. G. Shi, Y. F. Guo, S. Yu +11

Newly synthesized perovskite NaOsO3 shows Curie-Weiss metallic nature at high temperature and suddenly goes into an antiferromagnetically insulating state at 410 K on cooling. Elec…