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Chi-Cheng Lee

Researcher at University of Tokyo

Publications -  91
Citations -  14034

Chi-Cheng Lee is an academic researcher from University of Tokyo. The author has contributed to research in topics: Weyl semimetal & Fermion. The author has an hindex of 33, co-authored 84 publications receiving 12251 citations. Previous affiliations of Chi-Cheng Lee include Academia Sinica & Brookhaven National Laboratory.

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Nonresonant Inelastic X-Ray Scattering and Energy-Resolved Wannier Function Investigation of d-d Excitations in NiO and CoO

TL;DR: Nonresonant inelastic x-ray scattering measurements on NiO and CoO show that strong dipole-forbidden d-d excitations appear within the Mott gap at large wave vectors, and the sensitivity to weak symmetry breaking in particle-hole wave functions suggests a wide application to strongly correlated systems.
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Unfolding method for first-principles LCAO electronic structure calculations

TL;DR: The unfolding method is generalized to the linear combination of atomic orbitals (LCAO) method, and a general formula to calculate the unfolded spectral weight is presented, showing the usefulness of the unfolding method.
Posted Content

Observation of the Adler-Bell-Jackiw chiral anomaly in a Weyl semimetal

TL;DR: In this article, the experimental discovery of Adler-Bell-Jackiw chiral anomaly in a Weyl semimetal crystal was reported, which was later confirmed by the same authors.
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Signatures of Fermi Arcs in the Quasiparticle Interferences of the Weyl Semimetals TaAs and NbP.

TL;DR: The results, for the first time, propose a universal interference signature of the topological Fermi arcs in TaAs, which is fundamental for scanning tunneling microscope (STM) measurements on this prototypical Weyl semimetal compound.
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Coupling of spin and orbital excitations in the iron-based superconductor FeSe 0.5 Te 0.5

TL;DR: In this paper, a combined analysis of neutron scattering and photoemission measurements on superconducting FeSe{sub 0.5}Te{sub0.5}. was presented, showing that low-energy magnetic excitations dispersed only in the direction transverse to the characteristic wave vector (1/2,0,0) whereas the electronic Fermi surface near (1 2,0,0) appears to consist of four incommensurate pockets.