Abhishek Nag

Dr. Abhishek Nag

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Research Focus & Metrics

Academic Career Length

7Years (2020-Present)

(Calculated once Scilit publication data is synced: current year − year of first publication + 1)

Representative Publications

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21 September 2020 in Nature Energy
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RHRobert A. House
Robert A. House
GRGregory J. Rees
Gregory J. Rees
MPMiguel A. Pérez-Osorio
Miguel A. Pérez-Osorio
JMJohn-Joseph Marie
John-Joseph Marie
EBEDOUARD BOIVIN
EDOUARD BOIVIN
Peter G. BrucePeter G. Bruce
Peter G. Bruce

9 July 2021 in Science
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HLH. Lu
H. Lu
MRM. Rossi
M. Rossi
ANAbhishek Nag
Abhishek Nag
MOM. Osada
M. Osada
DLD. F. Li
D. F. Li
WLW. S. Lee
W. S. Lee
Looking for magnetic clues: Thin films of the neodymium nickelate NdNiO 2 doped with strontium have recently been found to be superconducting. This materials class bears structural and electronic similarities to the famed cuprate superconductors, but how far the analogy goes remains unclear. Lu et al. used resonant inelastic x-ray scattering to look for magnetism, which exists in the cuprates, in Nd 1-x Sr x NiO 2 films (see the Perspective by Benckiser). The authors observed magnetic modes in the undoped compound that had a doping evolution consistent with the behavior of a doped Mott insulator. Science , abd7726, this issue p. 213 ; see also abi6855, p. 157

18 August 2022 in Nature Materials
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CTCharles C. Tam
Charles C. Tam
JCJaewon Choi
Jaewon Choi
XDXiang Ding
Xiang Ding
SAStefano Agrestini
Stefano Agrestini
ANAbhishek Nag
Abhishek Nag
KZKe-Jin Zhou
Ke-Jin Zhou

25 July 2022 in Nature Physics
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MRMatteo Rossi
Matteo Rossi
MOMotoki Osada
Motoki Osada
JCJaewon Choi
Jaewon Choi
SAStefano Agrestini
Stefano Agrestini
DJDaniel Jost
Daniel Jost
WLWei-Sheng Lee
Wei-Sheng Lee

22 February 2022 in Journal of Synchrotron Radiation
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KZKe-Jin Zhou
Ke-Jin Zhou
AWAndrew Walters
Andrew Walters
MGMirian Garcia-Fernandez
Mirian Garcia-Fernandez
TRThomas Rice
Thomas Rice
MHMatthew Hand
Matthew Hand
GHGeorge Howell
George Howell
The I21 beamline at Diamond Light Source is dedicated to advanced resonant inelastic X-ray scattering (RIXS) for probing charge, orbital, spin and lattice excitations in materials across condensed matter physics, applied sciences and chemistry. Both the beamline and the RIXS spectrometer employ divergent variable-line-spacing gratings covering a broad energy range of 280–3000 eV. A combined energy resolution of ∼35 meV (16 meV) is readily achieved at 930 eV (530 eV) owing to the optimized optics and the mechanics. Considerable efforts have been paid to the design of the entire beamline, particularly the implementation of the collection mirrors, to maximize the X-ray photon throughput. The continuous rotation of the spectrometer over 150° under ultra high vacuum and a cryogenic manipulator with six degrees of freedom allow accurate mappings of low-energy excitations from solid state materials in momentum space. Most importantly, the facility features a unique combination of the high energy resolution and the high photon throughput vital for advanced RIXS applications. Together with its stability and user friendliness, I21 has become one of the most sought after RIXS beamlines in the world.

8 December 2021 in Physical Review B
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MRM. Rossi
M. Rossi
HLH. Lu
H. Lu
ANAbhishek Nag
Abhishek Nag
DLD. Li
D. Li
MOM. Osada
M. Osada
WLW. S. Lee
W. S. Lee
The recent discovery of superconductivity in Nd1−xSrxNiO2 has drawn significant attention in the field. A key open question regards the evolution of the electronic structure with respect to hole doping. Here we exploit x-ray absorption spectroscopy (XAS) and resonant inelastic x-ray scattering (RIXS) to probe the doping-dependent electronic structure of Nd1−xSrxNiO2. Upon doping, a high-energy feature in Ni L3-edge XAS develops in addition to the main absorption peak, while XAS at the O K-, Nd M3- and Nd M5-edge exhibits a much weaker response. This implies that doped holes are mainly introduced into Ni 3d states. By comparing our data to atomic multiplet calculations including D4h crystal field, the doping-induced feature in Ni L3-edge XAS is consistent with a d8 spin-singlet state in which doped holes reside in the 3dx2−y2 orbitals. This is further supported by the softening of RIXS orbital excitations due to doping, corroborating with the Fermi level shift associated with increasing holes in the Ni 3dx2−y2 orbital.