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Journal Articles

Resonant inelastic X-ray scattering study of electronic excitations in insulating K$$_{0.83}$$Fe$$_{1.53}$$Se$$_2$$

Gretarsson, H.*; Nomura, Takuji; Jarrige, I.*; Lupascu, A.*; Upton, M. H.*; Kim, J.*; Casa, D.*; Gog, T.*; Yuan, R. H.*; Chen, Z. G.*; et al.

Physical Review B, 91(24), p.245118_1 - 245118_8, 2015/06

https://doi.org/10.1103/PhysRevB.91.245118
 Times Cited Count：6 Percentile：27.97(Materials Science, Multidisciplinary)

Journal Articles

Kondo interactions from band reconstruction in YbInCu$$_4$$

Jarrige, I.*; Kotani, Akio*; Yamaoka, Hitoshi*; Tsujii, Naohito*; Ishii, Kenji; Upton, M.*; Casa, D.*; Kim, J. H.*; Gog, T.*; Hancock, J. N.*

Physical Review Letters, 114(12), p.126401_1 - 126401_5, 2015/03

https://doi.org/10.1103/PhysRevLett.114.126401
 Times Cited Count：11 Percentile：60.87(Physics, Multidisciplinary)

Journal Articles

Resonant inelastic X-ray scattering study of intraband charge excitations in hole-doped high-$$T_c$$ cuprates

Wakimoto, Shuichi; Ishii, Kenji; Kimura, Hiroyuki*; Ikeuchi, Kazuhiko*; Yoshida, Masahiro*; Adachi, Tadashi*; Casa, D.*; Fujita, Masaki*; Fukunaga, Yasushi*; Gog, T.*; et al.

Physical Review B, 87(10), p.104511_1 - 104511_7, 2013/03

https://doi.org/10.1103/PhysRevB.87.104511
 Times Cited Count：10 Percentile：43.41(Materials Science, Multidisciplinary)

Journal Articles

Resonant inelastic X-ray scattering study of charge excitations in superconducting and nonsuperconducting PrFeAsO$$_{1-y}$$

Jarrige, I.*; Nomura, Takuji; Ishii, Kenji; Gretarsson, H.*; Kim, Y.-J.*; Kim, J.*; Upton, M.*; Casa, D.*; Gog, T.*; Ishikado, Motoyuki*; et al.

Physical Review B, 86(11), p.115104_1 - 115104_4, 2012/09

https://doi.org/10.1103/PhysRevB.86.115104
 Times Cited Count：8 Percentile：35.38(Materials Science, Multidisciplinary)

We report the first observation by momentum-resolved resonant inelastic X-ray scattering of charge excitations in an iron-based superconductor and its parent compound, PrFeAsO$$_{0.7}$$ and PrFeAsO respectively, with two main results. First, using calculations based on a 16 band $$dp$$ model, we show that the energy of the lowest-lying excitations, identified as $$dd$$ interband transitions of dominant $$xz$$, $$yz$$ orbital character, exhibits a dramatic dependence on electron correlation. This enables us to estimate the Coulomb repulsion $$U$$ and Hund's coupling $$J$$, and to highlight the role played by $$J$$ in these peculiar orbital-dependent electron correlation effects. Second, we show that short-range antiferromagnetic correlations, which are a prerequisite to the occurrence of these excitations at the $$Gamma$$ point, are still present in the superconducting state.

Journal Articles

Magnetic nature of the 500 meV peak in La$$_{2-x}$$Sr$$_x$$CuO$$_4$$ observed with resonant inelastic X-ray scattering at the Cu $$K$$-edge

Ellis, D. S.*; Kim, J.*; Hill, J. P.*; Wakimoto, Shuichi; Birgeneau, R. J.*; Shvyd'ko, Y.*; Casa, D.*; Gog, T.*; Ishii, Kenji; Ikeuchi, Kazuhiko*; et al.

Physical Review B, 81(8), p.085124_1 - 085124_12, 2010/02

https://doi.org/10.1103/PhysRevB.81.085124
 Times Cited Count：40 Percentile：80.38(Materials Science, Multidisciplinary)

Journal Articles

Incident energy and polarization-dependent resonant inelastic X-ray scattering study of La$$_2$$CuO$$_4$$

Lu, L.*; Hancock, J. N.*; Chabot-Couture, G.*; Ishii, Kenji; Vajk, O. P.*; Yu, G.*; Mizuki, Junichiro; Casa, D.*; Gog, T.*; Greven, M.*

Physical Review B, 74(22), p.224509_1 - 224509_9, 2006/12

https://doi.org/10.1103/PhysRevB.74.224509
 Times Cited Count：34 Percentile：77.83(Materials Science, Multidisciplinary)

We present a detailed Cu $$K$$-edge resonant inelastic X-ray scattering (RIXS) study of the Mott insulator La$$_2$$CuO$$_4$$ in the 1-7 eV energy loss range. As initially found for the high-temperature superconductor HgBa$$_2$$CuO$$_{4+delta}$$, the spectra exhibit a multiplet of weakly dispersive electron-hole excitations, which are revealed by utilizing the subtle dependence of the cross section on the incident photon energy. The close similarity between the fine structures for in-plane and out-of-plane polarizations is indicative of the central role played by the 1s core hole in inducing charge excitations within the CuO$$_2$$ planes. On the other hand, we observe a polarization dependence of the spectral weight, and careful analysis reveals two separate features near 2 eV that may be related to different charge-transfer processes. The polarization dependence indicates that the $$4p$$ electrons contribute significantly to the RIXS cross section.

Journal Articles

Resonant inelastic X-ray scattering study of overdoped La$$_{2-x}$$Sr$$_{x}$$CuO$$_{4}$$

Wakimoto, Shuichi; Kim, Y.-J.*; Kim, H.*; Zhang, H.*; Gog, T.*; Birgeneau, R. J.*

Physical Review B, 72(22), p.224508_1 - 224508_7, 2005/12

https://doi.org/10.1103/PhysRevB.72.224508
 Times Cited Count：13 Percentile：49.98(Materials Science, Multidisciplinary)

Resonant inelastic X-ray scattering (RIXS) at the copper Kabsorption edge has been performed for heavily overdoped samplesof La$$_{2-x}$$Sr$$_{x}$$CuO$$_{4}$$ with $$x= 0.25$$ and $$0.30$$. We have observed the chargetransfer and molecular orbital excitations which exhibit resonances at incident energies of $$E_i= 8.992$$ and $$8.998$$ keV,respectively. From a comparison with previous results on undoped andoptimally-doped samples, we determine that the charge transfer excitation energy increases monotonically as doping increases. In addition, the $$E_i$$-dependences of the RIXS spectral weight and absorption spectrum exhibit no clear peak at $$E_i = 8.998$$ keV in contrast to results in the underdoped samples. The low-energy ($$leq 3$$ eV) continuum excitation intensity has been studied utilizing the high energy resolution of 0.13 eV (FWHM). A comparison of the RIXS profiles at $$(pi 0)$$ and $$(pi pi)$$ indicates that the continuum intensity exists even at $$(pi pi)$$ in the overdoped samples, while it has been reported only at $$(0 0)$$ and $$(pi 0)$$ for the $$x=0.17$$ sample. Furthermore, we also found an additional excitation on top of the continuum intensity at the $$(pi pi)$$ and $$(pi 0)$$ positions.

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