2001
DOI: 10.1103/physrevb.63.184430
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Mechanism of resonant x-ray magnetic scattering in NiO

Abstract: We study the resonant x-ray magnetic scattering (RXMS) around the K edge of Ni in the antiferromagnet NiO, by treating the 4p states of Ni as a band and the 3d states as localized states. We propose a mechanism that the 4p states are coupled to the magnetic order through the intra-atomic Coulomb interaction between the 4p and the 3d states and through the p-d mixing to the 3d states of neighboring Ni atoms. These couplings induce the orbital moment in the 4p band, and thereby give rise to the RXMS intensity at… Show more

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Cited by 17 publications
(10 citation statements)
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“…Finally we point out that this type of ab initio calculation can be applied to analyzing the magnetic RXS spectra at the K edge in transition-metal compounds, 31,32 and may clarify the p orbital polarization in antiferromagnetic phases. According to our recent calculation of the magnetic RXS spectra in NiO, 33 the main peak intensity almost disappears when the SOI on the 4p band is turned off.…”
Section: Discussionmentioning
confidence: 99%
“…Finally we point out that this type of ab initio calculation can be applied to analyzing the magnetic RXS spectra at the K edge in transition-metal compounds, 31,32 and may clarify the p orbital polarization in antiferromagnetic phases. According to our recent calculation of the magnetic RXS spectra in NiO, 33 the main peak intensity almost disappears when the SOI on the 4p band is turned off.…”
Section: Discussionmentioning
confidence: 99%
“…The sensitivity of the experiment to magnetic order at the quadrupole, 1s-3d, threshold energy has its origin in the spin polarization of the 3d states, whilst at the 1s-4 p dipole transition energy the resonant enhancement for magnetic reflections is due to the 4p-3d intra-atomic Coulomb interaction and to the mixing of the 4p with the 3d states of neighboring Cu atoms. 18 The two resonant terms are superimposed to a much weaker, nonresonant contribution. 19,20 Both the resonant and the nonresonant magnetic scattering amplitudes depend on the polarization of the incident (, ) and of the scattered (Ј, Ј) photons, and are discussed in Refs.…”
Section: Experimental Methods and Detailsmentioning
confidence: 99%
“…21 The density matrix mm Ј ( j) becomes symmetric by neglecting the spin-orbit interaction. 27,28 Using ␣, ␤, ␥, , , and , functions of , the matrix at the V1 site can be represented as (1) …”
Section: Rxs Spectramentioning
confidence: 99%