pith. sign in

Goro Shibata

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Papers (11)

  1. Possibility of ferro-octupolar order in Ba$_2$CaOsO$_6$ assessed by X-ray magnetic dichroism measurements cond-mat.str-el · 2025 · author #1
  2. Electronic structure of the novel high-$T_{\rm C}$ ferromagnetic semiconductor (Ga,Fe)Sb: x-ray magnetic circular dichroism and resonance photoemission spectroscopy studies cond-mat.str-el · 2018 · author #8
  3. Anisotropic Charge Distribution Induced by Spin Polarization in La$_{0.6}$Sr$_{0.4}$MnO$_{3}$ Thin Films Studied by X-ray Magnetic Linear Dichroism cond-mat.mtrl-sci · 2018 · author #1
  4. Local Magnetic States of the Weakly Ferromagnetic Iron-Based Superconductor Sr$_2$VFeAsO$_{3-\delta}$ Studied by X-ray Magnetic Circular Dichroism cond-mat.str-el · 2018 · author #8
  5. Systematic study of the electronic structure and the magnetic properties of a few-nm-thick epitaxial (Ni1-xCox)Fe2O4 (x = 0 - 1) layers grown on Al2O3(111)/Si(111) using soft X-ray magnetic circular dichroism: effects of cation distribution cond-mat.mtrl-sci · 2018 · author #7
  6. Electronic States and Possible Origin of the Orbital-Glass State in a Nearly Metallic Spinel Cobalt Vanadate: An X-ray Magnetic Circular Dichroism Study cond-mat.str-el · 2018 · author #2
  7. Effect(s) of Cobalt Substitution in $L1_{0}$-(Fe,Co)Pt Thin Films cond-mat.mtrl-sci · 2017 · author #6
  8. Electronic structure and magnetic properties of magnetically dead layers in epitaxial CoFe2O4/Al2O3/Si(111) films studied by X-ray magnetic circular dichroism cond-mat.mtrl-sci · 2017 · author #7
  9. Origin of the large positive magnetoresistance in Ge1-xMnx granular thin films cond-mat.mtrl-sci · 2016 · author #5
  10. Magnetization Process of the n-type Ferromagnetic Semiconductor (In,Fe)As:Be Studied by X-ray Magnetic Circular Dichroism cond-mat.mtrl-sci · 2015 · author #4
  11. Thickness-dependent ferromagnetic metal to paramagnetic insulator transition in La$_{0.6}$Sr$_{0.4}$MnO$_3$ thin films studied by x-ray magnetic circular dichroism cond-mat.str-el · 2013 · author #1

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