検索対象:     
報告書番号:
※ 半角英数字
 年 ~ 
 年
検索結果: 167 件中 1件目~20件目を表示

発表形式

Initialising ...

選択項目を絞り込む

掲載資料名

Initialising ...

発表会議名

Initialising ...

筆頭著者名

Initialising ...

キーワード

Initialising ...

発表言語

Initialising ...

発行年

Initialising ...

開催年

Initialising ...

選択した検索結果をダウンロード

論文

Spin-orbit-entangled state of Ba$$_2$$CaOsO$$_6$$ studied by O $$K$$-edge resonant inelastic X-ray scattering and Raman spectroscopy

岡本 淳*; 芝田 悟朗; 藤森 淳; 他9名*

npj Quantum Materials (Internet), 10, p.44_1 - 44_8, 2025/04

 被引用回数:0 パーセンタイル:0.00(Materials Science, Multidisciplinary)

Transition-metal ions with 5$$d^2$$ electronic configuration in a cubic crystal field are prone to have a vanishing dipolar magnetic moment but finite higher-order multipolar moments, and they are expected to exhibit exotic physical properties. Through an investigation using resonant inelastic X-ray spectroscopy (RIXS), Raman spectroscopy, and theoretical ligand-field multiplet and ab initio calculations, we fully characterized the electronic structure of Ba$$_2$$CaOsO$$_6$$, particularly, the crystal field symmetry of the 5$$d^2$$ electrons in this anomalous material. The low-energy multiplet excitations from RIXS at the oxygen $$K$$ edge and Raman-active phonons both show no splitting, confirming the absence of Jahn-Teller distortion. These findings are consistent with the ground state with the "hidden order" of magnetic octupoles.

論文

Relationship between orbital moment anisotropy, magnetocrystalline anisotropy, and Dzyaloshinskii-Moriya interaction in W/Co/Pt trilayers

Chi, Z.*; 芝田 悟朗; 藤森 淳; 他15名*

Physical Review B, 110, p.184401_1 - 184401_8, 2024/11

 被引用回数:0 パーセンタイル:0.00(Materials Science, Multidisciplinary)

We have studied the Co layer thickness dependences of magnetocrystalline anisotropy (MCA), Dzyaloshinskii-Moriya interaction (DMI), and orbital moment anisotropy (OMA) in W/Co/Pt trilayers, in order to clarify their correlations with each other. We find that the MCA favors magnetization along the film normal and monotonically increases with decreasing effective magnetic layer thickness ($$t_{rm eff}$$). The magnitude of the Dzyaloshinskii-Moriya exchange constant ($$|D|$$) increases with decreasing $$t_{rm eff}$$ until $$T_{rm eff}$$ $$sim$$ 1 nm, below which $$|D|$$ decreases. The MCA and $$|D|$$ scale with 1/$$T_{rm eff}$$ for $$t_{rm eff}$$ larger than $$sim 1$$ nm, indicating an interfacial origin. Using X-ray magnetic circular dichroism (XMCD), we find non-zero OMA when $$t_{rm eff}$$ is smaller than $$sim 0.8$$ nm. The OMA increases with decreasing $$t_{rm eff}$$ more rapidly than what is expected from the MCA, indicating that factors other than OMA contribute to the MCA at small $$t_{rm eff}$$.

論文

強磁性5$$d$$ $$j_{eff}=3/2$$絶縁体Sr$$_3$$OsO$$_6$$のX線磁気円二色性測定

若林 勇希*; Krockenberger, Y.*; 山神 光平*; 和達 大樹*; 芝田 悟朗; 藤森 淳*; 河村 直己*; 鈴木 基寛*; 谷保 芳孝*; 山本 秀樹*

SPring-8/SACLA利用研究成果集(インターネット), 12(5), p.291 - 293, 2024/10

本研究では、高温強磁性酸化物Sr$$_3$$OsO$$_6$$の電子状態を明らかにすることを目的として、Os $$L_{2,3}$$吸収端におけるX線吸収分光(XAS)及びX線磁気円二色性(XMCD)測定を行った。実験結果から、Osの軌道磁気モーメントがスピン磁気モーメントと同程度のオーダーであることが明らかになった。しかし、XMCD総和則による推定では、軌道磁気モーメントはSQUID磁化測定の値よりもかなり小さかった。今後の課題としては、SrやOの吸収端でのXMCD測定による磁気モーメントの観測や、サンプルの経時変化を低減させるための対策が挙げられる。

論文

Origin of magnetically dead layers in spinel ferrites $$M$$Fe$$_2$$O$$_4$$ grown on Al$$_2$$O$$_3$$; Effects of postdeposition annealing studied by XMCD

野中 洋亮*; 若林 勇希*; 芝田 悟朗; 坂本 祥哉*; 池田 啓祐*; Chi, Z.*; Wan, Y.*; 鈴木 雅弘*; 田中 新*; 田中 雅明*; et al.

Physical Review Materials (Internet), 7(4), p.044413_1 - 044413_10, 2023/04

 被引用回数:5 パーセンタイル:47.86(Materials Science, Multidisciplinary)

We study the electronic and magnetic states of as-grown and annealed $$M$$Fe$$_2$$O$$_4$$(111)/Al$$_2$$O3(111) ($$M =$$Co, Ni) thin films with various thicknesses grown on Si(111) substrates with the $$gamma$$-Al$$_2$$O$$_3$$(111)buffer layers by using X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD), to investigate magnetically dead layers in these films. Although the magnetically dead layers in the as-grown samples are formed near the interface with the Al$$_2$$O$$_3$$ buffer layer, we reveal that ferrimagnetic order is partially recovered by postdeposition annealing at 973 K for 48 hours in air. By analyzing the line shapes of the XAS and XMCD spectra, we conclude that, in the dead layers, there are a significant number of vacancies at the $$T_d$$ sites of the spinel structure, which may be the microscopic origin of the degraded ferrimagnetic order in the $$M$$Fe$$_2$$O$$_4$$ thin films.

論文

Weyl-Kondo semimetal behavior in the chiral structure phase of Ce$$_{3}$$Rh$$_{4}$$Sn$$_{13}$$

岩佐 和晃*; Suyama, Kazuya*; 河村 聖子; 中島 健次; Raymond, S.*; Steffens, P.*; Yamada, Akira*; 松田 達磨*; 青木 勇二*; 川崎 郁斗; et al.

Physical Review Materials (Internet), 7(1), p.014201_1 - 014201_11, 2023/01

 被引用回数:4 パーセンタイル:39.92(Materials Science, Multidisciplinary)

The spin dynamics, crystalline-electric-field (CEF) level scheme, specific heat, and X-ray photoemission spectra (XPS) of Ce$$_{3}$$Rh$$_{4}$$Sn$$_{13}$$ were investigated, which exhibits anomalous semimetal transport in the chiral crystallographic phase. CEF excitations observed at approximately 7 and 39 meV are consistent with the two inequivalent Ce-ion cites in the chiral structure. Because of broader CEF excitations and a strong 4$$f^{1}$$ peak at the Fermi level in the Ce 4$$f$$ on-resonance spectrum, the hybridized Ce 4$$f$$ electrons contribute to the semimetal carriers. In addition, the spin fluctuation associated with the Kramers doublet ground state is characterized by the peak located at 0.15 meV. The electronic state involving the spin fluctuation causes the $$T^{3}$$ behavior of specific heat below 0.6 K, which is attributed to linear dispersion relations of electrons of the Weyl Kondo semimetal in the chiral-lattice symmetry.

論文

垂直磁気異方性を示す鉄挿入遷移金属ダイカルコゲナイドFe$$_x$$TaS$$_2$$のX線磁気円二色性による研究; Fe$$_x$$TiS$$_2$$との比較

芝田 悟朗; Won, C.*; Kim, J.*; 野中 洋亮*; 池田 啓祐*; Wan, Y.*; 鈴木 雅弘*; 小出 常晴*; 田中 新*; Cheong, S.-W.*; et al.

Photon Factory Activity Report 2022 (インターネット), 2 Pages, 2023/00

Feをインターカレートした遷移金属ダイカルコゲナイド化合物Fe$$_x$$TiS$$_2$$およびFe$$_x$$TaS$$_2$$は、巨大な保磁力および垂直磁気異方性を示す強磁性体になることが知られている。我々は以前、Fe$$_x$$TiS$$_2$$についてのX線磁気円二色性(XMCD)実験の結果から、Fe$$^{2+}$$の凍結していない軌道磁気モーメントが結晶場の1次摂動によって直接磁気異方性エネルギーを生むことを明らかにした。今回、Fe$$_x$$TiS$$_2$$よりもさらに強い磁気異方性を示す遷移金属ダイカルコゲナイドFe$$_x$$TaS$$_2$$について同様にXMCD実験を行い、磁気異方性の強さが何によって左右されているかを探ることを試みた。

論文

Cr doping-induced ferromagnetism in the spin-glass Cd$$_{1-x}$$Mn$$_x$$Te studied by X-ray magnetic circular dichroism

Verma, V.*; 坂本 祥哉*; 石川 弘一郎*; Singh, V. R.*; 石上 啓介*; 芝田 悟朗; 門野 利治*; 小出 常晴*; 黒田 真司*; 藤森 淳*

Physica B; Condensed Matter, 642, p.414129_1 - 414129_5, 2022/10

 被引用回数:5 パーセンタイル:36.31(Physics, Condensed Matter)

The prototypical diluted magnetic semiconductor Cd$$_{1-x}$$Mn$$_x$$Te is a spin glass ($$x < 0.6$$) or an antiferromagnet ($$x > 0.6$$) but becomes ferromagnetic upon doping with a small amount of Cr atoms. To investigate the origin of the ferromagnetism in Cd$$_{1-x-y}$$Mn$$_x$$Cr$$_y$$Te, we have studied its element specific magnetic properties by X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD). Measured XAS and XMCD spectra indicate that both Cr and Mn atoms are divalent and that the magnetic moments of Cr and Mn are aligned parallel. By analyzing the element-specific magnetization curves, we conclude that Cr doping leads to the formation of ferromagnetic or superparamagnetic clusters consisting of several Cr ions surrounded by a much larger number of Mn ions.

論文

Magnetic properties and electronic configurations of Mn ions in the diluted magnetic semiconductor Ba$$_{1-x}$$K$$_x$$(Zn$$_{1-y}$$Mn$$_y$$)$$_2$$As$$_2$$ studied by X-ray magnetic circular dichroism and resonant inelastic X-ray scattering

鈴木 博人*; Zhao, G.*; 岡本 淳*; 坂本 祥哉*; Chen, Z.-Y.*; 野中 洋亮*; 芝田 悟朗; Zhao, K.*; Chen, B.*; Wu, W.-B.*; et al.

Journal of the Physical Society of Japan, 91(6), p.064710_1 - 064710_5, 2022/06

 被引用回数:2 パーセンタイル:0.00(Physics, Multidisciplinary)

The magnetic properties and the electronic excitations of the new diluted magnetic semiconductor Ba$$_{1-x}$$K$$_x$$(Zn$$_{1-y}$$Mn$$_y$$)$$_2$$As$$_2$$ have been studied by X-ray magnetic circular dichroism (XMCD) and resonant inelastic X-ray scattering (RIXS). The sum rule analysis of the XMCD spectra indicates that the Mn atoms are in the high-spin configurations of $$d^5$$, whereas the presence of competing ferromagnetic and antiferromagnetic interactions between the Mn ions reduces the net spin moment. Based on a comparison of the RIXS line shapes with those of Ga$$_{1-x}$$Mn$$_x$$As, it is concluded that the ground state of Mn in Ba$$_{1-x}$$K$$_x$$(Zn$$_{1-y}$$Mn$$_y$$)$$_2$$As$$_2$$ consists of both the $$3d^5 underline{L}$$ and $$3d^5$$ electron configurations.

論文

Hybridization of Bogoliubov quasiparticles between adjacent CuO$$_2$$ layers in the triple-layer cuprate Bi$$_2$$Sr$$_2$$Ca$$_2$$Cu$$_3$$O$$_{10+delta}$$ studied by angle-resolved photoemission spectroscopy

出田 真一郎*; Johnston, S.*; 吉田 鉄平*; 田中 清尚*; 森 道康; 安齋 太陽*; 井野 明洋*; 有田 将司*; 生天目 博文*; 谷口 雅樹*; et al.

Physical Review Letters, 127(21), p.217004_1 - 217004_6, 2021/11

 被引用回数:13 パーセンタイル:71.00(Physics, Multidisciplinary)

Hybridization of Bogoliubov quasiparticles (BQPs) between the CuO$$_2$$ layers in the triple-layer cuprate high-temperature superconductor Bi$$_2$$Sr$$_2$$Ca$$_2$$Cu$$_3$$O$$_{10+delta}$$ is studied by angle-resolved photoemission spectroscopy (ARPES). In the superconducting state, an anti-crossing gap opens between the outer- and inner-BQP bands, which we attribute primarily to interlayer single-particle hopping with possible contributions from interlayer Cooper pairing. We find that the $$d$$-wave superconducting gap of both BQP bands smoothly develops with momentum without abrupt jump in contrast to a previous ARPES study. Hybridization between the BQPs also gradually increases in going from the off-nodal to the anti-nodal region, which is explained by the momentum-dependence of the interlayer single-particle hopping. As possible mechanisms for the enhancement of the superconducting transition temperature, the hybridization between the BQPs, as well as the combination of phonon modes of the triple CuO$$_2$$ layers and spin fluctuations are discussed.

論文

Alternation of magnetic anisotropy accompanied by metal-insulator transition in strained ultrathin manganite heterostructures

小林 正起*; Anh, L. D.*; 鈴木 雅弘*; 金田-高田 真悟*; 竹田 幸治; 藤森 伸一; 芝田 悟朗*; 田中 新*; 田中 雅明*; 大矢 忍*; et al.

Physical Review Applied (Internet), 15(6), p.064019_1 - 064019_10, 2021/06

 被引用回数:8 パーセンタイル:46.19(Physics, Applied)

A fundamental understanding of the interfacial magnetic properties in ferromagnetic heterostructures is essential for utilizing ferromagnetic materials for spintronic device applications. Here, we investigate the interfacial magnetic and electronic structures of epitaxial single-crystalline LaAlO$$_3$$(LAO)/La$$_{0.6}$$Sr$$_{0.4}$$MnO$$_3$$(LSMO)/Nb:SrTiO$$_3$$(Nb:STO) heterostructures with varying LSMO layer thicknesses, in which the magnetic anisotropy strongly changes with the LSMO thickness due to the delicate balance between strains originating from both the Nb:STO and LAO layers, using X-ray magnetic circular dichroism and photoemission spectroscopy. We successfully detect the clear change of the magnetic behavior of the Mn ions concomitant with the thickness-dependent metal-insulator transition. Our results suggest that the double-exchange interaction induces ferromagnetism in the metallic LSMO film under tensile strain caused by the STO substrate, while the superexchange interaction determines the magnetic behavior in the insulating LSMO film under compressive strain originating from the top LAO layer. The change in strain, depending on LSMO layer thickness, is confirmed by scanning transmission electron microscopy. Based on those findings, the formation of a magnetic dead layer near the LAO/LSMO interface is attributed to competition between the superexchange interaction via Mn $$3d_{3z^2-r^2}$$ orbitals under compressive strain and the double-exchange interaction via the $$3d_{x^2-y^2}$$ orbitals. These findings provide key aspects of ferromagnetic oxide heterostructures for the development of spintronic device applications.

論文

Direct observation of the magnetic ordering process in the ferromagnetic semiconductor Ga$$_{1-x}$$Mn$$_{x}$$As via soft X-ray magnetic circular dichroism

竹田 幸治; 大矢 忍*; Pham, N. H.*; 小林 正起*; 斎藤 祐児; 山上 浩志; 田中 雅明*; 藤森 淳*

Journal of Applied Physics, 128(21), p.213902_1 - 213902_11, 2020/12

 被引用回数:8 パーセンタイル:38.75(Physics, Applied)

In order to understand the mechanism of the ferromagnetism in Ga$$_{1-x}$$Mn$$_{x}$$As ((Ga,Mn)As), we have investigated the magnetic behavior on a microscopic level through systematic temperature ($$T$$) and magnetic-field ($$H$$) dependent soft X-ray magnetic circular dichroism (XMCD) experiments at the Mn $$L_mathrm{2,3}$$ absorption edges. The $$T$$ and $$H$$ dependences of XMCD intensities have been analyzed using a model consisting of the ferromagnetic (FM), paramagnetic, and superparamagnetic (SPM) components. Intriguingly, we have found a common behavior for the ferromagnetic ordering process in (Ga,Mn)As samples with different Mn concentrations and different Curie temperature ($$T_mathrm{C}$$) values. In particular, the SPM component develops well above $$T_mathrm{C}$$, indicating that local FM regions are formed well above $$T_mathrm{C}$$. The present findings indicate that the onset of ferromagnetic ordering is triggered by local electronic states around the substitutional Mn ions. Insight into the most representative ferromagnetic semiconductor, (Ga,Mn)As, will be an important step in understanding the mechanism of ferromagnetic ordering in various ferromagnetic semiconductor families.

論文

Evolution of Fe 3$$d$$ impurity band state as the origin of high Curie temperature in the $$p$$-type ferromagnetic semiconductor (Ga,Fe)Sb

武田 崇仁*; 坂本 祥哉*; 荒木 恒星*; 藤澤 唯太*; Anh, L. D.*; Tu, N. T.*; 竹田 幸治; 藤森 伸一; 藤森 淳*; 田中 雅明*; et al.

Physical Review B, 102(24), p.245203_1 - 245203_8, 2020/12

 被引用回数:7 パーセンタイル:34.47(Materials Science, Multidisciplinary)

(Ga$$_{1-x}$$,Fe$$_x$$)Sb is one of the promising ferromagnetic semiconductors for spintronic device applications because its Curie temperature (Tc) is above 300 K when the Fe concentration $$x$$ is equal to or higher than 0.20. However, the origin of the high Tc in (Ga,Fe)Sb remains to be elucidated. To address this issue, we use resonant photoemission spectroscopy (RPES) and first-principles calculations to investigate the x dependence of the Fe 3$$d$$ states in (Ga$$_{1-x}$$,Fe$$_x$$)Sb ($$x$$ = 0.05, 0.15, and 0.25) thin films. The observed Fe 2$$p$$-3$$d$$ RPES spectra reveal that the Fe-3$$d$$ impurity band (IB) crossing the Fermi level becomes broader with increasing $$x$$, which is qualitatively consistent with the picture of double-exchange interaction. Comparison between the obtained Fe-3$$d$$ partial density of states and the first-principles calculations suggests that the Fe-3$$d$$ IB originates from the minority-spin ($$downarrow$$) $$e$$ states. The results indicate that enhancement of the double-exchange interaction between $$e_{downarrow}$$ electrons with increasing $$x$$ is the origin of the high Tc in (Ga,Fe)Sb.

論文

Electronic structure of the high-$$T_{rm C}$$ ferromagnetic semiconductor (Ga,Fe)Sb; X-ray magnetic circular dichroism and resonance photoemission spectroscopy studies

坂本 祥哉*; Tu, N. T.*; 竹田 幸治; 藤森 伸一; Hai, P. N.*; Anh, L. D.*; 若林 勇希*; 芝田 悟朗*; 堀尾 眞史*; 池田 啓祐*; et al.

Physical Review B, 100(3), p.035204_1 - 035204_8, 2019/07

The electronic structure and the magnetism of the ferromagnetic semiconductor (Ga,Fe)Sb, whose Curie temperature $$T_{rm C}$$ can exceed room temperature, were investigated by means of X-ray absorption spectroscopy (XAS), X-ray magnetic circular dichroism (XMCD), and resonance photoemission spectroscopy (RPES). The line-shape analyses of the XAS and XMCD spectra suggest that the ferromagnetism is of intrinsic origin. The orbital magnetic moments deduced using XMCD sum rules were found to be large, indicating that there is a considerable 3$$d^{6}$$ contribution to the ground state of Fe. From RPES, we observed a strong dispersive Auger peak and nondispersive resonantly enhanced peaks in the valence-band spectra. The latter is a fingerprint of the correlated nature of Fe 3$$d$$ electrons, whereas the former indicates their itinerant nature. It was also found that the Fe 3$$d$$ states have a finite contribution to the density of states at the Fermi energy. These states, presumably consisting of majority-spin $$p$$-$$d$$ hybridized states or minority-spin e states, would be responsible for the ferromagnetic order in this material.

論文

Electronic structure of the high-$$T_{rm C}$$ ferromagnetic semiconductor (Ga,Fe)Sb; X-ray magnetic circular dichroism and resonance photoemission spectroscopy studies

坂本 祥哉*; Tu, N. T.*; 竹田 幸治; 藤森 伸一; Hai, P. N.*; Anh, L. D.*; 若林 勇希*; 芝田 悟朗*; 堀尾 眞史*; 池田 啓祐*; et al.

Physical Review B, 100(3), p.035204_1 - 035204_8, 2019/07

 被引用回数:17 パーセンタイル:60.65(Materials Science, Multidisciplinary)

The electronic structure and the magnetism of the ferromagnetic semiconductor (Ga,Fe)Sb, whose Curie temperature $$T_{rm C}$$ can exceed room temperature, were investigated by means of X-ray absorption spectroscopy (XAS), X-ray magnetic circular dichroism (XMCD), and resonance photoemission spectroscopy (RPES). The line-shape analyses of the XAS and XMCD spectra suggest that the ferromagnetism is of intrinsic origin. The orbital magnetic moments deduced using XMCD sum rules were found to be large, indicating that there is a considerable 3$$d^{6}$$ contribution to the ground state of Fe. From RPES, we observed a strong dispersive Auger peak and nondispersive resonantly enhanced peaks in the valence-band spectra. The latter is a fingerprint of the correlated nature of Fe 3$$d$$ electrons, whereas the former indicates their itinerant nature. It was also found that the Fe 3$$d$$ states have a finite contribution to the density of states at the Fermi energy. These states would be responsible for the ferromagnetic order in this material.

論文

Manifestation of electron correlation effect in 5$$f$$ states of uranium compounds revealed by 4$$d$$-5$$f$$ resonant photoelectron spectroscopy

藤森 伸一; 小畠 雅明; 竹田 幸治; 岡根 哲夫; 斎藤 祐児; 藤森 淳; 山上 浩志; 芳賀 芳範; 山本 悦嗣; 大貫 惇睦*

Physical Review B, 99(3), p.035109_1 - 035109_5, 2019/01

 被引用回数:14 パーセンタイル:53.84(Materials Science, Multidisciplinary)

In the present study, we have elucidated the nature of the electron correlation effect in uranium compounds by imaging the partial $$mathrm{U}~5f$$ density of states (pDOS) of typical itinerant, localized, and heavy fermion uranium compounds by using the $$mathrm{U}$$ 4$$d$$-5$$f$$ resonant photoemission spectroscopy. Obtained $$mathrm{U}~5$$ pDOS exhibit a systematic trend depending on the physical properties of compounds: Although the coherent peak at the Fermi level can be explained by the band-structure calculation, an incoherent peak emerges on the higher binding energy side ($$lesssim 1~mathrm{eV}$$) in the cases of localized and heavy fermion compounds. The intensity and energy position of the incoherent peak is increased and shifted to a higher binding energy as the localization of the $$mathrm{U}~5$$ state increases. These behaviors are consistent with the prediction of the Mott metal-insulator transition, suggesting that the Hubbard-$$U$$ type mechanism takes an essential role in the $$5f$$ electronic structure of actinide materials.

論文

Electronic structure of URu$$_2$$Si$$_2$$ studied by photoelectron spectroscopy (INVITED)

藤森 伸一; 竹田 幸治; 岡根 哲夫; 斎藤 祐児; 藤森 淳; 山上 浩志; 芳賀 芳範; 山本 悦嗣; 大貫 惇睦*

Progress in Nuclear Science and Technology (Internet), 5, p.82 - 85, 2018/11

One of the most remarkable properties of actinide compounds is the coexistence of superconductivity and magnetic ordering which has been realized in several strongly-correlated uranium based compounds. In these compounds, both superconductivity and magnetic ordering originate from U 5f states. To understand the origin of the coexistence as well as the mechanism of the superconductivity, it is essential to reveal their U 5f electronic structures. In this presentation, the U 5f electronic structures of heavy Fermion superconductors UPd$$_2$$Al$$_3$$ and URu$$_2$$Si$$_2$$ studied by photoelectron spectroscopy using soft X-rays from SPring-8 BL23SU are presented. For UPd$$_2$$Al$$_3$$, U 4d-5f resonant photoemission experiment was performed, and its partial U 5f spectrum was revealed experimentally. Furthermore, we have applied the three-dimentional ARPES to the hidden order compound URu$$_2$$Si$$_2$$, and revealed its complete 3D electronic structure in the paramagnetic phase. Their electronic structures are discussed based on these results.

論文

Local magnetic states of the weakly ferromagnetic iron-based superconductor Sr$$_{2}$$VFeAsO$$_{3-delta}$$ studied by X-ray magnetic circular dichroism

堀尾 眞史*; 竹田 幸治; 並木 宏允*; 片桐 隆雄*; 若林 勇希*; 坂本 祥哉*; 野中 洋亮*; 芝田 悟朗*; 池田 啓祐*; 斎藤 祐児; et al.

Journal of the Physical Society of Japan, 87(10), p.105001_1 - 105001_2, 2018/10

 被引用回数:2 パーセンタイル:18.95(Physics, Multidisciplinary)

We have performed X-ray magnetic circular dichroism (XMCD) measurements on the iron-based superconductor Sr$$_{2}$$VFeAsO$$_{3-delta}$$ to study the origin of weak ferromagnetism (WFM) reported for this compound. While Fe 3d electrons show a magnetic response similar to the other iron pnictides, signals from V 3d electrons remain finite at zero magnetic field and may be responsible for the WFM.

論文

Cation distribution and magnetic properties in ultrathin (Ni$$_{1-x}$$Co$$_{x}$$)Fe$$_{2}$$O$$_{4}$$ (x=0-1) layers on Si(111) studied by soft X-ray magnetic circular dichroism

若林 勇希*; 野中 洋亮*; 竹田 幸治; 坂本 祥哉*; 池田 啓祐*; Chi, Z.*; 芝田 悟朗*; 田中 新*; 斎藤 祐児; 山上 浩志; et al.

Physical Review Materials (Internet), 2(10), p.104416_1 - 104416_12, 2018/10

 被引用回数:14 パーセンタイル:42.78(Materials Science, Multidisciplinary)

We study the electronic structure and magnetic properties of epitaxial (Ni$$_{1-x}$$Co$$_{x}$$)Fe$$_{2}$$O$$_{4}$$(111) layers with thicknesses $$d$$ = 1.7 - 5.2 nm grown on Al$$_{2}$$O$$_{3}$$(111)/Si(111) structures. We revealed the crystallographic (octahedral $$O_{h}$$ or tetrahedral $$T_{d}$$) sites and the valences of the Fe, Co, and Ni cations using experimental soft X-ray absorption spectroscopy and X-ray magnetic circular dichroism spectra and configuration-interaction cluster-model calculation.

論文

Electronic structures of U$$X_3$$ ($$X$$=Al, Ga, and In) studied by photoelectron spectroscopy

藤森 伸一; 小畠 雅明; 竹田 幸治; 岡根 哲夫; 斎藤 祐児; 藤森 淳; 山上 浩志; 芳賀 芳範; 山本 悦嗣; 大貫 惇睦*

Physical Review B, 96(11), p.115126_1 - 115126_10, 2017/09

 被引用回数:7 パーセンタイル:32.12(Materials Science, Multidisciplinary)

The electronic structures of U$$X_3$$ ($$X$$=Al, Ga, and In) were studied by photoelectron spectroscopy to understand the relationship between their electronic structure and magnetic properties. The band structures and Fermi surfaces of UAl$$_3$$ and UGa$$_3$$ were revealed experimentally by angle-resolved photoelectron spectroscopy (ARPES), and they were compared with the result of band structure calculations. The topologies of the Fermi surfaces and the band structures of UAl$$_3$$ and UGa$$_3$$ were explained reasonably well by the calculation, although bands near the Fermi level ($$E_mathrm{F}$$) were renormalized owing to the finite electron correlation effect. The topologies of the Fermi surfaces of UAl$$_3$$ and UGa$$_3$$ are very similar to each other, except for some minor differences. Such minor differences in their Fermi surface or electron correlation effect might take an essential role in their magnetism.

論文

Electronic structure of ThRu$$_2$$Si$$_2$$ studied by angle-resolved photoelectron spectroscopy; Elucidating the contribution of U 5$$f$$ states in URu$$_{2}$$Si$$_{2}$$

藤森 伸一; 小畠 雅明; 竹田 幸治; 岡根 哲夫; 斎藤 祐児; 藤森 淳; 山上 浩志; 松本 裕司*; 山本 悦嗣; 立岩 尚之; et al.

Physical Review B, 96(12), p.125117_1 - 125117_9, 2017/09

 被引用回数:11 パーセンタイル:44.75(Materials Science, Multidisciplinary)

The Fermi surface and band structure of $$mathrm{ThRu}_2mathrm{Si}_2$$ have been studied by angle resolved photoelectron spectroscopy (ARPES) with the incident photon energies of $$hnu$$ = 665-735 eV. Detailed band structure and the three-dimensional shape of the Fermi surface were derived experimentally, and they are quantitatively explained by the band-structure calculation based on the density functional approximation. Comparison of the experimental ARPES spectra of $$mathrm{ThRu}_2mathrm{Si}_2$$ with those of $$mathrm{URu}_2mathrm{Si}_2$$ shows that they have considerably different spectral profiles particularly in the energy range of $$E_mathrm{B} = E_mathrm{F}$$ - 1 eV. Some energy bands with their energy dispersions of about 1 eV observed in $$mathrm{URu}_2mathrm{Si}_2$$ are missing in the ARPES spectra of $$mathrm{ThRu}_2mathrm{Si}_2$$ measured along the same high symmetry line of Brillouin zone, suggesting that U 5$$f$$ states form these bands in $$mathrm{URu}_2mathrm{Si}_2$$. The relationship between the ARPES spectra of $$mathrm{URu}_2mathrm{Si}_2$$ and $$mathrm{ThRu}_2mathrm{Si}_2$$ is very different from the case between $$mathrm{CeRu}_2mathrm{Si}_2$$ and $$mathrm{LaRu}_2mathrm{Si}_2$$ where their intrinsic difference is limited only in the very vicinity of the Fermi energy. The present result argues that the U 5$$f$$ electrons in $$mathrm{URu}_2mathrm{Si}_2$$ have strong hybridization with ligand states, and essentially have an itinerant character.

167 件中 1件目~20件目を表示