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論文

Magnetization process of the layered diluted ferromagnetic semiconductor (Ba,K)(Zn,Mn)$$_2$$As$$_2$$ studied by X-ray magnetic circular dichroism

Wan, Y.*; 芝田 悟朗; 竹田 幸治*; 岡根 哲夫; 斎藤 祐児; 山上 浩志; 藤森 淳*; 他10名*

Physical Review Materials (Internet), 10(5), p.054402_1 - 054402_8, 2026/05

https://doi.org/10.1103/69sm-fz7z

In order to unveil the nature of the ferromagnetism in (Ba,K)(Zn,Mn)$$_2$$As$$_2$$, its magnetization process has been studied by X-ray magnetic circular dichroism (XMCD) at the Mn $$L_{2,3}$$ edge in a wide range of temperature and magnetic field. The average magnetization of the Mn atoms as a function of magnetic field ($$M$$-$$H$$ curves) at various temperatures could be successfully explained by a mixture of paramagnetic (PM), superparamagnetic (SPM), and ferromagnetic (FM) components as previously reported for GaMnAs, revealing the complex nature of the ferromagnetism in (Ba,K)(Zn,Mn)$$_2$$As$$_2$$. The average magnetization of the SPM clusters of different sizes and the FM regions were found to be small compared to those in GaMnAs, which we attribute to the antiferromagnetic interaction between nearest-neighbor Mn atoms in (Ba,K)(Zn,Mn)$$_2$$As$$_2$$ on the basis of recent theoretical predictions.

論文

3GeV陽子ビーム輸送施設のためのパルス偏向電磁石とセプタム電磁石の検討

山口 雄司; 近藤 恭弘; 明午 伸一郎; 高柳 智弘; 藤森 寛*; 篠崎 信一

Proceedings of 22nd Annual Meeting of Particle Accelerator Society of Japan (インターネット), p.655 - 660, 2026/03

https://www.pasj.jp/web_publish/pasj2025/proceedings/PDF/THP0/THP061.pdf

J-PARC 3GeV陽子ビーム輸送施設(3NBT)では、パルス偏向電磁石やセプタム電磁石等を用いて3GeVシンクロトロンからの陽子ビームを下流の施設へ供給する。3NBTの電磁石には供給先の施設の運転条件に適した性能が求められるため、要求される運転条件に応じて電磁石性能の高度化が必要となる。高度化における設計条件を明確にするために、既存の偏向電磁石等の仕様と運転条件からの要求仕様を比較し、高度化により得られる性能を見積もった結果、パルス偏向電磁石の動作の高速化とセプタム電磁石の磁極の拡張により要求される性能を達成でき、安定なビーム供給が可能であることがわかった。

論文

Simulations of magnetic field effects on 3-GeV proton beam brought by magnets for muon beam in future proton beam transport line of J-PARC

山口 雄司; 近藤 恭弘; 明午 伸一郎; 篠崎 信一; 高柳 智弘; 藤森 寛*; 河村 成肇*

Journal of Physics; Conference Series, 3094(1), p.012023_1 - 012023_5, 2025/09

https://doi.org/10.1088/1742-6596/3094/1/012023

J-PARCでは、3GeV陽子ビーム輸送施設によって3GeVシンクロトロンから物質・生命科学実験施設(MLF)へ大強度陽子ビームを輸送している。陽子ビーム輸送施設のビームライン最下流部には、ミュオンビーム輸送用の偏向電磁石とソレノイドがあるため、これらの磁場による3GeV陽子ビームへの影響を補正する必要がある。シミュレーションにより偏向電磁石による軌道のずれとソレノイドによるプロファイルの回転に伴う垂直方向ビームサイズの増大を模擬し、それぞれの影響を補正する方法を検討した結果、追加の偏向電磁石とソレノイドを用いることで補正でき、安定なビーム輸送が可能であることがわかった。

論文

Influence of magnetic ordering on quasiparticle spectral functions; Comparison of electronic states of CeCu$$_6$$ and CeRu$$_2$$Ge$$_2$$

川崎 郁斗; 藤森 伸一; 山上 浩志; 松田 達磨*; 大貫 惇睦*

Journal of the Physical Society of Japan, 94(8), p.084702_1 - 084702_9, 2025/07

https://doi.org/10.7566/JPSJ.94.084702
 被引用回数：0 パーセンタイル：0.00(Physics, Multidisciplinary)

The electronic state of CeCu$$_6$$, an archetypical heavy compound without long-range magnetic order, has been investigated by angle-resolved photoemission spectroscopy (ARPES) experiments using soft X rays. The Ce 3$$d$$-4$$f$$ resonant ARPES experiments have revealed the 4$$f$$ partial density of states consists of a quasiparticle band near the Fermi level ($$f^1$$ component) and an $$f^0$$ component, the latter of which is physically equivalent to the lower Hubbard band in the Hubbard model. The observed strong intensity of the $$f^0$$ component indicates that the quasiparticle band near the Fermi level is strongly renormalized by the electron correlation effect, consistent with the significantly enhanced electronic specific-heat coefficient of CeCu$$_6$$. We compare the present 3$$d$$-4$$f$$ resonant ARPES spectra of CeCu$$_6$$ with those for CeRu$$_2$$Ge$$_2$$, which has a low Kondo temperature similar to CeCu$$_6$$ but shows a ferromagnetic order. The results of this comparison suggest that the ferromagnetic correlation in CeRu$$_2$$Ge$$_2$$ seems to strongly suppress the degree of renormalization for the quasiparticle band. We also showed that the intensities of both the $$f^1$$ and $$f^0$$ components for CeCu$$_6$$ hardly depend on temperature.

論文

Pulsed muon facility of J-PARC MUSE

下村 浩一郎*; 幸田 章宏*; Pant, A. D.*; 砂川 光*; 藤森 寛*; 梅垣 いづみ*; 中村 惇平*; 藤原 理賀; 反保 元伸*; 河村 成肇*; et al.

Interactions (Internet), 245(1), p.31_1 - 31_6, 2024/12

https://doi.org/10.1007/s10751-024-01863-8
 被引用回数：3 パーセンタイル：92.77

J-PARC Muon Facility: MUSE (Muon Science Establishment) is responsible for the inter-university user program and the operation, maintenance, and construction of the muon beamlines, namely D-line, S-line, U-line, and H-line, along with the muon source at J-PARC Materials and Life Science Facility (MLF). In this paper, recent developments are briefly presented.

論文

Impact of the Ce$$4f$$ states in the electronic structure of the intermediate-valence superconductor CeIr$$_3$$

藤森 伸一; 川崎 郁斗; 竹田 幸治; 山上 浩志; 雀部 矩正*; 佐藤 芳樹*; 清水 悠晴*; 仲村 愛*; Maruya, A.*; 本間 佳哉*; et al.

Electronic Structure (Internet), 5(4), p.045009_1 - 045009_7, 2023/11

https://doi.org/10.1088/2516-1075/ad0a3d

The electronic structure of the $$f$$-based superconductor $$mathrm{CeIr_3}$$ was studied by photoelectron spectroscopy. The energy distribution of the $$mathrm{Ce}~4f$$ state was revealed by the $$mathrm{Ce}~3d-4f$$ resonant photoelectron spectroscopy. The $$mathrm{Ce}~4f$$ state was mostly distributed in the vicinity of the Fermi energy, suggesting the itinerant character of the $$mathrm{Ce}~4f$$ state. The contribution of the $$mathrm{Ce}~4f$$ state to the density of states (DOS) at the Fermi energy was estimated to be nearly half of that of the$$mathrm{Ir}~5d$$ states, implying that the $$mathrm{Ce}~4f$$ state has aconsiderable contribution to the DOS at the Fermi energy. The $$mathrm{Ce}~3d$$ core-level and $$mathrm{Ce}~3d$$ X-ray absorption spectra were analyzed based on a single-impurity Anderson model. The number of the $$mathrm{Ce}~4f$$ state in the ground state was estimated to be 0.8-0.9, which is much larger than the values obtained in the previous studies (i.e., 0-0.4).

論文

Strongly renormalized quasiparticles in UPt$$_3$$

川崎 郁斗; 竹内 一陽*; 藤森 伸一; 竹田 幸治; 山上 浩志; 山本 悦嗣; 芳賀 芳範

Physical Review B, 108(16), p.165127_1 - 165127_9, 2023/10

https://doi.org/10.1103/PhysRevB.108.165127
 被引用回数：2 パーセンタイル：15.21(Materials Science, Multidisciplinary)

We performed angle-resolved photoemission spectroscopy (ARPES) experiments using soft X rays to investigate the electronic structure of the heavy-fermion superconductor UPt$$_3$$. The overall band structure revealed by the present ARPES measurements is compared with density-functional calculations for UPt$$_3$$ and the non-$$5f$$ reference compound ThPt$$_3$$. We showed that the calculation for ThPt$$_3$$ gives a better description of the experimental band structure, except for the $$5f$$-derived heavy quasiparticle bands. This situation is reminiscent of Ce-based heavy-fermion systems, whose band structures are often very similar to those of non-$$4f$$ La-based compounds. The narrow heavy quasiparticle bands are located just below the Fermi level ($$E_{rm F}$$), and their band structure could not be resolved by the present energy resolution. We also showed that most of the U $$5f$$ spectral weight exists not as the coherent heavy-fermion bands but as incoherent components that distribute over a wide energy range, spanning from near $$E_{rm F}$$ to approximately 2 eV. This result indicates that the heavy quasiparticle bands are enormously renormalized by the electron correlation effect. Additionally, we showed that the spectral intensity of the heavy-fermion bands is almost temperature independent, at least up to 100 K, where the magnetic susceptibility follows a Curie-Weiss behavior.

論文

Quasiparticle state in 4$$f$$ localized ferromagnet CeRu$$_2$$Ge$$_2$$ studied by soft X-ray photoemission spectroscopy

川崎 郁斗; 藤森 伸一; 竹田 幸治; 山上 浩志; 大貫 惇睦*

Journal of the Physical Society of Japan, 92(6), p.064709_1 - 064709_8, 2023/06

https://doi.org/10.7566/JPSJ.92.064709
 被引用回数：1 パーセンタイル：15.13(Physics, Multidisciplinary)

The electronic state of 4$$f$$ localized ferromagnet CeRu$$_2$$Ge$$_2$$ has been investigated by angle-resolved photoemission spectroscopy (APRES) experiments using soft X rays. The band structure and Fermi surfaces consisting of non-4$$f$$ bands are almost consistent with a calculation based on the density-functional theory for LaRu$$_2$$Ge$$_2$$, thus confirming a localized character of the 4$$f$$ electrons. On the other hand, the Ce 3$$d$$-4$$f$$ resonant ARPES experiments demonstrated that the 4$$f$$ spectral function is dominated by $$f^{1}$$ components in the vicinity of the Fermi level and thus is different from that expected for a localized electron system. We also revealed that the intensities of the $$f^{1}$$ components have almost no temperature dependence up to at least 100 K, which is two orders of magnitude larger than the Kondo temperature of CeRu$$_2$$Ge$$_2$$.

論文

Present status of J-PARC MUSE

下村 浩一郎*; 幸田 章宏*; Pant, A. D.*; 名取 寛顕*; 藤森 寛*; 梅垣 いづみ*; 中村 惇平*; 反保 元伸*; 河村 成肇*; 手島 菜月*; et al.

Journal of Physics; Conference Series, 2462, p.012033_1 - 012033_5, 2023/03

https://doi.org/10.1088/1742-6596/2462/1/012033
 被引用回数：2 パーセンタイル：93.04(Physics, Applied)

At J-PARC MUSE, since the $$mu$$SR2017 conference and up to FY2022, there have been several new developments at the facility, including the completion of a new experimental area S2 at the surface muon beamline S-line and the first muon beam extraction to the H1 area in the H-line, mainly to carry out high-statistics fundamental physics experiments. Several new studies are also underway, such as applying negative muon non-destructive elemental analysis to the analysis of samples returned from the asteroid Ryugu in the D2 area of the D-line. This paper reports on the latest status of MUSE.

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

https://doi.org/10.1103/PhysRevMaterials.7.014201
 被引用回数：6 パーセンタイル：37.93(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

Electronic structure of ThPd$$_2$$Al$$_3$$; Impact of the U $$5f$$ states on the electronic structure of UPd$$_2$$Al$$_3$$

藤森 伸一; 竹田 幸治; 山上 浩志; Posp$'i$$v{s}$il, J.*; 山本 悦嗣; 芳賀 芳範

Physical Review B, 105(11), p.115128_1 - 115128_6, 2022/03

https://doi.org/10.1103/PhysRevB.105.115128
 被引用回数：1 パーセンタイル：4.73(Materials Science, Multidisciplinary)

The electronic structure of $$mathrm{ThPd_2Al_3}$$, which is isostructural to the heavy fermion superconductor $$mathrm{UPd_2 Al_3}$$, was investigated by photoelectron spectroscopy. The band structure and Fermi surfaces of $$mathrm{ThPd_2Al_3}$$ were obtained by angle-resolved photoelectron spectroscopy (ARPES), and the results were well-explained by the band-structure calculation based on the local density approximation. The comparison between the ARPES spectra and the band-structure calculation suggests that the Fermi surface of $$mathrm{ThPd_2Al_3}$$ mainly consists of the $$mathrm{Al}~3p$$ and $$mathrm{Th}~6d$$ states with a minor contribution from the $$mathrm{Pd}~4d$$ states. The comparison of the band structures between $$mathrm{ThPd_2Al_3}$$ and $$mathrm{UPd_2Al_3}$$ argues that the $$mathrm{U}~5f$$ states form Fermi surfaces in $$mathrm{UPd_2Al_3}$$ through hybridization with the $$mathrm{Al}~3p$$ state in the $$mathrm{Al}$$ layer, suggesting that the Fermi surface of $$mathrm{UPd_2Al_3}$$ has a strong three-dimensional nature.

論文

Electronic structure of the intermediate-valence compound EuNi$$_2$$P$$_2$$ studied by soft X-ray photoemission spectroscopy

川崎 郁斗; 小畠 雅明; 藤森 伸一; 竹田 幸治; 山上 浩志; 辺土 正人*; 仲間 隆男*; 大貫 惇睦*

Physical Review B, 104(16), p.165124_1 - 165124_8, 2021/10

https://doi.org/10.1103/PhysRevB.104.165124
 被引用回数：1 パーセンタイル：3.70(Materials Science, Multidisciplinary)

We carried out angle-resolved photoemission (ARPES) experiments using soft X rays to investigate the electronic structure of the intermediate valence compound EuNi$$_2$$P$$_2$$. Both the Eu$$^{2+}$$ and Eu$$^{3+}$$ components arising from the 4$$f^6$$ and 4$$f^5$$ final states were observed in the valence spectra, directly confirming an intermediate character of Eu ions. The three-dimensional band structure was studied by ARPES measurements, and we found that the ARPES spectra up to just below the Fermi level can well be explained by a calculation based on the density-functional theory for the non-4$$f$$ reference compound SrNi$$_2$$P$$_2$$. The heavy-fermion bands in EuNi$$_2$$P$$_2$$ are thus considered to be formed through the hybridization between the dispersive valence bands, which resemble those for SrNi$$_2$$P$$_2$$, and the Eu$$^{2+}$$ components located at the very vicinity of the Fermi level.

論文

Electronic structure of URu$$_2$$Si$$_2$$ in paramagnetic phase; Three-dimensional angle resolved photoelectron spectroscopy study

藤森 伸一; 竹田 幸治; 山上 浩志; 山本 悦嗣; 芳賀 芳範

Electronic Structure (Internet), 3(2), p.024008_1 - 024008_8, 2021/06

https://doi.org/10.1088/2516-1075/abfd20

The three-dimensional (3D) electronic structure of the hidden order compound $$mathrm{URu_2Si_2}$$ in a paramagnetic phase was revealed using a 3D angle-resolved photoelectron spectroscopy where the electronic structure of the entire Brillouin zone is obtained by scanning both incident photon energy and detection angles of photoelectrons. The quasi-particle bands with enhanced contribution from the $$mathrm{U}~5f$$ state were observed near $$E_mathrm{F}$$, formed by the hybridization with the $$mathrm{Ru}~4d$$ states. The energy dispersion of the quasi-particle band is significantly depend on$$k_z$$, indicating that they inherently have a 3D nature. The band-structure calculation qualitatively explain the characteristic features of the band structure and Fermi surface although the electron correlation effect strongly renormalizes the quasi-particle bands. The 3D and strongly-correlated nature of the quasi-particle bands in$$mathrm{URu_2Si_2}$$ is an essential ingredient for modeling its hidden-order transition.

論文

Core-level photoelectron spectroscopy study of UTe$$_{2}$$

藤森 伸一; 川崎 郁斗; 竹田 幸治; 山上 浩志; 仲村 愛*; 本間 佳哉*; 青木 大*

Journal of the Physical Society of Japan, 90(1), p.015002_1 - 015002_2, 2021/01

https://doi.org/10.7566/JPSJ.90.015002
 被引用回数：24 パーセンタイル：81.02(Physics, Multidisciplinary)

The valence state of $$mathrm{UTe}_2$$ was studied by core-level photoelectron spectroscopy. The main peak position of the $$mathrm{U}~4f$$ core-level spectrum of $$mathrm{UTe}_2$$ coincides with that of $$mathrm{UB}_2$$, which is anitinerant compound with a nearly $$5f^3$$ configuration. However, the main peak of $$mathrm{UTe}_2$$ is broader than that of $$mathrm{UB}_2$$, and satellite structures are observed in the higher binding energy side of the main peak, which are characteristics of mixed-valence uranium compounds. These results suggest that the $$mathrm{U}~5f$$ state in $$mathrm{UTe}_2$$ isin a mixed valence state with a dominant contribution from the itinerant$$5f^3$$ configuration.

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

https://doi.org/10.1063/5.0031605
 被引用回数：9 パーセンタイル：38.08(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

Two-parameter model for optimizing target beam distribution with an octupole magnet

明午 伸一郎; 大井 元貴; 藤森 寛*

Physical Review Accelerators and Beams (Internet), 23(6), p.062802_1 - 062802_24, 2020/06

https://doi.org/10.1103/PhysRevAccelBeams.23.062802
 被引用回数：5 パーセンタイル：39.16(Physics, Nuclear)

加速器駆動の核変換システム(ADS)や核破砕中性子源に用いられる陽子加速器のビーム出力増強につれ、ビーム窓や標的の損傷は深刻な問題となり、損傷緩和のためにビーム電流密度の均一化が重要となる。密度均一化のため比較的よく用いられるラスター磁石には、故障時のビーム集束の重大な問題がある。一方、非線形光学を用いたビーム平坦化にはビーム拡大の問題があることが指摘され、これまで非線形効果導入の八極磁石におけるビームの角度の広がりを無視したフィラメント近似模型による検討が行われた。フィラメント近似模型では、非線形収斂作用を適切に評価できないため、本研究では一般化した非線形モデルの適用により非線形ビーム光学における収斂および発散作用を詳細に検討した。正規化した八極強度$$ K^{*}_8 $$と位相進行$$phi$$における$$cotphi$$の2つのパラメータ導入により、非線形効果を特定な条件によらず一般化できることを明確にした。ビームのピーク密度低減と損失最小化という拮抗する問題の解決には、$$K^{*}_8 sim $$ 1および$$ cotphisim$$ 3とすることにより解決できることが判明した。J-PARCの陽子ビーム輸送系(3NBT)に本検討結果を適用し、核破砕中性子源の水銀標的入口のビーム形状の比較検討した結果、モデル計算によるビーム分布は実験データとよい一致を示し、線形光学においてピーク電流密度を約50%にできることを示した。

論文

Electronic structure of trivalent compound EuPd$$_3$$ studied by soft X-ray angle-resolved photoemission spectroscopy

川崎 郁斗; 小畠 雅明; 藤森 伸一; 竹田 幸治; 山上 浩志; 仲村 愛*; 伊覇 航*; 辺土 正人*; 仲間 隆男*; 大貫 惇睦*

Journal of the Physical Society of Japan, 89(4), p.044704_1 - 044704_6, 2020/04

https://doi.org/10.7566/JPSJ.89.044704
 被引用回数：3 パーセンタイル：22.83(Physics, Multidisciplinary)

EuPd$$_3$$ is a rare Eu-based compound, whose Eu ions are in a trivalent state. The electronic structure of EuPd$$_3$$ was investigated by angle-resolved photoemission spectroscopy (ARPES) using soft X rays. Eu$$^{3+}$$ components arising from the 4f$$^5$$ final state multiplet were clearly observed in the valence spectra, and no Eu$$^{2+}$$ components were observed within an experimental accuracy, confirming a robust Eu$$^{3+}$$ state. The band structure and Fermi surfaces revealed by ARPES measurements were compared to the band structure calculations based on the density-functional theory for LaPd$$_3$$ andYPd$$_3$$. We found that the calculation for LaPd$$_3$$ provides a better description for our ARPES results. The effective electron masses estimated from the ARPES spectra near the Fermi level are in good agreement with the corresponding cyclotron effective masses in previous de Haas-van Alphen experiments.

論文

Electronic structure of UTe$$_2$$ studied by photoelectron spectroscopy

藤森 伸一; 川崎 郁斗; 竹田 幸治; 山上 浩志; 仲村 愛*; 本間 佳哉*; 青木 大*

Journal of the Physical Society of Japan, 88(10), p.103701_1 - 103701_5, 2019/10

https://doi.org/10.7566/JPSJ.88.103701
 被引用回数：51 パーセンタイル：89.59(Physics, Multidisciplinary)

The electronic structure of the unconventional superconductor $$mathrm{UTe_2}$$ was studied by resonant photoelectron spectroscopy (RPES) and angle-resolved photoelectron spectroscopy (ARPES) with soft X-ray synchrotron radiation. The partial $$mathrm{U}~5f$$ density of states of $$mathrm{UTe_2}$$ were imaged by the $$mathrm{U}~4d$$ - $$5f$$ RPES and it was found that the $$mathrm{U}~5f$$ state has an itinerant character, but there exists an incoherent peak due to the strong electron correlation effects. Furthermore, an anomalous admixture of the $$mathrm{U}~5f$$ states into the $$mathrm{Te}~5p$$ bands was observed at a higher binding energy, which cannot be explained by band structure calculations. On the other hand, the band structure of $$mathrm{UTe_2}$$ was obtained by ARPES and its overall band structure were mostly explained by band structure calculations. These results suggest that the $$mathrm{U}~5f$$ states of $$mathrm{UTe_2}$$ have itinerant but strongly-correlated nature with enhanced hybridization with the $$mathrm{Te}~5p$$ states.

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

https://doi.org/10.1103/PhysRevB.100.035204
 被引用回数：17 パーセンタイル：56.90(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

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

https://doi.org/10.1103/PhysRevB.100.035204

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.

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