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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:3 パーセンタイル:37.82(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

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:46.34(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:0 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

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:38.96(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:16 パーセンタイル:62.18(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

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:19.88(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:13 パーセンタイル:40.50(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

Origin of robust nanoscale ferromagnetism in Fe-doped Ge revealed by angle-resolved photoemission spectroscopy and first-principles calculation

坂本 祥哉*; 若林 勇希*; 竹田 幸治; 藤森 伸一; 鈴木 博人*; 伴 芳祐*; 山上 浩志; 田中 雅明*; 大矢 忍*; 藤森 淳*

Physical Review B, 95(7), p.075203_1 - 075203_5, 2017/02

 被引用回数:9 パーセンタイル:40.80(Materials Science, Multidisciplinary)

Ge$$_{1-x}$$Fe$$_x$$ (Ge:Fe) shows ferromagnetic behavior up to a relatively high temperature of 210 K and hence is a promising material for spintronic applications compatible with Si technology. We have studied its underlying electronic structure by soft X-ray angle-resolved photoemission spectroscopy measurements and first-principles supercell calculation. We observed finite Fe 3$$d$$ components in the states at the Fermi level ($$Erm_F$$) in a wide region of momentum space, and the $$Erm_F$$ was located $$sim$$0.35 eV above the valence-band maximum of the host Ge. Our calculation indicates that the $$Erm_F$$ is also within the deep acceptor-level impurity band induced by the strong $$p$$-$$d$$($$t_2$$) hybridization. We conclude that the additional minority-spin $$d(e)$$ electron characteristic of the Fe$$^{2+}$$ state is responsible for the short-range ferromagnetic coupling between Fe atoms.

論文

Origin of the large positive magnetoresistance of Ge$$_{1-x}$$Mn$$_{x}$$ granular thin films

若林 勇希*; 秋山 了太*; 竹田 幸治; 堀尾 眞史*; 芝田 悟朗*; 坂本 祥哉*; 伴 芳祐*; 斎藤 祐児; 山上 浩志; 藤森 淳*; et al.

Physical Review B, 95(1), p.014417_1 - 014417_6, 2017/01

 被引用回数:11 パーセンタイル:46.65(Materials Science, Multidisciplinary)

Ge$$_{1_x}$$Mn$$_x$$ (GeMn) granular thin films are a unique and promising material for spintronic applications owing to their large positive magnetoresistance (MR). The microscopic origin of the MR has not yet been clarified. Here, we develop a method to separately investigate the magnetic properties of the nanoparticles and the matrix, utilizing the extremely high sensitivity of X-ray magnetic circular dichroism (XMCD) to the local magnetic state of each atom. We find that the MR ratio is proportional to the product of the magnetizations originating from the nanoparticles and the matrix. This result indicates that the spin-polarized holes in the nanoparticles penetrate into the matrix and that these holes undergo first order magnetic scattering by the paramagnetic Mn atoms in the matrix, which induces the large MR.

論文

Volume-wise destruction of the antiferromagnetic Mott insulating state through quantum tuning

Frandsen, B. A.*; Liu, L.*; Cheung, S. C.*; Guguchia, Z.*; Khasanov, R.*; Morenzoni, E.*; Munsie, T. J. S.*; Hallas, A. M.*; Wilson, M. N.*; Cai, Y.*; et al.

Nature Communications (Internet), 7, p.12519_1 - 12519_8, 2016/08

 被引用回数:34 パーセンタイル:76.48(Multidisciplinary Sciences)

RENiO$$_3$$ (RE = rare-earth element) and V$$_2$$O$$_3$$ are archetypal Mott insulator systems. When tuned by chemical substitution (RENiO$$_3$$) or pressure (V$$_2$$O$$_3$$), they exhibit a quantum phase transition (QPT) between an antiferromagnetic Mott insulating state and a paramagnetic metallic state. Because novel physics often appears near a Mott QPT, the details of this transition, such as whether it is first or second order, are important. Here, we demonstrate through muon spin relaxation/rotation experiments that the QPT in RENiO$$_3$$ and V$$_2$$O$$_3$$ is first order: the magnetically ordered volume fraction decreases to zero at the QPT, resulting in a broad region of intrinsic phase separation, while the ordered magnetic moment retains its full value until it is suddenly destroyed at the QPT. These findings bring to light a surprising universality of the pressure-driven Mott transition, revealing the importance of phase separation and calling for further investigation into the nature of quantum fluctuations underlying the transition.

論文

Room-temperature local ferromagnetism and its nanoscale expansion in the ferromagnetic semiconductor Ge$$_{1-x}$$Fe$$_{x}$$

若林 勇希*; 坂本 祥哉*; 竹田 幸治; 石上 啓介*; 高橋 文雄*; 斎藤 祐児; 山上 浩志; 藤森 淳*; 田中 雅明*; 大矢 忍*

Scientific Reports (Internet), 6, p.23295_1 - 23295_9, 2016/03

AA2016-0503.pdf:1.66MB

 被引用回数:20 パーセンタイル:64.49(Multidisciplinary Sciences)

We investigate the local electronic structure and magnetic properties of the group-IV-based ferromagnetic semiconductor, Ge$$_{1-x}$$Fe$$_{x}$$ (GeFe), using soft X-ray magnetic circular dichroism. Our results show that the doped Fe 3$$d$$ electrons are strongly hybridized with the Ge 4$$p$$ states, and have a large orbital magnetic moment relative to the spin magnetic moment, namely $$m_{rm orb}$$/$$m_{rm spin}$$ $$approx$$ 0.1. We find that nanoscale local ferromagnetic regions, which are formed through ferromagnetic exchange interactions in the high-Fe-content regions of the GeFe films, exist even at room temperature, well above the Curie temperature of 20 - 100K. We observe the intriguing nanoscale expansion of the local ferromagnetic regions with decreasing temperature, followed by a transition of the entire film into a ferromagnetic state at the Curie temperature.

論文

Magnetization process of the $$n$$-type ferromagnetic semiconductor (In,Fe)As:Be studied by X-ray magnetic circular dichroism

坂本 祥哉*; Anh, L. D.*; Hai, P. N.*; 芝田 悟朗*; 竹田 幸治; 小林 正起*; 高橋 文雄*; 小出 常晴*; 田中 雅明*; 藤森 淳*

Physical Review B, 93(3), p.035203_1 - 035203_6, 2016/01

AA2016-0502.pdf:1.1MB

 被引用回数:19 パーセンタイル:62.92(Materials Science, Multidisciplinary)

In order to investigate the mechanism of ferromagnetic ordering in the new $$n$$-type magnetic semiconductor (In,Fe)As codoped with Be, we have performed X-ray absorption spectroscopy and X-ray magnetic circular dichroism (XMCD) studies. The spectral line shapes suggest that the ferromagnetism is intrinsic, originating from Fe atoms incorporated into the zinc-blende-type InAs lattice. The magnetization curves of Fe measured by XMCD were well reproduced by the superposition of a Langevin function representing superparamagnetic (SPM) behavior of nanoscale ferromagnetic domains and a $$T$$-linear function representing Curie-Weiss paramagnetism even much above the Curie temperatures. The data at 20 K showed a deviation from the Langevin behavior, suggesting a gradual establishment of macroscopic ferromagnetism on lowering temperature. The existence of nanoscale ferromagnetic domains indicated by the SPM behavior suggests spatial fluctuations of Fe concentration on the nanoscale.

論文

Spin and orbital magnetic moments of Fe in the $$n$$-type ferromagnetic semiconductor (In,Fe)As

小林 正起*; Anh, L. D.*; Hai, P. N.*; 竹田 幸治; 坂本 祥哉*; 門野 利治*; 岡根 哲夫; 斎藤 祐児; 山上 浩志; 原田 慈久*; et al.

Applied Physics Letters, 105(3), p.032403_1 - 032403_4, 2014/07

AA2015-0418.pdf:0.82MB

 被引用回数:6 パーセンタイル:25.97(Physics, Applied)

The electronic and magnetic properties of Fe atoms in the ferromagnetic semiconductor (In,Fe)As codoped with Be have been studied by X-ray absorption spectroscopy (XAS) and X-ray magnetic circular dichroism (XMCD) at the Fe $$L_{2,3}$$ edge. The XAS and XMCD spectra showed simple spectral line shapes similar to Fe metal, but the ratio of the orbital and spin magnetic moments estimated using the XMCD sum rules was significantly larger than that of Fe metal, indicating a significant orbital moment of Fe 3$$d$$ electrons in (In,Fe)As:Be. The XMCD intensity as a function of magnetic field indicated hysteretic behavior of the superparamagnetic-like component due to discrete ferromagnetic domains. VC

報告書

不要RFの抑制によるジャイロトロンの高性能化

春日井 敦; 坂本 慶司; 林 健一*; 高橋 幸司; 庄山 裕章*; 梶原 健*; 池田 佳隆; 假家 強*; 満仲 義加*; 藤井 常幸; et al.

JAERI-Research 2002-027, 57 Pages, 2002/11

JAERI-Research-2002-027.pdf:3.6MB

ジャイロトロン内に発生する不要RFは、ジャイロトロンの長パルス化あるいは高効率化等の性能向上を妨げている要因の1つである。ジャイロトロンの内部に発生する不要RFには、(1)ビームトンネルにおける寄生発振,(2)放射器における寄生発振,(3)ジャイロトロン内部の散乱RFがある。ビームトンネルにおける寄生発振は、ビームトンネルの表面に炭化珪素材を適用することで完全に抑制することができた。その結果、ジャイロトロンの空胴共振器における主モードの発振効率を従来の約20%から30%以上に改善でき、高効率動作の実現を達成した。放射器の寄生発振については、空胴共振器での発振効率を高めることで軽減できることを明らかにした。ジャイロトロン内部の高周波回路の回折損失に起因する散乱RFはジャイロトロン出力の10%以上あることが明らかとなったが、冷却の工夫及びDCブレークの材質の変更により、動作を制限する要因にはなっていない。以上のように、寄生発振を抑制したこと及び散乱RFを管外で処理し、散乱RFに起因する内部加熱に対する冷却の強化により1MW-10秒レベル(0.9MW-9.2秒)の長パルス動作が可能となった。

論文

Development and design of an ECRF launching system for ITER

高橋 幸司; 今井 剛; 坂本 慶司; 小林 則幸*; 森 清治*; 毛利 憲介*; 伊藤 保之*; 庄山 裕章; 春日井 敦

Fusion Engineering and Design, 56-57, p.587 - 592, 2001/10

 被引用回数:7 パーセンタイル:48.43(Nuclear Science & Technology)

国際熱核融合実験炉(ITER)では、プラズマ加熱電流駆動,分布制御,プラズマ立ち上げ等のツールとして電子サイクロトロン波帯加熱(ECRF)装置が必要とされている。水平ポートから中心及び周辺の加熱電流駆動を目的として、上斜めポートからは分布制御を目的として、前者はトロイダル入射角20~45度,後者はポロイダル入射角度50~58度の可変性能を有する入射系(ランチャー)が要求されている。何れも周波数は170GHz,総入射パワー20MWである。原研ではITER設計タスクのもと、先端ミラーによってに入射角度可変とするランチャーを基本に設計を行っている。その設計及びそれに必要な耐中性子可動ミラー用摺動部やダイヤモンド窓の開発、さらに先端から離れた位置に可動ミラーを設置し、そのミラーにより入射角度を変える遠隔駆動型ランチャーの開発を行っている。その成果について報告する。

論文

High-efficiency oscillation of 170GHz high-power gyrotron at TE$$_{31.8}$$ mode with depressed collector

庄山 裕章; 坂本 慶司; 林 健一*; 春日井 敦; 恒岡 まさき; 高橋 幸司; 池田 幸治; 假家 強*; 満仲 義加*; 今井 剛

Japanese Journal of Applied Physics, Part 2, 40(8B), p.L906 - L908, 2001/08

 被引用回数:28 パーセンタイル:71.63(Physics, Applied)

170GHz大電力ジャイロトロンを用いて安定な1.1MWの発振を達成した。発振モードはTE$$_{31.8}$$であり、CW運転可能なモードである。発振効率は32%であり、減速コレクター運転により総合効率として57%に達した。発振効率を低下させるビームトンネル(電子銃とキャビティの間の電子ビームが通過する筒)での寄生発振をRF吸収体を装備することにより抑制した。この結果は核融合装置に求められる1MW長パルスジャイロトロンの開発に大きなインパクトを与えるものである。

論文

1 MW and long pulse operation of Gaussian beam output gyrotron with CVD diamond window for fusion devices

春日井 敦; 坂本 慶司; 高橋 幸司; 梶原 健; 庄山 裕章; 池田 幸治; 恒岡 まさき; 池田 佳隆; 藤井 常幸; 假家 強*; et al.

Fusion Engineering and Design, 53(1-4), p.399 - 406, 2001/01

 被引用回数:17 パーセンタイル:74.43(Nuclear Science & Technology)

原研ではITER R&Dのもとで、ITER用170GHzジャイロトロンの開発を行っている。これまでに、ダイヤモンド窓の開発などにより、世界のトップデータとなる出力約0.5MWで8秒間の出力を達成した。次のステップとしてジャイロトロンのビームトンネルを改良し、発振効率を28%まで改善させた。さらに、1MW-10秒を目標とした次期170GHzジャイロトロンを製作し、現在発振実験を行っている。また170GHzジャイロトロンの開発をベースに、JT-60Uでの電子サイクロトロン加熱/電流駆動のための、周波数110GHz、ダイヤモンド窓搭載ガウシアンビーム出力ジャイロトロンを製作し、プラズマへの応用を開始した。これまでに出力1MWで0.6秒の発振が得られている。

論文

大電力100GHz帯ジャイロトロンの開発

庄山 裕章; 坂本 慶司; 林 健一*; 春日井 敦; 高橋 幸司; 恒岡 まさき; 池田 幸治; 假家 強*; 満仲 義加*; 今井 剛

信学技報, 100(506), p.39 - 44, 2000/12

ITER,JT-60U等の大型核融合装置における電子サイクロトロン共鳴加熱及び電流駆動装置の発振源として大電力、長パルス、高効率の100GHz帯ジャイロトロンの開発を行い、これまでにエネルギー回収運動による効率50%発振、超高次モードを用いた1MW発振、数MW/連続出力で使用可能な人工ダイヤモンド出力窓の開発等の成果を得てきた。最近では、長パルス化に向けてさらなる発振効率の向上を図るために、SiCビームトンネル付170GHzジャイロトロンを開発し、1.1MW/57%の発振を達成した。

論文

ECH用大電力ジャイロトロンの開発

今井 剛; 坂本 慶司; 春日井 敦; 恒岡 まさき; 高橋 幸司; 庄山 裕章; 池田 幸治; 池田 佳隆; 梶原 健; 藤井 常幸; et al.

平成12年度電気学会原子力研究資料(NE-00-4), p.19 - 24, 2000/09

原研が、ITER及びJT-60U用に開発しているミリ波(100-200GHz帯)の大電力、長パルス、高効率ジャイロトロンの開発成果について報告する。人工ダイヤモンド窓により、大電力、長パルスが可能となり、また、エネルギー回収により、高効率が可能となった。これらの技術を最適化して、170GHz、1MWで50%の発振を達成し、また、長パルスでは、110GHzで、1MW,3秒,170GHzでは、約500kWで8秒の出力を得ている。

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