検索対象:     
報告書番号:
※ 半角英数字
 年 ~ 
 年
検索結果: 9 件中 1件目~9件目を表示
  • 1

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 ...

使用言語

Initialising ...

発行年

Initialising ...

開催年

Initialising ...

選択した検索結果をダウンロード

口頭

Anisotropy and magnetic entropy of UTe$$_{2}$$

Opletal, P.; 酒井 宏典; 芳賀 芳範; 山本 悦嗣; 神戸 振作; 徳永 陽; 常盤 欣文

no journal, , 

Recently rediscovered orthorhombic UTe$$_{2}$$ exhibits superconductivity at low temperatures below 2 K. The origin of superconductivity is still unknown even though its properties were investigated by different techniques and reported in literature. The origin of superconductivity could be found by investigating physical properties at temperatures above superconductivity. Existence of ferromagnetic fluctuations along the $$a$$-axis was suggested based on thermodynamic and transport measurements while antiferromagnetic fluctuations were found by inelastic neutron scattering along the $$b$$-axis. We investigate magnetic properties for all crystallographic axes in fields up to 7 T and temperature interval from 2 K up to 60 K. The obtained data are than evaluated by Maxwell relations between entropy and magnetization to obtain change of magnetic part of entropy in T-H diagram. The entropy for field along the $$a$$-axis show ferromagnetic behavior with unusual behavior below ~ 7 K, while for field along the $$b$$-axis we observe antiferromagnetic-like behavior. We discuss our results with consideration of results in literature and propose possible scenarios. The results obtained on superconducting sample are compared to non-superconducting

口頭

Magnetic entropy of UTe$$_{2}$$

Opletal, P.; 酒井 宏典; 芳賀 芳範; 山本 悦嗣; 神戸 振作; 徳永 陽; 常盤 欣文

no journal, , 

Recently rediscovered orthorhombic UTe$$_{2}$$ exhibits superconductivity at low temperatures below 2 K. The origin of superconductivity is still unknown even though its properties were investigated by different techniques and reported in literature. The origin of superconductivity could be found by investigating physical properties at temperatures above superconductivity. Existence of ferromagnetic fluctuations along the $$a$$-axis was suggested based on thermodynamic and transport measurements while antiferromagnetic fluctuations were found by inelastic neutron scattering along the $$b$$-axis. We investigate magnetic properties for all crystallographic axes in fields up to 7 T and temperature interval from 2 K up to 60 K. The obtained data are than evaluated by Maxwell relations between entropy and magnetization to obtain change of magnetic part of entropy in T-H diagram. The entropy for field along the $$a$$-axis show ferromagnetic behavior with unusual behavior below ~ 7 K, while for field along the $$b$$-axis we observe antiferromagnetic-like behavior. We discuss our results with consideration of results in literature and propose possible scenarios. The results obtained on superconducting sample are compared to non-superconducting

口頭

UTe$$_2$$の格子欠陥が物性に及ぼす影響

芳賀 芳範; Opletal, P.; 常盤 欣文; 山本 悦嗣; 徳永 陽; 神戸 振作; 酒井 宏典

no journal, , 

超伝導体UTe$$_2$$の単結晶を化学気相成長法により育成し、育成条件の違いが及ぼす影響を調べた。超伝導を示さない試料(NS)ではウランサイトの占有率が有意に減少していることを、EPMA組成分析及び単結晶X線構造解析により示した。欠損の影響は常伝導状態の電子比熱にも大きく影響を及ぼしており、これが超伝導の有無と関係している可能性がある。

口頭

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*

no journal, , 

The electronic structure of UTe$$_2$$ was studied by resonant photoelectron spectroscopy (RPES) and angle-resolved photoelectron spectroscopy (ARPES) with soft X-ray synchrotron radiation. The partial U 5f density of states of UTe$$_2$$ were imaged by the U~$$4d$$-$$5f$$ RPES and it was found that the U~$$5f$$ state has an itinerant character, but there exists an incoherent peak due to the strong electron correlation effects. The band structure of UTe$$_2$$ was obtained by ARPES and its overall band structure was mostly explained by band structure calculations, except for the incoherent band at $$E_B=0.5$$ eV. These results suggest that the U~$$5f$$ states of UTe$$_2$$ have itinerant but strongly-correlated nature with enhanced hybridization with the Te~$$5p$$ states. In addition, the valence state of UTe$$_2$$ was studied by core-level photoelectron spectroscopy. The main peak position of the U~$$4f$$ core-level spectrum of UTe$$_2$$ coincides with that of UB$$_2$$, which is an itinerant compound with a nearly $$5f^3$$ configuration. However, the main peak of UTe$$_2$$ is broader than that of 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 U~$$5f$$ state in UTe$$_2$$ is in a mixed valence state with a dominant contribution from the itinerant 5$$f^3$$ configuration.

口頭

UTe$$_2$$の高純度単結晶における上部臨界磁場

芳賀 芳範; 酒井 宏典; Opletal, P.; 常盤 欣文; 山本 悦嗣; 神戸 振作; 徳永 陽; 木俣 基*; 中村 慎太郎*; 淡路 智*; et al.

no journal, , 

特異な超伝導体UTe$$_{2}$$が国内外で大きな注目を集め、盛んに研究されているが既存試料は純度が低くその詳細は不明であった。本研究では、従来より飛躍的に純良な単結晶を用いて測定した上部臨界磁場の特徴を報告する。

口頭

Single crystal growth and $$H$$-$$T$$ phase diagram of spin-triplet superconducting UTe$$_2$$

酒井 宏典

no journal, , 

スピン三重項超伝導体として注目されているUTe$$_2$$における新しい単結晶育成法を考案し、その条件最適化をおこなった結果、超伝導転移温度の向上に加えて、残留抵抗率比の大幅な改善がみられた。こうして得られた純良単結晶を用いて、電気抵抗率と交流帯磁率の同時測定を行なって強磁場25Tまでの磁場($$H$$)-温度($$T$$)相図の決定を行った。

口頭

重い電子系超伝導体UTe$$_2$$高純度単結晶の強磁場磁気抵抗

芳賀 芳範; 酒井 宏典; 常盤 欣文; Opletal, P.; 木俣 基*; 中村 慎太郎*; 淡路 智*; 佐々木 孝彦*; 青木 大*; 神戸 振作; et al.

no journal, , 

重い電子系UTe$$_2$$の高純度単結晶について強磁場磁気抵抗測定を行った。強磁場領域でシュブニコフ・ドハース振動が観測され、$$H||c$$でのフェルミ面極値断面積及び有効質量を決定し、$$c$$軸方向にのびた2次元フェルミ面を観測した。また、フェルミ面に起因する横磁気抵抗が観測され、キャリアの易動度に関する情報が得られ、重い電子の挙動に関する新たな情報が得られた。

口頭

Electronic structure of UTe$$_2$$; A Perspective from 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*

no journal, , 

The unconventional superconductors in $$f$$-based materials attract much attention in recent years. Recently, it was discovered that UTe$$_2$$ has relatively high transition temperature, and it is classified into one of such class of materials. In the present study, the electronic structure of UTe$$_2$$ was studied by resonant photoelectron spectroscopy (RPES) and angle-resolved photoelectron spectroscopy (ARPES) with soft X-ray synchrotron radiation. The partial U 5$$f$$ density of states of UTe$$_2$$ were imaged by the U 4$$d$$-5$$f$$ RPES and it was found that the U 5$$f$$ state has an itinerant character, but there exists an incoherent peak due to the strong electron correlation effects. The band structure of UTe$$_2$$ was obtained by ARPES and its overall band structure was mostly explained by band structure calculations, except for the incoherent band at $$E_B sim 0.5$$ eV. These results suggest that the U 5$$f$$ states of UTe$$_2$$ have itinerant but strongly-correlated nature with enhanced hybridization with the Te 5$$p$$ states. The new ARPES data of the detailed electronic structure of Z point will be presented.

口頭

Electronic structure of UTe$$_2$$; A Perspective from photoelectron spectroscopy

藤森 伸一

no journal, , 

The unconventional superconductors in $$f$$-based materials attract much attention in recent years. Recently, it was discovered that UTe$$_2$$ has relatively high transition temperature ($$T_{mathrm{SC}}$$=1.65 K), and it is classified into one of such class of materials. In the present study, the electronic structure of UTe$$_2$$ was studied by resonant photoelectron spectroscopy (RPES) and angle-resolved photoelectron spectroscopy (ARPES) with soft X-ray synchrotron radiation. The partial U 5$$f$$ density of states of UTe2 were imaged by the U 4$$d$$-5$$f$$ RPES and it was found that the U 5$$f$$ state has an itinerant character, but there exists an incoherent peak due to the strong electron correlation effects. The band structure of UTe$$_2$$ was obtained by ARPES and its overall band structure was mostly explained by band structure calculations, except for the incoherent band at $$E_{mathrm{B}} sim$$ 0.5 eV. These results suggest that the U 5$$f$$ states of UTe$$_2$$ have itinerant but strongly-correlated nature with enhanced hybridization with the Te 5$$p$$ states.

9 件中 1件目~9件目を表示
  • 1