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Thermal Conductivity Switching in Pd-Catalyzed Gd and GdH2 Films Upon Gasochromic Hydrogenation and Dehydrogenation
International Journal of Thermophysics ( IF 2.2 ) Pub Date : 2024-02-21 , DOI: 10.1007/s10765-023-03322-y
Riko Hirata , Yuichiro Yamashita , Takashi Yagi , Makoto Kashiwagi , Satoshi Takeya , Yuki Oguchi , Fabio Iesari , Toshihiro Okajima , Naoyuki Taketoshi , Yuzo Shigesato

Abstract

Thermal conductivity switching in Pd-catalyzed Gd hydride films was investigated using in situ analyses of electrical, optical, structural, and thermophysical properties upon gasochromic hydrogenation/dehydrogenation at room temperature. These reactions allow the films to reversibly switch between the metallic (GdH2) phase in the hydrogenated state and the semiconductor (GdH3) phase in the dehydrogenated state. We fabricated three-layered films comprising Pd (5 nm)/Gd or GdH2 (300 nm)/Mo (100 nm) using DC magnetron sputtering using Pd, Gd, and Mo targets, respectively, on unheated synthetic quartz substrates. Ar or mixture of Ar + H2 (H2: 5 % to 50 %) gases were used for the deposition of the Gd or GdH2 films, respectively. The thermal conductivities of the Gd or GdH2 films were analyzed using in situ rear-heating/rear-detection type time-domain picosecond pulsed light heating thermoreflectance measurements by employing a gas mixture of N2/Ar and H2 (H2: 3 %) at 1 atm, which is below the explosive limit for hydrogen. The thermal conductivities of Gd and GdH2 films were measured for one and two hydro-/dehydrogenation cycles, respectively. The thermal switching ratios of the ON state thermal conductivity to the OFF state thermal conductivity were 6.4 and 2.9–5.4 for the Gd film and the GdH2 (H2: 5 %–50 %) films, respectively. The thermal conductivity of the Gd hydrides films changed along with those estimated from the Wiedemann–Franz Law and electrical conductivities.



中文翻译:

Pd 催化 Gd 和 GdH2 薄膜在气致变色氢化和脱氢过程中的热导率转变

摘要

通过对室温气致变色氢化/脱氢时的电学、光学、结构和热物理性质进行原位分析,研究了 Pd 催化的氢化钆薄膜的热导率转换。这些反应使得薄膜能够在氢化状态的金属(GdH 2 )相和脱氢状态的半导体(GdH 3 )相之间可逆地转换。我们分别使用 Pd、Gd 和 Mo 靶材在未加热的合成石英基板上使用直流磁控溅射技术制备了包含 Pd (5 nm)/Gd 或 GdH 2 (300 nm)/Mo (100 nm)的三层薄膜。Ar或Ar+H 2 (H 2:5%至50%)气体的混合物分别用于沉积Gd或GdH 2膜。采用原位后加热/后检测型时域皮秒脉冲光加热热反射测量,采用 N 2 / Ar和 H 2 (H 2 : 3 %)在 1 个大气压下,低于氢气的爆炸极限。分别测量一次和两次加氢/脱氢循环的Gd和GdH 2膜的热导率。Gd薄膜和GdH 2 (H 2 : 5 %–50 %)薄膜的ON状态热导率与OFF状态热导率的热切换比分别为6.4和2.9-5.4。Gd 氢化物薄膜的热导率随着 Wiedemann-Franz 定律和电导率估计值的变化而变化。

更新日期:2024-02-21
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