わずか50℃が、平坦か崩壊かを分ける ― L10-FePd膜を蝕む”膜の崩壊”を、二段階焼成の最初の一手で封じ込める ―

2026-08-04 富山大学

富山大学を中心とする国際共同研究グループは、次世代不揮発性磁気メモリ(MRAM)の記録層として有望なL1₀-FePd規則合金薄膜について、膜厚5 nmという極薄領域で高い規則化と原子レベルの平坦性を両立する二段階焼成法を確立した。研究では、1回目の焼成温度がわずか50℃異なるだけで、その後600℃で再加熱しても覆らないほど膜の品質が決定されることを発見した。低温焼成時に生じる微小な穴が、薄膜が島状に分裂するデウェッティング(膜の崩壊)の引き金となることを、原子分解能電子顕微鏡観察と第一原理計算による表面自由エネルギー解析で解明した。最適条件では、規則度0.99、垂直磁気異方性1.33 MJ/m³を達成し、極薄膜でも高い磁気特性を維持できることを実証した。本成果は、MRAMのさらなる高密度化・低消費電力化を可能にするほか、高性能スピントロニクスデバイスの実用化を加速する材料・プロセス設計指針となる。

わずか50℃が、平坦か崩壊かを分ける ― L10-FePd膜を蝕む”膜の崩壊”を、二段階焼成の最初の一手で封じ込める ―
図1 二段階焼成法によるL1₀-FePd極薄膜の「平坦性」と「規則化」の両立と、Dewettingの抑制

<関連情報>

2段階加熱と固体脱湿を利用した高秩序L10 – FePd合金エピタキシャル膜 Harnessing two-step heating and solid-state dewetting for highly ordered L10-FePd alloy epitaxial films

Samuel Vergara, Shingo Maruyama, Soki Yoshida, Hanuma Kumar Dara, Keisuke Haruki, Naohiro Matsumoto, Mitsuharu Uemoto, Tomoya Ono, Shintaro Yasui, Yasushi Endo, Amit Kohn, Masaki Mizuguchi, Tomoyuki Ogawa, Hiroshi Naganuma
Journal of Alloys and Compounds  Available online: 26 July 2026
DOI:https://doi.org/10.1016/j.jallcom.2026.189751

Highlights

  • Two-step heating enables morphology control unreachable by one-step heating.
  • 50 K Ts shift switches FM, SSD, and SK/late-stage SSD growth regimes.
  • FM at 150°C yields flat L10-FePd with strong PMA and high Mr/Ms.
  • SSD at 200–250°C achieves SL10 = 0.99 and PMA = 1.33 MJ/m3.
  • Results enable ultra-thin L10-FePd films for next-generation MRAM.

Abstract

L10-ordered FePd epitaxial films with a nominal thickness of 5 nm were grown by r.f. magnetron sputtering on the SrTiO3 (001) single crystal substrates by a two-step heating method. A subtle 50 K change in the first-heating temperature of a two-step process drastically alters the morphological trajectory of L10-FePd films, switching among three regimes: (i) Frank–van der Merwe (FM — atomically flat), (ii) Solid-state dewetting (SSD — square holes), and (iii) Stranski-Krastanov or late-stage SSD (SK or SSD late stage — 3D grains). (i) [FM mode] Almost no lattice disturbance in the in-plane direction, and perfect constraint by tensile strain from the SrTiO3 substrate was achieved. (ii) [SSD mode] Square holes penetrating to the SrTiO3 substrate were formed, and sides of the square were grown along the < 100 > or < 010 > of the SrTiO3 substrate. According to first-principles calculations, a large difference in surface free energy between L10-FePd and the SrTiO3 substrate is predicted. This difference in surface free energy is the minimum necessary condition for SSD to occur. The trigger for SSD is small holes/voids formed during the 1st heating process in the two-step heating process. (iii) [SK or late-stage SSD mode] Grains grew 3-dimensionally, which can be considered as SK growth mode or the late stages of SSD. Note that the 1st heating temperature of the two-step heating process significantly changed the morphological trajectory, even though the 2nd heating temperature of 600°C was significantly higher than that of the 1st growth temperature. The SSD reduced the substrate restraint, resulting in the highest degree of L10-ordering (SL10 = 0.99) and the highest perpendicular magnetic anisotropy (PMA = 1.33MJ/m3).

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