2017年第64回応用物理学会春季学術講演会

講演情報

一般セッション(口頭講演)

10 スピントロニクス・マグネティクス » 10.4 半導体スピントロニクス・超伝導・強相関

[15a-501-1~10] 10.4 半導体スピントロニクス・超伝導・強相関

10.1と10.2と10.3と10.4のコードシェアセッションあり

2017年3月15日(水) 09:00 〜 12:00 501 (501)

岡林 潤(東大)、眞砂 卓史(福岡大)

09:30 〜 09:45

[15a-501-3] Increase of tunneling magnetoresistance in trilayer structures composed of group-IV ferromagnetic semiconductor Ge1-xFex, MgO, and Fe

瀧口 耕介1、若林 勇希1、岡本 浩平1、伴 芳祐1、田中 雅明1、大矢 忍1 (1.東大院工)

キーワード:ferromagnetic semiconductor, tunneling magnetoresistance

Group-IV ferromagnetic semiconductor (FMS) Ge1-xFex (GeFe) is a promising material for spin injectors and spin detectors for Si and Ge. GeFe can be epitaxially grown on Si and Ge substrates by low temperature molecular beam epitaxy (LT-MBE) and its conductivity can be controlled from metallic to insulating by boron (B) doping. Recently, tunneling magnetoresistance (TMR) has been observed in Fe/MgO/Ge0.935Fe0.065 magnetic tunnel junctions (MTJs) for the first time in MTJs with group-IV FMS, confirming the presence of spin-polarized carriers at the Fermi level in GeFe. However, the TMR ratio reported in the previous research was only 0.27%. Thus, it is necessary to improve TMR in Fe/MgO/GeFe. Here, we show that the TMR ratio is increased up to 1.5% by decreasing the size of the mesa diodes and by increasing the Fe concentration x of Ge1-xFex.
We have grown Fe / MgO (3 nm)/ Ge1-xFex (x = 6.5%, 10.5%, 14%, 17.5%) / Ge:B (B: 4 × 1019 cm-3) on p+ Ge (001) substrates by MBE. When x ≥ 10.5%, although the reflection high energy electron diffraction (RHEED) pattern of the MgO layer became broader with increasing x, the RHEED patterns of other layers were streaky. The observed RHEED patterns indicated that the MgO and Fe layers were epitaxially grown on Ge1-xFex with the epitaxial relationship of Fe[100](001) // MgO[110](001) // Ge1-xFex[100](001).
After the growth, an Al layer was deposited on the samples as a top electrode. We patterned mesa diodes with a diameter φ of 15, 60, and 150 μm using photolithography and Ar-ion etching. SiO2 was deposited for passivation. We observed the x dependence of the TMR ratio. Compared with the previous research, the TMR ratio was increased by changing the shape and size of the mesa diodes from a square with the size of 700×700 μm2 to the circle with φ = 60 μm when x = 6.5%. The TMR ratio became maximum at x = 10.5%, which is probably due to the enhancement of the ferromagnetic ordering in GeFe. The decrease in the TMR ratio at higher x can be attributed to the degradation of the crystallinity of the MgO layer by the increase in x.