TY - JOUR
T1 - Realization of efficient tuning of the Fermi level in iron-based ferrimagnetic alloys
AU - Yamashita, N.
AU - Shigematsu, E.
AU - Honda, S.
AU - Ohshima, R.
AU - Shiraishi, M.
AU - Ando, Y.
N1 - Funding Information:
N.Y. acknowledges support from the Japan Society of the Promotion of Science (JSPS) Research Fellow Program (Grant No. 20J22776). A part of this study was supported by a Grant-in-Aid for Scientific Research from the Ministry of Education, Culture, Sports, Science and Technology (MEXT) of Japan, Grant-in-Aid for Scientific Research (S) “Semiconductor Spincurrentronics” No. 16H06330, Grant-in-Aid for Scientific Research (B) 19H02197 and 20H02607, Grant-in-Aid for Scientific Research (A) 22H00214, and Grant-in-Aid for Research Activity Start-up 20K22413, and by Japan Science and Technology Agency (JST), JST-PRESTO ‘Information Carrier’, Grant No. JPMJPR20B2, by Adaptable and Seamless Technology transfer Program through Target-driven R&D (A-STEP) Grant No. JPMJTR20RN, and by Kansai Research foundation for Technology Promotion. N.Y. also acknowledges the JSPS Research Fellowship (DC1), Tateishi Science and Technology Foundation (Grant No. C2207007), and the WISE Program “Innovation of Advanced Photonic and Electronic Devices” at Kyoto University. A part of this work was supported by the Kyoto University Nano Technology Hub in “Nanotechnology Platform Project” sponsored by MEXT, Japan. A part of this work was conducted in Nagoya Institute of Technology, supported by Advanced Research Infrastructure for Materials and Nanotechnology (JPMXP1222NI1501) of the Ministry of Education, Culture, Sports, Science and Technology (MEXT), Japan. The authors are grateful to Dr. Yasuyuki Kondo for his fruitful discussion on the physics of the drastic change in the work function and Dr. Mitsuaki Kaneko for his fruitful advice on the measurements of the Schottky barrier height.
Publisher Copyright:
© 2022 American Physical Society.
PY - 2022/10
Y1 - 2022/10
N2 - The Stoner criterion allows only three single elements possessing room-temperature (RT) ferromagnetism: cobalt (Co), nickel (Ni), and iron (Fe). Although these three elements have played central roles in magnetism-based materials, their large work function (4.5∼5.2eV) is becoming a non-negligible obstacle for realization of spin devices using nonmetallic materials with finite energy gaps, because injection of electron spins into these nonmetallic materials is strongly hampered due to the large Schottky barrier height. Hence, a novel ferromagnetic or ferrimagnetic material simultaneously possessing RT ferromagnetism or ferrimagnetism and high Fermi energy is strongly required. Here, we show that an Fe-based alloy, iron-gadolinium (FeGd), allows circumvention of the obstacle. Surprisingly, only 20% of Gd incorporation in Fe dramatically modulates the Fermi energy from -4.8 to -3.0 eV, which is the largest modulation in all metallic alloys reported thus far. The coexistence of ferrimagnetism and nonzero spin polarization at RT of FeGd supports its abundant potential for future applications in low-carrier-density materials such as monolayer, organic, and nondegenerate inorganic semiconductors.
AB - The Stoner criterion allows only three single elements possessing room-temperature (RT) ferromagnetism: cobalt (Co), nickel (Ni), and iron (Fe). Although these three elements have played central roles in magnetism-based materials, their large work function (4.5∼5.2eV) is becoming a non-negligible obstacle for realization of spin devices using nonmetallic materials with finite energy gaps, because injection of electron spins into these nonmetallic materials is strongly hampered due to the large Schottky barrier height. Hence, a novel ferromagnetic or ferrimagnetic material simultaneously possessing RT ferromagnetism or ferrimagnetism and high Fermi energy is strongly required. Here, we show that an Fe-based alloy, iron-gadolinium (FeGd), allows circumvention of the obstacle. Surprisingly, only 20% of Gd incorporation in Fe dramatically modulates the Fermi energy from -4.8 to -3.0 eV, which is the largest modulation in all metallic alloys reported thus far. The coexistence of ferrimagnetism and nonzero spin polarization at RT of FeGd supports its abundant potential for future applications in low-carrier-density materials such as monolayer, organic, and nondegenerate inorganic semiconductors.
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U2 - 10.1103/PhysRevMaterials.6.104405
DO - 10.1103/PhysRevMaterials.6.104405
M3 - Article
AN - SCOPUS:85140246404
SN - 2475-9953
VL - 6
JO - Physical Review Materials
JF - Physical Review Materials
IS - 10
M1 - 104405
ER -