TY - JOUR
T1 - Engineering large perpendicular magnetic anisotropy in amorphous ferrimagnetic gadolinium cobalt alloys
AU - Srinivasan, Karthik
AU - Chen, Yulan
AU - Cestarollo, Ludovico
AU - Dare, Darrah K.
AU - Wright, John G.
AU - El-Ghazaly, Amal
N1 - Publisher Copyright:
© 2023 The Royal Society of Chemistry.
PY - 2023/3/20
Y1 - 2023/3/20
N2 - Amorphous magnetic alloys with large perpendicular magnetic anisotropy (PMA) have emerged as a suitable material choice for spintronic memory and high-frequency non-reciprocal devices on-chip. Unlike ferromagnets, ferrimagnets offer faster switching dynamics, lower net saturation magnetization, minimal stray field and a lower net angular momentum. Ferrimagnetic thin films of GdxCo1−x sputter deposited as heterostructures of Ta/Pt/GdxCo1−x(t)/Pt on Si/SiO2 have bulk-like PMA for thicknesses of 5-12 nm and room-temperature magnetic compensation for x = 28-32%. Preferential oxygenation of GdCo has been found to increase the effective anisotropy energy density by an order of magnitude and produce near-ideal remanence ratios. X-ray photoelectron spectroscopy accurately quantifies the metal-oxidation ratio, which shows that an oxygen-rich and Co-deficient stoichiometry (Gd21Co28O51) likely weakens the ferromagnetic exchange interaction between Co-Co and contributes additional antiferromagnetic exchange through superexchange-like interactions between Gd and Co via O, resulting in a stronger out-of-plane magnetization. Even greater PMA and giant-anisotropy field of 11 kOe are achieved in super-lattices of the Gd21Co28O51 heterostructure. The combination of ferrimagnetic ordering in amorphous GdxCo1−x and its affordance of pathways for engineering large PMA will enable the design of integrated high-frequency devices beyond 30 GHz and ultrafast energy efficient memory devices with switching speeds down to tens of picoseconds.
AB - Amorphous magnetic alloys with large perpendicular magnetic anisotropy (PMA) have emerged as a suitable material choice for spintronic memory and high-frequency non-reciprocal devices on-chip. Unlike ferromagnets, ferrimagnets offer faster switching dynamics, lower net saturation magnetization, minimal stray field and a lower net angular momentum. Ferrimagnetic thin films of GdxCo1−x sputter deposited as heterostructures of Ta/Pt/GdxCo1−x(t)/Pt on Si/SiO2 have bulk-like PMA for thicknesses of 5-12 nm and room-temperature magnetic compensation for x = 28-32%. Preferential oxygenation of GdCo has been found to increase the effective anisotropy energy density by an order of magnitude and produce near-ideal remanence ratios. X-ray photoelectron spectroscopy accurately quantifies the metal-oxidation ratio, which shows that an oxygen-rich and Co-deficient stoichiometry (Gd21Co28O51) likely weakens the ferromagnetic exchange interaction between Co-Co and contributes additional antiferromagnetic exchange through superexchange-like interactions between Gd and Co via O, resulting in a stronger out-of-plane magnetization. Even greater PMA and giant-anisotropy field of 11 kOe are achieved in super-lattices of the Gd21Co28O51 heterostructure. The combination of ferrimagnetic ordering in amorphous GdxCo1−x and its affordance of pathways for engineering large PMA will enable the design of integrated high-frequency devices beyond 30 GHz and ultrafast energy efficient memory devices with switching speeds down to tens of picoseconds.
UR - http://www.scopus.com/inward/record.url?scp=85151814585&partnerID=8YFLogxK
U2 - 10.1039/d3tc00332a
DO - 10.1039/d3tc00332a
M3 - Article
AN - SCOPUS:85151814585
VL - 11
SP - 4820
EP - 4829
JO - Journal of Materials Chemistry C
JF - Journal of Materials Chemistry C
IS - 14
ER -