A conductive epitaxial underlayer for voltage control in magnetic garnet heterostructures

R Ryan T. Huynh (Department of Materials Science and Engineering, Massachusetts Institute of Technology 1 , Cambridge, Massachusetts 02139,) P Paul Fourmont (Department of Materials Science and Engineering, Massachusetts Institute of Technology 1 , Cambridge, Massachusetts 02139,) H Hyeon-Su Shin (Department of Materials Science and Engineering, Korea National University of Transportation 3 , Chungju 27469,) S Sylvain G. Cloutier (Department of Electrical Engineering, École de Technologie Supérieure 2 , 1100 Notre Dame Street West, Montreal, Quebec H3C 1K3,) Y Young-Min Kang (Department of Materials Science and Engineering, Massachusetts Institute of Technology 1 , Cambridge, Massachusetts 02139,) C Caroline A. Ross

Abstract

Magnetic iron garnets hold great interest for magnonic, spintronic, and magnetooptical devices, but utilizing voltage-driven phenomena in insulating garnets has been prevented by the lack of a conductive epitaxial garnet underlayer. Beyond providing sufficient electrical conduction, the underlayer should exhibit low saturation magnetization to minimize magnetic interaction with the magnetic layers of the heterostructure, while maintaining high crystalline quality to enable epitaxial growth. Here, defect engineering via site-selective doping is employed to enhance the electrical conductivity of Y3Fe5O12 (YIG) while suppressing its magnetization. Epitaxial Fe-deficient Ca-doped YIG (Y2.7Ca0.3Fe4.7O12-δ, CaYIG) films, where Ca2+ substitutes Y3+ in the dodecahedral sites, exhibit electrical resistivities of 5.8 × 103 Ω cm and above and show saturation magnetization of 145 kA/m comparable to that of YIG, with perpendicular magnetic anisotropy or an in-plane easy axis depending on the substrate. Substitution of Al3+ into tetrahedral Fe3+ sites in Ca0.3Y2.7Fe3.5Al1O12-δ (CaAlYIG) reduces the saturation magnetization to below 25 kA/m and increases the resistivity to 1.65 × 104 Ω cm or higher. The functionality of CaAlYIG was demonstrated in a heterostructure of Bi1.2Y1.8Fe5O12 (BiYIG)/CaAlYIG/Gd3Sc2Ga3O12, where the CaAlYIG layer enables a voltage to be applied through the thickness of the BiYIG layer.

Article Details

Volume / Issue Vol. 128, Issue 21
Published May 25, 2026
ISSN 0003-6951
Publisher American Institute of Physics

Journal Info

Applied Physics Letters

American Institute of Physics

ISSN: 0003-6951 Physical Sciences

Authors (6)

R

Ryan T. Huynh

Department of Materials Science and Engineering, Massachusetts Institute of Technology 1 , Cambridge, Massachusetts 02139,

P

Paul Fourmont

Department of Materials Science and Engineering, Massachusetts Institute of Technology 1 , Cambridge, Massachusetts 02139,

H

Hyeon-Su Shin

Department of Materials Science and Engineering, Korea National University of Transportation 3 , Chungju 27469,

S

Sylvain G. Cloutier

Department of Electrical Engineering, École de Technologie Supérieure 2 , 1100 Notre Dame Street West, Montreal, Quebec H3C 1K3,

Y

Young-Min Kang

Department of Materials Science and Engineering, Massachusetts Institute of Technology 1 , Cambridge, Massachusetts 02139,

C

Caroline A. Ross