Ultrahigh Exchange Bias Field/Coercive Field Ratio in In Situ Formed Two-Dimensional Magnetic Te-Cr<sub>2</sub>O<sub>3</sub>/Cr<sub>5</sub>Te<sub>6</sub> Heterostructures.
basic_science · Level V
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- Record sourced from PubMed, PMID 39865984.
- Also identified by DOI 10.1002/adma.202410816.
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Abstract
The exchange bias (EB) effect is a fundamental magnetic phenomenon, in which the exchange bias field/coercive field ratio (|H<sub>EB</sub>/H<sub>C</sub>|) can improve the stability of spintronic devices. Two-dimensional (2D) magnetic heterostructures have the potential to construct low-power and high-density spintronic devices, while their typically air unstable and |H<sub>EB</sub>/H<sub>C</sub>| lesser, limiting the possibility of applications. Here, 2D Cr<sub>5</sub>Te<sub>6</sub> nanosheets have been systematically synthesized with an in situ formed ≈2 nm-thick Te doped Cr<sub>2</sub>O<sub>3</sub> layer (Te-Cr<sub>2</sub>O<sub>3</sub>) on the upper surface by chemical vapor deposition (CVD) method. The strong and air stable EB effect, achieving a |H<sub>EB</sub>/H<sub>C</sub>| of up to 80% under an ultralow cooling field of 0.01 T, which is greater than that of the reported 2D magnetic heterostructures. Meanwhile, the uniformity of thickness and chemical composition of the Te-Cr<sub>2</sub>O<sub>3</sub> layer can be controlled by the growth conditions which are highly correlated with the EB effect of 2D Te-Cr<sub>2</sub>O<sub>3</sub>/Cr<sub>5</sub>Te<sub>6</sub> heterostructures. First-principles calculations show that the Te-Cr<sub>2</sub>O<sub>3</sub> can provide uncompensated spins in the Cr<sub>2</sub>O<sub>3</sub>, thus forming strong spin pinning effect. The systematical investigation of the EB effect in 2D Te-Cr<sub>2</sub>O<sub>3</sub>/Cr<sub>5</sub>Te<sub>6</sub> heterostructures with high |H<sub>EB</sub>/H<sub>C</sub>| will open up exciting opportunities in low-power and high-stability 2D spintronic devices.