Dec 4, 2024
8:00pm - 10:00pm
Hynes, Level 1, Hall A
Yufan Feng1,Qi Song1,Ludi Miao1,Xiaoxi Huang1,Evan Krysko1,Christopher Parzyck1,Daniel C Ralph1,2,Kyle Shen1,2,Darrell Schlom1
Cornell University1,Kavli Institute at Cornell for Nanoscale Science2
Yufan Feng1,Qi Song1,Ludi Miao1,Xiaoxi Huang1,Evan Krysko1,Christopher Parzyck1,Daniel C Ralph1,2,Kyle Shen1,2,Darrell Schlom1
Cornell University1,Kavli Institute at Cornell for Nanoscale Science2
PdCoO
2 with a delafossite structure has emerged as a prominent material in condensed matter physics and materials science, prized for its high conductivity. Another delafossite material, PdCrO
2, presents a metallic nature but shows antiferromagnetic (AFM) order at low temperature. Compared to PdCoO
2, PdCrO
2 has unpaired electrons in the CrO
2 layer. We are investigating the effect of unpaired electrons on the magnetic properties of these metallic delafossite materials by creating epitaxial films with solid solutions of a transition metal with no unpaired electrons (Co
3+) with transition metals with unpaired electrons (Fe
3+ and Cr
3+), i.e., PdFe
xCo
1–xO
2, PdCr
xCo
1–xO
2, enabling the concentration of unpaired electrons to be continuously varied. Molecular beam epitaxy (MBE) is employed to precisely control the thin film growth of these solid solutions.
Our PdCrO
2 film shows an AFM peak in
dρ/dT at low temperature, similar to that of PdCrO
2 single crystals. On the other hand, the PdFe
xCo
1–xO
2 films (0 ≤
x ≤ 0.2) present a dip at around 20 K. Moreover, our PdCr
xCo
1–xO
2 films show similar transport behaviors to the PdFe
xCo
1–xO
2 films, distinct from either pure PdCrO
2 or PdCoO
2 films. This raises questions about the disruption caused by the Cr-Co interaction to the AFM order in the pure CrO
2 layer. In this presentation, we present our quantitative analysis of the Cr-Co interaction in PdCr
xCo
1–xO
2 films with various chromium concentrations (0 ≤
x ≤ 1). Our findings provide new insights into tuning magnetic properties through targeted solid solutions that introduce unpaired electrons into delafossite materials.