English

Room-temperature magnon-phonon transduction in high-damping Co/Pt structures

Materials Science 2026-06-26 v1

Abstract

Quantum communication and information processing strongly benefit from the coupling between different quasi-particles, offering complementary advantages. Magnetoelastic materials inherently allow for direct coupling between magnetization dynamics and quantized lattice vibrations, called phonons. Near the ferromagnetic resonances, phonons may thus trade energy and angular momentum with uniformly precessing magnetization, called magnons, and enable transduction of information from magnetic to phononic modes, thereby paving the way for long-range transport of magnetic information without the need of magnetic material. Here, we employ tailored magnetic-nonmagnetic heterostructures, which simultaneously act as cavities for standing shear waves, to bring selective phonons and magnons into resonance. These Co films with Pt seed layers show extended linewidth and reduced amplitude of the phonon-resonant FMR lines, providing a hallmark of energy and angular momentum exchange. Complementarily, by theoretical modeling and ultra-fast coherent phonon spectroscopy, we identify the responsible transverse acoustic phonons as standing shear waves in the combined Co and Pt structure. We find a high crystal quality in conjunction with a large magnetoelastic coupling constant as a prerequisite for efficient magnon-phonon coupling of this type. Such resonant enhancement of magnon-phonon coupling in CMOS-compatible material provides an ideal material platform for future quantum transducers.

Keywords

Cite

@article{arxiv.2606.28073,
  title  = {Room-temperature magnon-phonon transduction in high-damping Co/Pt structures},
  author = {Gauravkumar Patel and Takuma Sato and Maximilian Frenzel and Prakriti P. Joshi and Ruslan Salikhov and Ievgeniia Korniienko and Dominik Legut and Olav Hellwig and Sebastian F. Maehrlein and Kilian Lenz and Jürgen Lindner},
  journal= {arXiv preprint arXiv:2606.28073},
  year   = {2026}
}