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Microwave interference between a spin ensemble and its mirror image

  • B.-Y. Wu (Co-first Author)
  • , Y.-T. Cheng (Co-first Author)
  • , K.-T. Lin (Co-first Author)
  • , Fahad Aziz
  • , C.-X. Run
  • , K.-M. Hsieh
  • , J.-C. Liu
  • , K.-V. Rangdhol
  • , Y.-Y. Yeung
  • , Sen Yang
  • , Qiming Shao
  • , Xin Wang
  • , Y.-Y. Zhao
  • , A. F. Kockum
  • , G.-D. Lin
  • , Franco Nori
  • , I.-C. Hoi*
  • *Corresponding author for this work

Research output: Journal Publications and ReviewsRGC 21 - Publication in refereed journalpeer-review

Abstract

We investigate microwave interference between a spin ensemble and its mirror image in a one-dimensional (1D) waveguide. Away from the mirror, the resonance frequency of the Kittel mode (KM) inside a ferrimagnetic spin ensemble displays sinusoidal shifts (compared to a setup without the mirror) as a function of the distance to the mirror. Furthermore, the radiative decay of the KM into the waveguide shows a cosine-squared oscillation as the distance to the mirror is varied. These shifting frequencies and decay rates are a consequence of the KM’s interaction with its own image, mediated by the waveguide. The decay is enhanced twofold when the spin ensemble sits at the magnetic antinode of the corresponding eigenmode in the waveguide; conversely, we measure an extension of the KM lifetime by a factor of 8 when the spin ensemble is approximately at a node. We can finely tune the KM decay rate to achieve maximal absorption of input photons at a critical coupling point. Moreover, by pumping the spin ensemble to generate a pump-induced magnon mode in a two-tone experiment, we achieve a pump-induced phase shift of up to about 90° for a coherent microwave probe field.

©2026 American Physical Society
Original languageEnglish
Article number 053720
Number of pages15
JournalPhysical Review A
Volume113
Issue number5
Online published26 May 2026
DOIs
Publication statusPublished - May 2026

Funding

We thank Bimu Yao for fruitful discussions. I.-C.H. acknowledges financial support from City University of Hong Kong through the start-up Project No. 9610569, from the Research Grants Council of Hong Kong (Grant No. 11312322) and from Guangdong Provincial Quantum Science Strategic Initiative (GDZX2203001, GDZX2303005, and GDZX2403001). F.N. is supported in part by the Japan Science and Technology Agency (JST) [via the CREST Quantum Frontiers program Grant No. JPMJCR24I2, the Quantum Leap Flagship Program (Q-LEAP), and the Moonshot R&D Grant No. JPMJMS2061]. A.F.K. acknowledges support from the Swedish Foundation for Strategic Research (Grants No. FFL21-0279 and No. FUS21-0063), the Horizon Europe programme HORIZON-CL4-2022-QUANTUM-01-SGA via the Project No. 101113946 OpenSuperQPlus100, and from the Knut and Alice Wallenberg Foundation through the Wallenberg Centre for Quantum Technology (WACQT). G.-D.L. acknowledges support from National Science and Technology Council Grants No. NSTC-113-2112-M-002-025 and No. NSTC-112-2112-M-002-001. J.-C.L. and Q.S. acknowledge the funding support from RGC-GRF (16303322).

RGC Funding Information

  • RGC-funded

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