Photonics Insights, Volume. 1, Issue 2, R05(2022)
Terahertz spin dynamics in rare-earth orthoferrites Story Video , Author Presentation , On the Cover
Fig. 1. Overview of current scientific and technological interests related to spin dynamics in solid-state materials. Four topics arranged as smaller triangular elements are covered in this review, which are key elements for achieving the three grander goals (three sides of the larger triangle).
Fig. 2. “Phase space” for review articles in spintronics, spanned by the horizontal axis of materials and vertical axis of novel physical phenomena. The current review represents a vertical cut in the phase space.
Fig. 4. Basic physical properties of
Fig. 5. Observation of (a) the inverse Faraday effect[118] and (b) the inverse Cotton–Mouton effect[119] in
Fig. 6. Path of solving for the full dynamics of photomagnetic pump, magneto-optical probe experiments on
Fig. 7. THz time-domain techniques. (a) Layout of a THz time-domain spectroscopy setup configured in a transmission geometry. (b) Zoom-in view of the polarization-sensitive differential detection setup[36]. (c) Layout of a THz emission spectroscopy setup. (d) Function of a reflective echelon used in a single-shot THz spectrometer[138]. (e) Pulse-front-tilt technique for generating intense THz radiation in
Fig. 8. Six measurement configurations, along with the magnon polarization selection rule in the
Fig. 9. Temperature-dependent SRT probed by THz spectroscopy[170
Fig. 10. Magnetic-field-induced
Fig. 11. CFTs of
Fig. 12. CFTs of
Fig. 13. Studying
Fig. 14. Electromagnons in
Fig. 15. Three-temperature model. (a) Separate but mutually interacting reservoirs. (b) Time dynamics of temperatures of the reservoirs.
Fig. 17. Ultrafast-heating-induced SRT in
Fig. 18. (a) Ultrafast-heating-induced SRT in
Fig. 19. Reconfigurable magnetic domains in
Fig. 21. Inertia-driven SRT in
Fig. 22. Domain-controllable laser-induced SRT due to the combined effect of IFE and ultrafast heating[232]. (a) Faraday rotation images taken after a single shot of pump pulse by various delay times around the
Fig. 23. Domain-controllable SRT in
Fig. 24. Solution of
Fig. 25. Nonlinear phononic control of magnetic phases in
Fig. 27. Phonon IFE in
Fig. 28. Nonlinear excitation of magnons by pumping rare-earth crystal-field transitions[244]. (a) Intense THz pump repopulates
Fig. 29. Comparing the onset of magnetic anisotropy due to rare-earth pumping and phonon pumping[245]. (a) Pathway that leads to anisotropy modification. 25 THz pump drives optical phonons, while 33 THz pump drives
Fig. 30. Floquet spectrum and exchange interaction energy of a two-site cluster Hubbard model[256]. (a) Energy-level structure versus the Floquet parameter
Fig. 31. Floquet modification of exchange interaction in
Fig. 32. High
Fig. 33. Double-pulse coherent control of magnons in
Fig. 34. Single-pulse coherent control of magnons in
Fig. 35. Magnon–phonon-polaritons in a photonic crystal cavity[295]. (a) Experimental configuration. (b) Electro-optic sampling imaging of the cavity mode 3 ps after pump excitation. (c) Anticrossing branches of the magnon–phonon-polariton. Temperature is adjusted to detune the magnon and the phonon-polariton frequencies. Gray and yellow markers: data. Solid lines: polariton branches. Dashed lines: mode frequencies assuming no coupling. Reproduced with permission from Ref. [295].
Fig. 36. Magnon-polaritons in a Fabry–Pérot cavity[296]. (a) Experimental phase shift of
Fig. 37. Magnon–phonon-polaritons in a hybrid waveguide[295]. (a) Experimental configuration. (b) Dispersion relation of transverse-electric phonon-polariton modes. (c) Zoom-in view of the red-oval-enclosed region, where polariton branches form an anticrossing pattern. Reproduced with permission from Ref. [295].
Fig. 38. Signatures of magnon-polaritons in free space[297]. (a) As optically excited magnons propagate in a
Fig. 39. Demonstration of magnon propagation at a supersonic group velocity[299]. (a) High-
Fig. 40. Efficient magnon excitation in
Fig. 41. Correlated SRT in
Fig. 42. Nonlinearity of magnons as evidence for all-coherent spin switching[312]. (a) Experimental configuration. (b) Spin orientations in the
Fig. 43. 2D coherent THz spectroscopy[313]. (a) Experimental configuration. (b) Various signal fields with either a single pulse or double pulses. The nonlinear signal
Fig. 44. Light–matter interaction setup for studying the Dicke phase transition in the USC regime[337]. (a)
Fig. 46. Evidence for Dicke cooperativity in magnetic interactions[169]. (a)–(k) THz absorption spectra of
Fig. 47. Magnonic superradiant phase transition in
Fig. 48. Temperature-field phase diagram for
Fig. 49.
Fig. 50. Perfect intrinsic squeezing at an SRPT critical point[338]. Minimized quadrature fluctuation (red) versus coupling strength shows perfect suppression at the SRPT transition point. Upper panel shows complementary polariton mode frequencies.
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Xinwei Li, Dasom Kim, Yincheng Liu, Junichiro Kono, "Terahertz spin dynamics in rare-earth orthoferrites," Photon. Insights 1, R05 (2022)
Category: Review Articles
Received: Sep. 2, 2022
Accepted: Nov. 10, 2022
Published Online: Jan. 19, 2023
The Author Email: Kono Junichiro (kono@rice.edu)