Terahertz magneto-optical investigation of quadrupolar spin-lattice effects in magnetically frustrated Tb2Ti2O7
Source abstract
Abstract
Condensed matter magneto-optical investigations can be a powerful probe of a material's microscopic magnetoelectric properties. This is because subtle interactions between electric and magnetic multipoles on a crystal lattice show up in predictable and testable ways in a material's optical response tensor, which dictates the polarization state and absorption spectrum of propagating electromagnetic waves. Magneto-optical techniques are therefore strong complements to probes such as neutron scattering, particularly when spin-lattice coupling effects are present. Here we perform a magneto-optical investigation of vibronic spin-lattice coupling in the magnetically frustrated pyrochlore ${\mathrm{Tb}}2{\mathrm{Ti}}2{\mathrm{O}}7$. Coupling of this nature involving quadrupolar mixing between the ${\mathrm{Tb}}3+$ electronic levels and phonons in ${\mathrm{Tb}}2{\mathrm{Ti}}2{\mathrm{O}}7$ has been a topic of debate for some time. This is particularly due to its implication for describing the exotic spin-liquid phase diagram of this highly debated system. A manifestation of this vibronic effect is observed as splitting of the ground and first excited crystal field doublets of the ${\mathrm{Tb}}3+$ electronic levels, providing a fine structure to the absorption spectra in the terahertz (THz) frequency range. In this investigation, we apply a static magnetic field along the cubic [111] direction while probing with linearly polarized THz radiation. Through the Zeeman effect, the magnetic field enhances the splitting within the low-energy crystal field transitions revealing new details in our THz spectra. Complementary magneto-optical quantum calculations including quadrupolar terms show that indeed vibronic effects are required to describe our observations at 3 K. A further prediction of our theoretical model is the presence of a novel magneto-optical birefringence as a result of this vibronic process. Essentially, spin-lattice coupling within ${\mathrm{Tb}}2{\mathrm{Ti}}2{\mathrm{O}}7$ may break the optical isotropy of the cubic system, supporting two different electromagnetic wave propagations within the crystal. Together our results reveal the significance of considering quadrupolar spin-lattice effects when describing the spin-liquid ground state of ${\mathrm{Tb}}2{\mathrm{Ti}}2{\mathrm{O}}7$. They also highlight the potential for future magneto-optical investigations to probe complex materials where spin-lattice coupling is present and reveal new magneto-optical activity in the THz range.
Source: openalex_inverted_index · Quality: baseline
Research context
OpenAlex topics: Advanced Condensed Matter Physics · Multiferroics and related materials · Seismic Waves and Analysis
SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.
References (42)
Show source-provided references
1. 10.1103/PhysRevB.8.57110.1103/PhysRevB.8.571 ↗
2. 10.1103/Physics.2.2010.1103/Physics.2.20 ↗
3. 10.1103/PhysRevLett.84.371810.1103/PhysRevLett.84.3718 ↗
4. 10.1103/PhysRevLett.88.06720310.1103/PhysRevLett.88.067203 ↗
5. 10.1103/RevModPhys.82.5310.1103/RevModPhys.82.53 ↗
6. 10.1103/PhysRevB.68.18040110.1103/PhysRevB.68.180401 ↗
7. 10.1103/PhysRevB.83.18443410.1103/PhysRevB.83.184434 ↗
8. 10.1103/PhysRevB.84.18440910.1103/PhysRevB.84.184409 ↗
9. 10.1103/PhysRevLett.111.08720110.1103/PhysRevLett.111.087201 ↗
10. 10.1103/PhysRevLett.112.01720310.1103/PhysRevLett.112.017203 ↗
11. 10.1103/PhysRevLett.105.07720310.1103/PhysRevLett.105.077203 ↗
12. I. V. Aleksandrov · Sov. Phys. JETP · 1985 · 62 · 1287
13. 10.1038/nature0115710.1038/nature01157 ↗
14. 10.1103/PhysRevB.94.02443010.1103/PhysRevB.94.024430 ↗
15. 10.1103/PhysRevB.95.02041510.1103/PhysRevB.95.020415 ↗
16. 10.1103/PhysRevB.87.06040810.1103/PhysRevB.87.060408 ↗
17. 10.1103/PhysRevB.62.649610.1103/PhysRevB.62.6496 ↗
18. 10.1103/PhysRevB.64.22441610.1103/PhysRevB.64.224416 ↗
19. 10.1103/PhysRevB.76.18443610.1103/PhysRevB.76.184436 ↗
20. 10.1103/PhysRevB.77.21431010.1103/PhysRevB.77.214310 ↗
21. 10.1063/1.167216710.1063/1.1672167 ↗
22. 10.1063/1.44243710.1063/1.442437 ↗
23. 10.1063/1.44752610.1063/1.447526 ↗
24. 10.1134/1.198402810.1134/1.1984028 ↗
25. 10.1038/nphys21210.1038/nphys212 ↗
26. 10.1103/PhysRevB.89.19514510.1103/PhysRevB.89.195145 ↗
27. 10.1103/PhysRevB.86.17440310.1103/PhysRevB.86.174403 ↗
28. 10.1080/1364281920822458910.1080/13642819208224589 ↗
29. B. E. A. Saleh · 199110.1002/0471213748 ↗
30. 10.1103/PhysRevLett.116.21720110.1103/PhysRevLett.116.217201 ↗
31. 10.1103/PhysRevB.88.18442810.1103/PhysRevB.88.184428 ↗
32. 10.1038/s41592-019-0686-210.1038/s41592-019-0686-2 ↗
33. 10.1107/S002188981103897010.1107/S0021889811038970 ↗
34. 10.1088/0370-1298/65/3/30810.1088/0370-1298/65/3/308 ↗
35. 10.1016/S0081-1947(08)60517-210.1016/S0081-1947(08)60517-2 ↗
36. 10.1088/0953-8984/24/25/25600310.1088/0953-8984/24/25/256003 ↗
37. 10.1134/S0030400X1406013710.1134/S0030400X14060137 ↗
38. 10.1103/PhysRevB.89.13441010.1103/PhysRevB.89.134410 ↗
39. 10.1103/PhysRev.62.43810.1103/PhysRev.62.438 ↗
40. B. G. Wybourne · 1965
41. 10.1103/PhysRevB.91.22443010.1103/PhysRevB.91.224430 ↗
42. 10.1063/1.167390410.1063/1.1673904 ↗