Abstract:Spin-phonon coupling, the interaction of spins with surrounding lattice is a key parameter to understand the underlying physics of multiferroics and engineer their magnetization dynamics. Elementary excitations in multiferroic materials are strongly influenced by spin-phonon interaction, making Raman spectroscopy a unique tool to probe these coupling(s). Recently, it has been suggested that the dielectric and magnetic properties of 15R-type hexagonal BaMnO3 are correlated through the spin-lattice coupling. Her… Show more
“…Overall, the magnetic-field-induced frequency shifts are indications of the magnitude of spin-phonon coupling strengths of each mode. We postulate that when the applied field modifies the orientation and interaction of spins, the interatomic spring constants and the frequency of each mode changes accordingly, in a similar mechanism as the static magnetostriction effect. , Although nonmagnetic materials may also exhibit finite magnetostriction, , the observed large magnitude of phonon softening on the order of 0.1% above 4T is more consistent with the materials’ strong spin exchange interaction and magnetic order. , We have not observed any saturation or hysteresis in either the helicity or the intensity of the field-dependent Raman spectra, implying that the spin order, if any, is unlikely to be ferromagnetism. This agrees with the antiferromagnetic exchange between iron spins observed in pure Cs 3 Fe 2 Br 9 , but the onset of spin correlation occurs at a much higher temperature in doped ultrathin films than pure crystals .…”
Section: Resultsmentioning
confidence: 62%
“…We postulate that when the applied field modifies the orientation and interaction of spins, the interatomic spring constants and the frequency of each mode changes accordingly, in a similar mechanism as the static magnetostriction effect. 37,38 Although nonmagnetic materials may also exhibit finite magnetostriction, 39,40 the observed large magnitude of phonon softening on the order of 0.1% above 4T is more consistent with the materials' strong spin exchange interaction and magnetic order. 41,42 We have not observed any saturation or hysteresis in either the helicity or the intensity of the field-dependent Raman spectra, implying that the spin order, if any, is unlikely to be ferromagnetism.…”
Spin in semiconductors facilitates magnetically controlled optoelectronic and spintronic devices. In metal halide perovskites (MHPs), doping magnetic ions is proven to be a simple and efficient approach to introducing a spin magnetic momentum. In this work, we present a facile metal ion doping protocol through the vapor-phase metal halide insertion reaction to the chemical vapor deposition (CVD)-grown ultrathin Cs 3 BiBr 6 perovskites. The Fe-doped bismuth halide (Fe:CBBr) perovskites demonstrate that the iron spins are successfully incorporated into the lattice, as revealed by the spinphonon coupling below the critical temperature T c around 50 K observed through temperature-dependent Raman spectroscopy. Furthermore, the phonons exhibit significant softening under an applied magnetic field, possibly originating from magnetostriction and spin exchange interaction. The spin-phonon coupling in Fe:CBBr potentially provides an efficient way to tune the spin and lattice parameters for halide perovskite-based spintronics.
“…Overall, the magnetic-field-induced frequency shifts are indications of the magnitude of spin-phonon coupling strengths of each mode. We postulate that when the applied field modifies the orientation and interaction of spins, the interatomic spring constants and the frequency of each mode changes accordingly, in a similar mechanism as the static magnetostriction effect. , Although nonmagnetic materials may also exhibit finite magnetostriction, , the observed large magnitude of phonon softening on the order of 0.1% above 4T is more consistent with the materials’ strong spin exchange interaction and magnetic order. , We have not observed any saturation or hysteresis in either the helicity or the intensity of the field-dependent Raman spectra, implying that the spin order, if any, is unlikely to be ferromagnetism. This agrees with the antiferromagnetic exchange between iron spins observed in pure Cs 3 Fe 2 Br 9 , but the onset of spin correlation occurs at a much higher temperature in doped ultrathin films than pure crystals .…”
Section: Resultsmentioning
confidence: 62%
“…We postulate that when the applied field modifies the orientation and interaction of spins, the interatomic spring constants and the frequency of each mode changes accordingly, in a similar mechanism as the static magnetostriction effect. 37,38 Although nonmagnetic materials may also exhibit finite magnetostriction, 39,40 the observed large magnitude of phonon softening on the order of 0.1% above 4T is more consistent with the materials' strong spin exchange interaction and magnetic order. 41,42 We have not observed any saturation or hysteresis in either the helicity or the intensity of the field-dependent Raman spectra, implying that the spin order, if any, is unlikely to be ferromagnetism.…”
Spin in semiconductors facilitates magnetically controlled optoelectronic and spintronic devices. In metal halide perovskites (MHPs), doping magnetic ions is proven to be a simple and efficient approach to introducing a spin magnetic momentum. In this work, we present a facile metal ion doping protocol through the vapor-phase metal halide insertion reaction to the chemical vapor deposition (CVD)-grown ultrathin Cs 3 BiBr 6 perovskites. The Fe-doped bismuth halide (Fe:CBBr) perovskites demonstrate that the iron spins are successfully incorporated into the lattice, as revealed by the spinphonon coupling below the critical temperature T c around 50 K observed through temperature-dependent Raman spectroscopy. Furthermore, the phonons exhibit significant softening under an applied magnetic field, possibly originating from magnetostriction and spin exchange interaction. The spin-phonon coupling in Fe:CBBr potentially provides an efficient way to tune the spin and lattice parameters for halide perovskite-based spintronics.
“…A non-reciprocal magneto-phonon interaction was also reported for CrI 3 in the form of polarization rotation asymmetric with magnetic field 43 , but little to negligible shift of the vibrational Raman modes was described in that report. In addition to CrI 3 , Raman frequency shifts in response to magnetic field have been observed in 15R-BaMnO 3 44 . The hysteretic shifts in α-RuCl 3 Raman modes reported here are statistically significant, but highly variable.…”
“…Even-though BaFe 2 Se 3 is only superconducting under pressure and at low temperature, the possibility of a spin-lattice coupling stronger than first expected need to be investigated. Indeed, growing number of works have recently accessed the importance of spin-lattice coupling in strongly correlated systems [29][30][31].…”
Section: Dft Calculations and Discussionmentioning
This paper presents a study of the lattice dynamics in BaFe2Se3. We combined first-principle calculations, infrared measurements and a thorough symmetry analysis. Our study confirms that Pnma cannot be the space group of BaFe2Se3, even at room temperature. The phonons assignment requires Pm to be the BaFe2Se3 space group, not only in the magnetic phase, but also in the paramagnetic phase at room temperature. This is due to a strong coupling between a short range spin-order along the ladders, and the lattice degrees of freedom associated with the Fe-Fe bond length. This coupling induces a change in the bond-length pattern from an alternated trapezoidal one (as in $Pnma$) to an alternated small/large rectangular one. Out of the two patterns, only the latter is fully compatible with the observed block-type magnetic structure. Finally, we propose a complete symmetry analysis of the BaFe2Se3 phase diagram in the 0-600\,K range.
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