Decay of Higgs amplitude mode in quasi two-dimensional antiferromagnet Ba<sub>2</sub>FeSi<sub>2</sub>O<sub>7</sub>
ORAL
Abstract
Spontaneous symmetry breaking produces longitudinal amplitude (Higgs) mode as a well-defined collective excitation [1]. We investigate the emergence of the longitudinal mode in two-dimensional square-lattice antiferromagnet Ba2FeSi2O7 –easy-plane antiferromagnet with effective S=1 near a continuous quantum phase transition into a quantum paramagnet [2,3]. Our inelastic neutron scattering measurements and extended spin wave theory analysis demonstrate its proximity to the quantum critical point (QCP), and reveal the presence of the longitudinal mode in the observed spectra. The longitudinal mode is visible thoughout the Brillouin zone. Noticeably, this mode is highly renormalized and broadened near the magnetic zone center, which though decay channels to the transverse mode. Finally, we discuss the necessary theoretical corrections to a generalized linear spin wave theory to accurately describe the decay of the longitudinal magnon in Ba2FeSi2O7.
[1] D. Pekker and C. M. Varma, Annu. Rev. Condens. Matter Phys. 6 269 (2015)
[2] M. Matsumoto, Journal. of the Phys. Soc. of Jap. 83 084704 (2014)
[3] T.-H. Jang et al., (in preparation)
[1] D. Pekker and C. M. Varma, Annu. Rev. Condens. Matter Phys. 6 269 (2015)
[2] M. Matsumoto, Journal. of the Phys. Soc. of Jap. 83 084704 (2014)
[3] T.-H. Jang et al., (in preparation)
*This research was supported by the U.S. Department of Energy, Office of Science, Basic Energy Sciences, Materials Sciences and Engineering Division.
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Presenters
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Seunghwan Do
- Materials Science and Technology Division, Oak Ridge National Laboratory
- Oak Ridge National Laboratory