2020
DOI: 10.1002/pssb.201900704
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Magnons in the Multiferroic Phase of Cupric Oxide

Abstract: Polarized neutron scattering is used to characterize low-energy magnetic excitations in the multiferroic and antiferromagnetic phases of cupric oxide (CuO). The experiments are performed with the novel type of polarization analysis available at the thermal three-axes spectrometer PUMA@FRM, II allowing the simultaneous detection of spinflip and nonspinflip scattering. The energy gaps of several magnon modes are determined, and evidence for the existence of electromagnons near 3 and 13 meV is found.

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Cited by 4 publications
(3 citation statements)
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“…Earlier, Kimura et al have achieved the induced multiferroic behavior in CuO near to room temperature and also observed the memory effect in CuO [11,12]. Copper oxide (CuO) is a type-II multiferroics, which possess ferroelectric transition of T C at 230 K and three consecutive antiferromagnetic transitions of T N1 at 213 K, T N2 at 229.2 K and T N3 at 229.8 K [13]. Moreover, CuO is widely studied for its potential applications in electromagnetic based refrigerator, diluted magnetic semiconductors and high temperature superconductors [14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…Earlier, Kimura et al have achieved the induced multiferroic behavior in CuO near to room temperature and also observed the memory effect in CuO [11,12]. Copper oxide (CuO) is a type-II multiferroics, which possess ferroelectric transition of T C at 230 K and three consecutive antiferromagnetic transitions of T N1 at 213 K, T N2 at 229.2 K and T N3 at 229.8 K [13]. Moreover, CuO is widely studied for its potential applications in electromagnetic based refrigerator, diluted magnetic semiconductors and high temperature superconductors [14][15][16].…”
Section: Introductionmentioning
confidence: 99%
“…In such materials 8 11 the retardation effects are relatively large and cannot be ignored. There, the polarization, , of a ferroelectric manifests retarded response to the electric filed , hence , where is the polarizability tensor 12 , 13 in a linear response approximation. The superexchange interaction of magnetic moments in granular multiferroics 14 , where electric and magnetic degrees of freedom mutually influence each other, acquires retardation as well.…”
Section: Introductionmentioning
confidence: 99%
“…In such materials [8][9][10][11] the retardation effects are relatively large and cannot be ignored. There, the polarization, P, of a ferroelectric manifests retarded response to the electric filed E, hence P(t) = α(t−t )E(t )dt , where α is the polarizability tensor 12,13 in a linear response approximation. The superexchange interaction of magnetic moments in granular multiferroics 14 , where electric and magnetic degrees of freedom mutually influence each other, acquires retardation as well.…”
mentioning
confidence: 99%