2013
DOI: 10.7566/jpsj.82.043001
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Neutron Brillouin Scattering with Pulsed Spallation Neutron Source – Spin-Wave Excitations from Ferromagnetic Powder Samples –

Abstract: Neutron Brillouin scattering (NBS) method was developed using a pulsed spallation neutron source, and the feasibility of NBS was demonstrated by observing ferromagnetic spin waves in La0.8Sr0.2MnO3 and SrRuO3 powders. Gapless spin-wave excitations were observed in La0.8Sr0.2MnO3, which were continuously extended to the lower scattering vector Q from previous results using single crystals. The novel result is a well-defined quadratic Q dependence in the spin-wave dispersion curve with a large energy gap in SrRu… Show more

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Cited by 24 publications
(22 citation statements)
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“…As shown in Fig. 1 (a), the spin wave dispersion relation at 7 K was well fitted to E(Q) = E g + DQ 2 with an apparent energy gap E g [3]. We clearly found the energy gap by accessing the low Q by the NBS method.…”
Section: Neutron Brillouin Scattering Experimentsmentioning
confidence: 52%
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“…As shown in Fig. 1 (a), the spin wave dispersion relation at 7 K was well fitted to E(Q) = E g + DQ 2 with an apparent energy gap E g [3]. We clearly found the energy gap by accessing the low Q by the NBS method.…”
Section: Neutron Brillouin Scattering Experimentsmentioning
confidence: 52%
“…Owing to the kinematic constraints of neutron spectroscopy, incident neutron energy (E i ) in the sub-eV region with a high resolution (∆E) is necessary, and the scattered neutrons need to be detected at very low scattering angles, for measuring the scattering near to the forward direction. On the HRC, the NBS experiments became feasible by reducing the background noise at low scattering angles [3,4]. The low background noise was achieved by the T0 chopper and the incident beam collimator.…”
Section: Neutron Brillouin Scattering Experimentsmentioning
confidence: 99%
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“…Refinements of crystal and magnetic structures were carried out by the Rietveld method using the GSAS program. 12) INS measurements were performed at the TOF neutron spectrometers 4SEASONS 13,14) and HRC 15,16) installed at BL01 and BL12, respectively, in MLF, J-PARC. Roughly 11 and 50 g of powder were used for the 4SEASONS and HRC measurements, and the measurements were performed at T = 4, 103, and 224 K. INS data were visualized by software suites Utsusemi.…”
Section: Experimental Methodsmentioning
confidence: 99%
“…6) Since Mo 2 O 10 pillars are nonmagnetic and the distance between the layers is large, the interlayer interaction is expected to be very weak. Susceptibility measurement on polycrystalline La 5 Mo 4 O 16 shows an antiferromagnetic phase transition at T N = 190 K. 6,7) In addition, single-crystal magnetization measurements on La 5 Mo 4 O 16 exhibited a metamagnetic transition from the antiferromagnetic to ferrimagnetic state above 0.5 T. 8) This ferrimagnetic phase is only observed when an external magnetic field is applied along the c axis, suggesting easy-axis magnetic anisotropy. 5,8,9) Recently, intriguing magnetic phenomena in La 5 Mo 4 O 16 were reported.…”
Section: Introductionmentioning
confidence: 99%