2007
DOI: 10.1016/j.jmmm.2006.10.649
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Spin dynamics in oxide glass of Fe2O3–Bi2O3–B2O3 system

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Cited by 13 publications
(18 citation statements)
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“…1 For example, BiFeO 3 crystal exhibits an antiferromagnetic ͑AFM͒ transition at Néel temperature, T N = 643 K, with weak ferromagnetism 2 while rapidly quenched amorphous BiFeO 3 film exhibits a transition from a paramagnetic ͑PM͒ to spin-glass ͑SG͒ phase at the SG transition temperature, T SG =20 K. 3 The AFM superexchange interaction via oxide ions is predominant in most of the magnetic amorphous oxides. [4][5][6][7][8][9] Due to the randomly distributed magnetic ions in amorphous oxides, the predominant AFM interaction causes geometrical magnetic frustration in the arrangement of magnetic moments. This leads to the random freezing of magnetic moments, i.e., SG transition [4][5][6][7][8][9] and the drastic suppression of magnetic ordering temperature.…”
Section: Introductionmentioning
confidence: 99%
“…1 For example, BiFeO 3 crystal exhibits an antiferromagnetic ͑AFM͒ transition at Néel temperature, T N = 643 K, with weak ferromagnetism 2 while rapidly quenched amorphous BiFeO 3 film exhibits a transition from a paramagnetic ͑PM͒ to spin-glass ͑SG͒ phase at the SG transition temperature, T SG =20 K. 3 The AFM superexchange interaction via oxide ions is predominant in most of the magnetic amorphous oxides. [4][5][6][7][8][9] Due to the randomly distributed magnetic ions in amorphous oxides, the predominant AFM interaction causes geometrical magnetic frustration in the arrangement of magnetic moments. This leads to the random freezing of magnetic moments, i.e., SG transition [4][5][6][7][8][9] and the drastic suppression of magnetic ordering temperature.…”
Section: Introductionmentioning
confidence: 99%
“…8 To clarify the mechanism of magnetic transition in oxide glasses, many studies have been performed on temperature dependence of dc and ac magnetic susceptibilities, Mössbauer spectrum, electron-spin-resonance spectrum, and so forth. [9][10][11][12][13][14][15][16][17][18][19][20][21][22][23] As a result, magnetic oxide glasses, in particular, those containing 3d transition-metal ions, have been regarded as a prototype of insulating spin glass. Recently, we have reported that Fe 2 O 3 -TeO 2 glasses manifest curious phenomena relevant to spin dynamics, including magnetic aging and memory effects as well as critical slowing down similar to those observed in canonical spin glasses.…”
Section: Introductionmentioning
confidence: 99%
“…1 Instead, short-range antiferromagnetic (AFM) superexchange interactions via 2p states of oxide ions are predominant in the magnetic oxide glasses, [2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17][18] with some exceptions such as Eu 2+ -containing glasses, where ferromagnetic (FM) interactions prevail. [19][20][21][22][23] In a system where magnetic moments are located at randomly distributed cations, the short-range AFM interactions inevitably bring about magnetic frustrations of geometrical origin.…”
Section: Introductionmentioning
confidence: 99%
“…[2][3][4][5][6][7][8][9][10][11][12][13][14][15][16][17] Those 3d TM-containing glasses have negative Weiss temperatures, the amplitude of which is tens or hundreds of degrees Kelvin, and exhibit a paramagnetic (PM) to SG transition at several or tens of degrees Kelvin. On the other hand, most of the oxide glasses possessing 4f rare-earth (RE) ions seldom show any magnetic transition down to 2 K, 24,25 which can be easily accessed in magnetic measurements.…”
Section: Introductionmentioning
confidence: 99%