1999
DOI: 10.1103/physrevlett.83.2829
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Disordered Magnetism at the Grain Boundary of Pure Nanocrystalline Iron

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Cited by 141 publications
(94 citation statements)
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References 27 publications
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“…1(b)) reveals the frequency dispersion of the signal more distinctly, albeit at a lower temperature of around 160 K. It is rather a common feature that the peak in χ ′′ 1 appears at a lower temperature than the same in the χ ′ 1 , and has been observed in many well-known systems [18][19][20] , but the temperature difference here (≈ 30 K) seems to be unusually large. However, even such behavior has been observed earlier 21 , especially in systems with coexisting ferromagnetic and spin-glass features, appearing from the grains and the disordered grain boundaries, respectively 22 . It is to be noted that the ferromagnetic T c of Sr 2 FeMoO 6 lies well above 400 K and therefore, this low temperature transition can only be associated with a coexisting metastability in the sample, arising from a very different magnetic origin.…”
Section: Resultsmentioning
confidence: 80%
“…1(b)) reveals the frequency dispersion of the signal more distinctly, albeit at a lower temperature of around 160 K. It is rather a common feature that the peak in χ ′′ 1 appears at a lower temperature than the same in the χ ′ 1 , and has been observed in many well-known systems [18][19][20] , but the temperature difference here (≈ 30 K) seems to be unusually large. However, even such behavior has been observed earlier 21 , especially in systems with coexisting ferromagnetic and spin-glass features, appearing from the grains and the disordered grain boundaries, respectively 22 . It is to be noted that the ferromagnetic T c of Sr 2 FeMoO 6 lies well above 400 K and therefore, this low temperature transition can only be associated with a coexisting metastability in the sample, arising from a very different magnetic origin.…”
Section: Resultsmentioning
confidence: 80%
“…The techniques of inert gas condensation, [3,[47][48][49][50] pulsed plasma deposition, [25] and sputtering [48] have exclusively been used for processing thin films or small amounts of nanocrystalline materials, whereas it is necessary to produce/process bulk samples for oxidation/corrosion or mechanical testing. Electrodeposition [33,34,51] and severe plastic deformation [28][29][30][31][52][53][54][55][56][57][58][59][60][61][62][63][64][65][66][67][68] have been recognized as the two relatively successful routes for processing thicker/larger sections of nanocrystalline metals and alloys. Pulsed electrodeposition has been employed successfully for processing nanocrystalline materials in bulk, [51] most notably, Ni-Fe and Ni-Co alloys.…”
Section: B Synthesis Of Nanocrystalline Alloysmentioning
confidence: 99%
“…Peculiarly, in the case rϾr c -as a tribute to intrinsic randomness-reentrance into a SSG phase is encountered at low temperatures similarly as in amorphous 13 and nanocrystalline 14 FM materials. It is argued in this case that SSG and SFM ordering takes place on different percolating clusters, thus establishing the coexistence of two phases.…”
Section: Introductionmentioning
confidence: 99%