1995
DOI: 10.1021/j100009a050
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Local order and global disorder in bidisperse ferrofluids

Abstract: We study the magnetization response of a frozen ferrofluid as large-diameter (10-nm) magnetite particles are added to a dilute, random distribution of small-diameter (5-nm) moments. The small dipole moments are free to relax down to low temperatures, while the large dipoles become immobilized when the solvent freezes, acting as a random local field. The glass transition temperature is a sensitive function of the random field concentration, permitting the investigation of the crossover from spin-glass to random… Show more

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“…Another type of quenched disorder occurs in systems of dipolar particles with the positions being frozen in an irregular configuration. Examples for such systems, which seem better described as amorphous solids rather than as liquids, are mixed crystals with polar impurities (e.g., K 1−x Li x TaO 3 ) [153,154], diluted dipolar-coupled magnets (e.g., LiHo x Y 1−x F 4 ) [155,156], assemblies of ultrafine ferromagnetic particles [157,158], and 'frozen ferrofluids' [159][160][161][162]. The latter systems result from a quench of an equilibrated ferrofluid into a state below the freezing temperature of the non-magnetic solvent.…”
Section: Positional Disordermentioning
confidence: 99%
“…Another type of quenched disorder occurs in systems of dipolar particles with the positions being frozen in an irregular configuration. Examples for such systems, which seem better described as amorphous solids rather than as liquids, are mixed crystals with polar impurities (e.g., K 1−x Li x TaO 3 ) [153,154], diluted dipolar-coupled magnets (e.g., LiHo x Y 1−x F 4 ) [155,156], assemblies of ultrafine ferromagnetic particles [157,158], and 'frozen ferrofluids' [159][160][161][162]. The latter systems result from a quench of an equilibrated ferrofluid into a state below the freezing temperature of the non-magnetic solvent.…”
Section: Positional Disordermentioning
confidence: 99%