A preliminary investigation of large shift in transition temperature (Tc) in Gd<sub>5</sub>Si<sub>3</sub> nanoparticles
POSTER
Abstract
Magnetic ordering temperatures in nanostructures depend on size. Curie temperature(Tc) of a bulk material where exchange interactions are comparable to thermal fluctuations tends to decrease in particles. The decrease of ordering temperature with size is described by the scaling theory of Fisher & Barber.
However, a large increase in Tc in Gd5Si3 NPs have been observed in the ball-milled gadolinium silicide. SEM images shows particle sizes ranging from 50 nm to >2 μm. XRD analysis on pre-separated sample show that ferromagnetic Gd5Si4 is the major phase while paramagnetic Gd5Si3 is the minor phase. Magnetic properties measured in VSM reveal that the Tc decreases for Gd5Si4 phase from 332K for bulk to 315K for ball-milled sample. Another Tc observed at 80K is attributed to Gd5Si3 phase undergoes large shift in its transition temperature at 110K and remains constant irrespective of particle sizes.
Plausible reasons for the increase in Tc for Gd5Si3 NPs could be due to the effect of high energy mechanical ball-milling process that could induce structural changes, lattice strains, exchange interaction between phases in a particle, or formation of new phase.
However, a large increase in Tc in Gd5Si3 NPs have been observed in the ball-milled gadolinium silicide. SEM images shows particle sizes ranging from 50 nm to >2 μm. XRD analysis on pre-separated sample show that ferromagnetic Gd5Si4 is the major phase while paramagnetic Gd5Si3 is the minor phase. Magnetic properties measured in VSM reveal that the Tc decreases for Gd5Si4 phase from 332K for bulk to 315K for ball-milled sample. Another Tc observed at 80K is attributed to Gd5Si3 phase undergoes large shift in its transition temperature at 110K and remains constant irrespective of particle sizes.
Plausible reasons for the increase in Tc for Gd5Si3 NPs could be due to the effect of high energy mechanical ball-milling process that could induce structural changes, lattice strains, exchange interaction between phases in a particle, or formation of new phase.
*Work at the Ames Lab was supported by DOE (contract No. DE-AC02-07CH11358). Work at VCU was funded by NSF, Award No.: 1610967.
Presenters
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Shivakumar Hunagund
- Virginia Commonwealth University