Bulletin of the American Physical Society
Fall 2024 Joint Meeting of the Texas Section of the APS, Texas Section of the AAPT & Zone 13 of the SPS
Thursday–Saturday, October 17–19, 2024; Southern Methodist University, Dallas, Texas
Session FB01: Poster Session (12:00pm - 1:00pm & 2:30pm - 3:30pm)
12:00 PM,
Friday, October 18, 2024
Southern Methodist University
Room: Lobby
Abstract: FB01.00024 : Non-Debye Behavior of the Néel and Brown Relaxation in Interacting Magnetic Nanoparticle Ensembles
Presenter:
Jeffrey M Knoop
(University of Texas at San Antonio)
Authors:
Cristian Botez
(University of Texas at San Antonio)
Jeffrey M Knoop
(University of Texas at San Antonio)
Below TF, the Néel mechanism is entirely responsible for the superspin relaxation, as the carrier fluid is frozen. We found that the temperature dependence of the relaxation time, τN(Tp1), is well described by the Dorman–Bessais–Fiorani (DBF) model. Above TF, both the internal (Néel) and the Brownian superspin relaxation mechanisms are active. Yet, we found evidence that the effective relaxation times, τeff, corresponding to the Tp2 peaks observed in the denser samples do not follow the typical Debye behavior described by the Rosensweig formula (τeff)-1= (τB)-1+(τN)-1.
First, τeff is 5 × 10−5 s at 225 K, almost three orders of magnitude more that its Néel counterpart, τN~8 × 10−8 s, estimated by extrapolating the above-mentioned DBF analysis. Thus, (τN)-1 >> (τeff)-1, which is clearly not consistent with the Rosensweig formula.
Second, the observed temperature dependence of the effective relaxation time, τeff(Tp2), is excellently described by a model solely based on the hydrodynamic Brown relaxation combined with an activation law for the temperature variation of the viscosity. The best fit yields 𝛾0 = 312 K, and T0′ = 178 K.
Finally, the higher temperature Tp2 peaks vanish in the more diluted samples (δ ≤ 0.02). This indicates that the formation of larger hydrodynamic particles via aggregation, which is responsible for the observed Brownian relaxation in dense samples, is inhibited by dilution. Our findings, corroborating previous results from Monte Carlo calculations, are important because they might lead to new strategies to synthesize functional magnetic ferrofluids for biomedical applications.
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