Superparamagnetic behaviour andT1,T2relaxivity of ZnFe2O4nanoparticles for magnetic resonance imaging

Manjura Hoque, S. ; Srivastava, C. ; Venkatesha, N. ; Anil Kumar, P.S. ; Chattopadhyay, K. (2013) Superparamagnetic behaviour andT1,T2relaxivity of ZnFe2O4nanoparticles for magnetic resonance imaging Philosophical Magazine, 93 (14). pp. 1771-1783. ISSN 1478-6435

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Official URL: http://doi.org/10.1080/14786435.2012.755271

Related URL: http://dx.doi.org/10.1080/14786435.2012.755271

Abstract

In the present study, ZnFe2O4 nanoparticles were synthesized by the chemical co-precipitation followed by calcinations at 473 and 673 K for 4 h. Particle sizes obtained were 4 and 6 nm for the calcination temperatures of 473 and 673 K, respectively. To study the origin of system’s low temperature spin dynamic behaviour, temperature dependence of susceptibility was investigated as a function of particle size and frequency. Slight increase in the grain size from 4 nm at 473 K to 6 nm at 673 K has led to a peak shift of temperature dependence of susceptibility measured at a constant frequency of 400 Hz. Temperature dependence of at different frequencies also resulted in peak shift. Relaxation time dependence of peak temperature obeys a power law, which provides the fitting parameters within the range of superparamagnetic nature of the particles. Further, dependence of relaxation time and peak temperature obeys Vogel–Fulcher law rather than Néel–Brown equation demonstrating that the particles follow the behaviour of superparamagnetism of slightly interacting system. Spin–lattice, T 1 and spin–spin, T 2 relaxivity of proton of the water molecule in the presence of chitosan-coated superparamagnetic ZnFe2O4 nanoparticle yields the values of 0.002 and 0.360 s−1 per ppm.

Item Type:Article
Source:Copyright of this article belongs to Informa UK Limited
Keywords:ZnFe2O4;superparamagnetism;T 1 and T 2 relaxivity;nuclear magnetic resonance;transmission electron microscopy
ID Code:135347
Deposited On:23 Jan 2023 04:01
Last Modified:23 Jan 2023 04:01

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