Please use this identifier to cite or link to this item: http://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/11111
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dc.contributor.advisorBAJPAI, ASHNA-
dc.contributor.authorDEVARAKONDA, HIMABINDU-
dc.date.accessioned2026-05-21T09:28:57Z-
dc.date.available2026-05-21T09:28:57Z-
dc.date.issued2026-05-
dc.identifier.citation61en_US
dc.identifier.urihttp://dr.iiserpune.ac.in:8080/xmlui/handle/123456789/11111-
dc.description.abstractCertain anti-ferromagnets are known as weak ferromagnets (WFMs). These magnetic crystals display a weak net magnetization which originates from Dzyaloshinskii-Moriya interactions (DMIs) that causes canting of the magnetic moments. Examples include hematite (α-Fe2O3) and RCO3 (R = Mn, Co), which exhibit unusual magnetization dynamics, as observed in remanence measurements using superconducting quantum interference device (SQUID) magnetometry. Prior work has shown existence of a quasistatic remanence with a counterintuitive magnetic field dependence. These measurements also bring forward an ultra-slow magnetization dynamic in these samples. Encapsulation of hematite inside multiwall carbon nanotubes (CNT) enhances the magnitude of this quasi-static remanence, as observed using SQUID magnetometry. It is non-trivial to stabilize hematite inside carbon nanotubes (Fe2O3@CNT) and scale-up well characterized samples of Fe2O3@CNT prepared in different batches. Furthermore, AC susceptibility, ac-χ, measurements are yet not reported on such hybrids of Fe & Fe2O3@CNT. Here ac-χ can be a more sensitive probe for understanding the unusual magnetization dynamics, especially through frequency dependence. This project pertains to synthesis of α-Fe2O3@CNT, characterization by x-ray diffraction (XRD), Raman, scanning electron microscopy (SEM), and ac susceptibility measurements. The work first requires growth of Fe@CNT via chemical vapour deposition, followed by suitable annealing to convert it to α-Fe2O3@CNT. While the condition of growth using a single zone furnace and a two quartz-tubes based synthesis chamber is routinely done in the lab, during this project, Fe@CNT was prepared using a single quartz-tube. Slight variations in experimental condition also led to significant improvement in the yield. Conversion of Fe@CNT led to a well characterized Fe2O3@CNT. In addition, a few samples with systematically varying fraction of Fe@CNT in Fe2O3@CNT were also prepared and characterized. Three samples with systematically varying mass fraction of Fe2O3@CNT samples were probed using AC–χ measurements to study both linear and nonlinear AC susceptibilities as functions of field, frequency, and temperature. A reference sample of bare hematite crystals in the form of hex-plates were also probed as a reference sample. The real part of the first harmonic susceptibility exhibits a systematic variation in the magnitude of the signal as a function of ferromagnetic content in Fe2O3@CNT and shows signature of the Morin transition associated with the canted-AFM phase. The frequency dependence of the real part of susceptibility shows the time-dependent magnetization dynamics in these Fe2O3@CNT hybrids.en_US
dc.language.isoenen_US
dc.subjectCarbon nanotubesen_US
dc.subjectDzyaloshinskii–Moriya interactionen_US
dc.subjectSpin orbit couplingen_US
dc.subjectAC susceptibilityen_US
dc.titleSynthesis of Fe2O3@CNT and Measurement of Linear & non-Linear Ac- Susceptibility.en_US
dc.typeThesisen_US
dc.description.embargoTwo Yearsen_US
dc.type.degreeBS-MSen_US
dc.contributor.departmentDept. of Physicsen_US
dc.contributor.registration20211202en_US
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