Shell thickness and dynamic magnetic field effects on the critical phenomena of magnetic core-shell nanoparticles with spherical geometry

YÜKSEL Y.

PHYSICA B-CONDENSED MATTER, cilt.508, ss.62-68, 2017 (SCI-Expanded) identifier identifier

  • Yayın Türü: Makale / Tam Makale
  • Cilt numarası: 508
  • Basım Tarihi: 2017
  • Doi Numarası: 10.1016/j.physb.2016.12.022
  • Dergi Adı: PHYSICA B-CONDENSED MATTER
  • Derginin Tarandığı İndeksler: Science Citation Index Expanded (SCI-EXPANDED), Scopus
  • Sayfa Sayıları: ss.62-68
  • Anahtar Kelimeler: Magnetically ordered materials, Nanostructured materials, Surfaces and interfaces, Phase diagrams, Phase transitions, Monte Carlo simulation, CYLINDRICAL ISING NANOWIRE, MONTE-CARLO-SIMULATION, CORE/SHELL NANOPARTICLES, PHASE-DIAGRAMS, EXCHANGE BIAS, FERRIMAGNETIC NANOPARTICLE, MIXED SPIN-1/2, MODEL, COMPENSATION, BEHAVIOR
  • Dokuz Eylül Üniversitesi Adresli: Evet

Özet

By using Monte Carlo simulations for classical Heisenberg spins, we study the critical phenomena and ferrimagnetic properties of spherical nanoparticles with core-shell geometry. The particle core is composed of ferromagnetic spins, and it is coated by a ferromagnetic shell. Total size of the particle is fixed but the thickness of the shell is varied in such a way that the shell layer is grown at the expense of the core. Effects of the shell thickness, as well as dynamic magnetic field parameters such as oscillation period and field amplitude on the magnetization profiles, dynamic hysteresis loops and phase diagrams have been investigated for the present system. It has been found that as the shell thickness varies then the easy axis magnetization of the overall system may exhibit Q-, P-, L-and N-type behaviors based on the Neel terminology. We also found that three distinct anomalies originate in the thermal variation of specific heat with increasing field period. Dynamic hysteresis loops corresponding to off-axial magnetization components exhibit unconventional behavior such as double rings with symmetric shapes around the vertical axis over the h(t) = 0 line which may originate due to the stochastic resonance behavior of these components.