journal article·2014-04

A study of crossover from 3D ferrimagnetic bulk NiCr2O4 compound into 2D spin-glass-like nanophase

H. Singh, T. Ono, T. Chakraborty, K. Srikanth, A. Venimadhav, R. Chandra, C. Mitra, U. Kumar

Journal of Nanoparticle Research· Volume 16· Issue 4
Publisher page

Abstract

In this report, the magnetic behaviour of $NiCr2O4$ bulk and nanoparticle samples under different applied magnetic field has been investigated extensively. Nanoparticles of $NiCr2O4$ were obtained by mechanical milling of polycrystalline powder prepared by polyol method. FC-ZFC measurement of bulk at different applied magnetic field has revealed the existence of a ferrimagnetic transition around 66K followed by an antiferromagnetic transition close to 30K. However, its nano counterpart has shown remarkable change in magnetic properties - a suppression of ferrimagnetic transition accompanied by strengthening low temperature magnetic phase and observation of a new transition at 90K ($T_P$), which is weakly magnetic in nature. The frequency dependent ac susceptibility data of nanoparticle have been fitted to the well known de Almedia-Thouless equation and a $H2/3$ dependence of the low temperature peak is observed with a resulting zero field freezing temperature ($T_f^0$) equal to 10.1K. Further, the dynamical behaviour near freezing temperature has been analysed in terms of critical behaviour and the obtained fitted parameters values being as $τ_0$(relaxation time constant) = $3.6 X 10-6s$, $T_f^0=8.7$K and $zν= 11.1$. Moreover, Vogel-Fulcher law has been used to understand the nature of freezing transition and the parameter after fitting are obtained as $E_a/k_B = 58.9$K, $τ_0 = 5.22 \times 10-8$ and $T_0 = 8.03$K. Finally, the spin-glass phase is concluded. Moreover, in contrast to bulk, the $H2/3$ dependence of freezing temperature of nanoparticle sample (75h) does support the 2D surface like spin glass nature.
Source: openaire · Quality: candidate unverified · Source record ↗

Research context

OpenAlex topics: Theoretical and Computational Physics · Multiferroics and related materials · Magnetic Properties and Synthesis of Ferrites

SciVX discovery tags are terminology-based. OpenAlex topics are source-provided classifications.

References (28)

Show source-provided references
1. Almeida JRL, Thouless DJ (1978) Stability of the Sherrington–Kirkpatrick solution of a spin glass model. J Phys A 11:983–990. doi: 10.1088/0305-4470/11/5/02810.1088/0305-4470/11/5/028 ↗
2. Batlle X, Labarta A (2002) Finite-size effects in fine particles: magnetic and transport properties. J Phys D Appl Phys 35:R15–R42. doi: 10.1088/0022-3727/35/6/20110.1088/0022-3727/35/6/201 ↗
3. Bedanta S, Kleemann W (2009) Supermagnetism. J Phys D Appl Phys 42:013001–013029. doi: 10.1088/0022-3727/42/1/01300110.1088/0022-3727/42/1/013001 ↗
4. Bock N, Riminucci A, Dionigi C, Russo A, Tampieri A, Landi E, Goranov VA, Marcacci M, Dediu V (2010) A novel route in bone tissue engineering: magnetic biomimetic scaffolds. Acta Biomater 6:786–796. doi: 10.1016/j.actbio.2009.09.01710.1016/j.actbio.2009.09.017 ↗
5. Buschow KHJ (2001) Handbook of magnetic material. Buschow KHJ (ed) North Holland, Amsterdam. 13:423–424
6. Chen XH, Zhang HT, Wang CH, Luo XG, Li PH (2009) Effect of particle size on magnetic properties of zinc chromite synthesized by sol–gel method. Appl Phys Lett 81:4419–4421. doi: 10.1063/1.152692110.1063/1.1526921 ↗
7. Coey JMD (1971) Noncollinear spin arrangement in ultrafine ferrimagnetic crystallites. Phys Rev Lett 27:1140–1142. doi: 10.1103/PhysRevLett.27.114010.1103/PhysRevLett.27.1140 ↗
8. Corot C, Robert P, Idée JM, Port M (2006) Recent advances in iron oxide nanocrystal technology for medical imaging. Adv Drug Delivery Rev 58:1471–1504. doi: 10.1016/j.addr.2006.09.01310.1016/j.addr.2006.09.013 ↗
9. Crottaz O, Kubel F, Schmid H (1997) Jumping crystals of the spinels NiCr2O4 and CuCr2O4. J Mater Chem 7:143–146. doi: 10.1039/A604758K10.1039/a604758k ↗
10. Edwards EA, Anderson PW (1975) Theory of spin glasses. J Phys F Met Phys 5:965–974. doi: 10.1088/0305-4608/5/5/01710.1088/0305-4608/5/5/017 ↗
11. Ishibashi H, Yasumi T (2007) Structural transition of spinel compound NiCr2O4 at ferrimagnetic transition temperature. J Magn Magn Mater 310:e610–e612. doi: 10.1016/j.jmmm.2006.10.113110.1016/j.jmmm.2006.10.1131 ↗
12. Klemme S, Miltenburg JC (2002) Thermodynamic properties of nickel chromite (NiCr2O4) based on adiabatic calorimetry at low temperatures. Phys Chem Miner 29:663–667. doi: 10.1007/s00269-002-0280-410.1007/s00269-002-0280-4 ↗
13. Kneller EF, Luborsky FE (1963) Particle size dependence of coercivity and remanence of single domain particles. J Appl Phys 34:656–658. doi: 10.1063/1.172932410.1063/1.1729324 ↗
14. Kodama RH, Berkowitz AE, McNiff EJ Jr, Foner S (1996) Surface spin disorder in NiFe2O4 nanoparticles. Phys Rev Lett 77:394–397. doi: 10.1103/PhysRevLett.77.39410.1103/PhysRevLett.77.394 ↗
15. Krupika S, Novak P (1982) Ferromagnetic materials. Wolfarth EP (ed) North-Holand Amsterdam 3:189
16. Mufti N, Nugroho AA, Blake GR, Palstra TTM (2002) Magnetodielectric coupling in frustrated spin systems: the spinels MCr2O4 (M = Mn, Co and Ni). J Phys Cond Mat 22:075902–075907. doi: 10.1088/0953-8984/22/7/07590210.1088/0953-8984/22/7/075902 ↗
17. Mukadam MD, Yusuf SM, Sharma P, Kulshreshtha SK, Dey GK (2005) Dynamics of spin clusters in amorphous Fe2O3. Phys Rev B 72:174408–174414. doi: 10.1103/PhysRevB.72.17440810.1103/PhysRevB.72.174408 ↗
18. Mydosh JA (1993) Spin glasses: an experimental introduction. Taylor and Francis, London
19. Pareta RA, Taylor E, Webster TJ (2008) Increased osteoblast density in the presence of novel calcium phosphate coated magnetic nanoparticles. Nanotechnology 19:265101–265107. doi: 10.1088/0957-4484/19/26/26510110.1088/0957-4484/19/26/265101 ↗
20. Parker FT, Foster MW, Margulies DT, Berkowitz AE (1993) Spin canting, surface magnetization, and finite-size effects in γ-Fe2O3 particles. Phys Rev B 47:7885–7891. doi: 10.1103/PhysRevB.47.788510.1103/PhysRevB.47.7885 ↗
21. Prince E (1961) Structure of nickle chromite. J Appl Phys 32:68S–69S. doi: 10.1063/1.200050410.1063/1.2000504 ↗
22. Souletie J, Tholence JL (1985) Critical slowing down in spin glasses and other glasses: Fulcher versus power law. Phys Rev B 32:516–519. doi: 10.1103/PhysRevB.32.51610.1103/PhysRevB.32.516 ↗
23. Sun C, Lee JSH, Zhang M (2008) Magnetic nanoparticles in MR imaging and drug delivery. Adv Drug Delivery Rev 60:1252–1265. doi: 10.1016/j.addr.2008.03.01810.1016/j.addr.2008.03.018 ↗
24. Tejada J, Ziolo RF, Zhang XX (1996) Quantum tunneling of magnetization in nanostructured materials. Chem Mater 8:1784–1792. doi: 10.1021/cm960200310.1021/cm9602003 ↗
25. Tejada J, Zhang XX, del Barco E, Hernandez JM, Chudnovsky EM (1997) Macroscopic resonant tunneling of magnetization in ferritin. Phys Rev Lett 79:1754–1757. doi: 10.1103/PhysRevLett.79.175410.1103/PhysRevLett.79.1754 ↗
26. Tomiyasu K, Kagomiya I (2004) Magnetic structure of NiCr2O4 studied by neutron scattering and magnetization measurements. J Phys Soc Jpn 73:2539–2542. doi: 10.1143/JPSJ.73.253910.1143/JPSJ.73.2539 ↗
27. Tomiyasu K, Hiraka H, Ohoyama K, Yamada K (2008) Resonance-like magnetic excitations in spinel ferrimagnets FeCr2O4 and NiCr2O4 observed by neutron scattering. J Phys Soc Jpn 77:124703–1–124703-5. doi: 10.1143/JPSJ.77.12470310.1143/JPSJ.77.124703 ↗
28. Ueda H, Mitamura H, Goto T, Ueda Y (2006) Successive field-induced transitions in a frustrated antiferromagnet HgCr2O4. Phys Rev B 73:094415–094420. doi: 10.1103/PhysRevB.73.09441510.1103/PhysRevB.73.094415 ↗