1887
banner image
No data available.
Please log in to see this content.
You have no subscription access to this content.
No metrics data to plot.
The attempt to load metrics for this article has failed.
The attempt to plot a graph for these metrics has failed.
Magnetic properties of Sm0.1Ca0.9MnO3 nanoparticles
Rent:
Rent this article for
USD
10.1063/1.4754310
/content/aip/journal/jap/112/6/10.1063/1.4754310
http://aip.metastore.ingenta.com/content/aip/journal/jap/112/6/10.1063/1.4754310
View: Figures

Figures

Image of FIG. 1.
FIG. 1.

(a) XRD spectra of SCMO25 and SCMO60. Indexing is done in the orthorhombic setting of the Pnma space group. (b) Rietveld plot for SCMO60 sample. The experimental data points are indicated by open circles, the calculated and difference patterns are shown by solid lines. The Bragg positions of the reflections of the orthorhombic manganite are indicated by vertical lines below the pattern.

Image of FIG. 2.
FIG. 2.

(a) High-resolution (phase contrast) transmission electron microscopy image and (b) energy dispersive spectrum of SCMO25 sample.

Image of FIG. 3.
FIG. 3.

Temperature dependence of zero field cooled MZ FC (open symbols) and field cooled M FC (solid symbols) magnetization of SCMO25 and SCMO60 recorded in magnetic field H = 100 Oe, 1 kOe (a),(b), and 15 kOe (c),(d).

Image of FIG. 4.
FIG. 4.

Temperature dependence of real (χ′) (a),(b) and imaginary (χ″) (c),(d) component of ac-susceptibility measured during heating at ac magnetic field of 10 Oe and different frequencies. Insets in (a) and (b): the inverse of the real part (χ′) of ac-susceptibility measured at 10 kHz. Dashed lines show fits to Curie-Weiss law. Insets to (c) and (d) show the inverse of the real part (χ′) of ac-susceptibility measured at 10 kHz and temperature dependence of H/M measured at 15 kOe.

Image of FIG. 5.
FIG. 5.

(a),(b) Magnetic field dependences of magnetization of SCMO25 and SCMO60 at various temperatures, as measured after FC and ZFC procedures. Insets: zoom into low field part of hysteresis loops measured after FC and ZFC at T = 10 K. (c) Coercive field of SCMO samples as a function of the temperature.

Image of FIG. 6.
FIG. 6.

Temperature dependence of H EB and M EB for LCMO25 (a) and LCMO60 (b) samples determined from hysteresis loops recorded within field range ±15 kOe after FC in 15 kOe. Solid lines in (a) are best fits of H EB = H EB(0)exp(−T/T 1) and M EB = M EB(0)exp(−T/T 3) for SCMO25, while the solid line in Fig. 6(b) represents fit of H EB = H EB(0)exp(−T/T 1).

Image of FIG. 7.
FIG. 7.

(a),(b) Magnetic field dependences of magnetization for SCMO25 and SCMO60 at 10 K, measured in magnetic field range ±90 kOe after FC and ZFC. Insets: zoom at low field part of the hysteresis loops measured at T = 10 K after FC and ZFC. Spontaneous magnetization M S, evaluated by linear extrapolation to H = 0 of the high field magnetization recorded after ZFC, is equal to M S ≈ 4.95 emu/g = 0.136 μ B/f.u. for SCMO25 and to M S ≈ 16.47 emu/g = 0.454 μ B/f.u. for SCMO60.

Image of FIG. 8.
FIG. 8.

(a) Variation of coercive field H C and the exchange bias field vs. H cool for SCMO25 at T = 10 K. (b) Magnetic coercivity M C and vertical shift M EB as a function of H cool for SCMO25 at T = 10 K.

Image of FIG. 9.
FIG. 9.

The temperature variation of the remanent magnetization of SCMO25 (a) and SCMO60 (b) at ambient and applied pressure.

Image of FIG. 10.
FIG. 10.

Field dependence of TRM and IRM for 25 nm LCMO NPs at 10 K.

Image of FIG. 11.
FIG. 11.

(a) Temperature dependence of ZFC magnetization recorded in various magnetic field. (b, c) Fitting of Eqs. (5) and (6) to experimental points of temperature of the maximum in ZFC magnetization.

Image of FIG. 12.
FIG. 12.

(a) Temperature dependence of the reference magnetization (open triangles) and of the magnetization with a stop and waiting protocol, (open squares) at a magnetic field H = 10 Oe. First, 25 nm SCMO sample was cooled from 300 K to 10 K with the rate of 3 K/min. Then the magnetization was measured during heating. After that, the system was cooled again from 300 K to a stop temperature T S. The system was annealed at a stop temperature T S = 40 K for the wait time 20 000 s. Next, the cooling was resumed and sample was cooled from T S to 10 K. At 10 K the magnetic field was turned on and the magnetization was measured at heating. (b) ΔM =  vs. temperature.

Image of FIG. 13.
FIG. 13.

Schematic plot of the morphological structure of SCMO nanoparticle. D is the particle diameter, λ0 is the disordered layer thickness, λm is the magnetic disorder length, V sd is the structural disorder volume, and V mo is the magnetically ordered volume.

Loading

Article metrics loading...

/content/aip/journal/jap/112/6/10.1063/1.4754310
2012-09-27
2014-04-19
Loading

Full text loading...

This is a required field
Please enter a valid email address
752b84549af89a08dbdd7fdb8b9568b5 journal.articlezxybnytfddd
Scitation: Magnetic properties of Sm0.1Ca0.9MnO3 nanoparticles
http://aip.metastore.ingenta.com/content/aip/journal/jap/112/6/10.1063/1.4754310
10.1063/1.4754310
SEARCH_EXPAND_ITEM