Experimental investigation of superspin glass dynamics
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Experimental investigation of Superspin glass dynamics. Dinah Parker 1 , E. Dubois 2 , V. Dupuis 3 , F. Ladieu 1 , G. Mériguet 2 , R. Perzynski 3 and E. Vincent 1. 1 Service de Physique de l’Etat Condensé DSM/DRECAM, CEA-Saclay (CNRS URA 2464)

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Experimental investigation of superspin glass dynamics

Experimental investigation of Superspin glass dynamics

Dinah Parker1, E. Dubois2, V. Dupuis3, F. Ladieu1, G. Mériguet2, R. Perzynski3 and

E. Vincent1

1Service de Physique de l’Etat Condensé

DSM/DRECAM, CEA-Saclay

(CNRS URA 2464)

2Laboratoire des Liquides Ioniques et Interfaces Chargées,Université Pierre et Marie Curie

3Laboratoire des Milieux Désordonnés et Hétérogènes,

Université Pierre et Marie Curie

Work supported by EC program DYGLAGEMEM


Superspin glasses

Concentrated nanoparticle system

Superspin glass

(interacting superspins)

Dilute nanoparticle system

superparamagnet

(non-interacting superspins)

Superspin Glasses

  • Small magnetic nanoparticle→ single domain magnetism

  • Response of single nanoparticle ~ response of single spin → a ‘superspin’

  • Varying concentration of nanoparticles in a liquid dispersion changes interparticle interaction

  • To what extent do superspin glasses behave like atomic spin glasses?


Summary of previous work on superspin glasses

  • Experimental investigations of superspin glasses have revealed some similarities with atomic spin glasses including

    • The behaviour of the AC and DC magnetisation vs. temperature

    • Critical behaviour indicative of collective dynamics (derived from AC susceptibility measurements)

    • Aging and memory effects

Uppsala University, Sweden- P. Nordblad, P. Jönsson, P. Svedlindh, M. F. Hansen, T. Jonsson, J. García-Palacios

National Research Institute for Metals, Tsukuba, Japan- H. Mamiya, I. Nakatani, T. Furubayashi

University of Tokyo, Japan- H. Takayama, M Sasaki, P. Jönsson

University of Versailles/University of Pierre and Marie Curie, France and Institute of Materials Chemistry, Italy- J. L. Dormann, E. Tronc, M. Noguès, D. Fiorani


Fe 2 o 3 nanoparticles

g-Fe2O3

γ-Fe2O3 nanoparticles

  • γ-Fe2O3 nanoparticles dispersed in H2O1

  • Citrate molecules adsorbed onto particle surface to prevent aggregation

  • Mean diameter ~ 8.5 nm

  • Lognormal distribution of particle size (σ ≈ 0.25)

  • Volume fractions (Φ) ranging from 0.01 % →35 %

  • Dipole-dipole interaction energies varying from << 1 K to ~ 45 K

1F. Gazeau, J. C. Bacri, F. Gendron, R. Perzynski, Yu. L. Raikher, V. I. Stepanov and E. Dubois, J. Magn Magn. Mat. 186 (1998) 175


Dc magnetisation vs temperature measurements
DC Magnetisation vs. Temperature Measurements

  • Dilute sample shows increase in FC magnetisation below TB→ indicative of superparamagnetic-like behaviour

  • In concentrated sample FC curve is flattened below Tg → characteristic of atomic spin glass behaviour

  • Increase in transition temperature seen in concentrated sample


Field Effects

  • High fields give a flattening of the ZFC peak and a decrease in Tg, also seen in atomic spin glasses

  • Observe a decrease in M/H with increasing H

  • Tpeak remains constant up to ~ 5 Oe, much lower than for an atomic spin glass

  • Typical superspin ~ 104 spins → enhanced Zeeman coupling w.r.t. atomic spin glasses


Ac susceptibility vs temperature measurements
AC Susceptibility vs. Temperature Measurements

  • See shift in χ’ peak with frequency as expected for both superparamagnets and spin glasses

  • We can apply Arrhenius Law:

  • τ= τ0 exp (Ea/kBTpeak)

  • For dilute sample (Φ = 1 %) τ0 ≈ 10-9 s

  • For concentrated sample (Φ = 35 %) τ0 ≈ 10-19 s → unphysically small as found for atomic spin glasses

  • Suggests collective behaviour driven by interparticle interactions

  • Previous studies have confirmed existence of a critical slowing down reminiscent of spin glass behaviour1

1 M F Hansen, P Jönsson, P Nordblad and P Svedlindh, J. Phys.:Condensed matter, 14, 4901 (2002)


Memory effects

  • Make a stop during the cooling for 20000 s at 60 K (≈ 0.6 Tg)

  • See relaxation of the AC susceptibility

  • On reheating at constant rate the susceptibility follows the cooling curve

  • Memory effect

  • Multiple memory dips can be made


T

ΔT

T1

Tg

T2

t

0

t1

t2

t3

Temperature Cycling

T1 = 60 K = 0.6 Tg

t2 = τ0 eB/(T1-ΔT), teff = τ0 eB/T1

If B is constant with T (simple thermal slowing down)

→ teff/t2 = (t2/τ0)-ΔT/T1

With τ0= 10-9s, data is inconsistent with calculation

Similar to Heisenberg-like spin glasses1

1 V. Dupuis, E. Vincent, J-P Bouchaud, J. Hammann, A. Ito, H. A. Katori; Phys. Rev. B 64 174204 (2001)


Thermoremnant magnetisation trm

TRM protocol

T

tw = waiting time

t = measuring time

Φ = 35 %

T

TM= 0.7 Tg (71 K)

H = 0.5 Gauss

g

Tm

H

0

t

tw

t

Thermoremnant Magnetisation (TRM)

  • In an atomic spin glass curves scale ~ t/tw μ

  • Horizontal spacing of relaxation curves much less than seen for atomic spin glasses (μ <<1?)

  • but tinflection ≈ tw (indicating μ ~ 1) as in spin glasses


Scaling of the TRM curves

  • Distribution of particle size leads to distribution of anisotropy energies (Ea = KV)

  • Average anisotropy energy of the same order as average dipole-dipole interaction→ <Ea>~ <J>

  • Only smallest particles will have Ea << <J> (as in an atomic spin glass)

  • Larger particles with Ea≥<J> may relax independently of interparticle interactions

  • → correct M/MFC by subtracting –B ln(t/τ0) term to account for superparamagnetic-like relaxation of larger particles

  • Scaling of the relaxation curves can be achieved after subtracting –B ln(t/τ0) term

  • Scaling parameters are comparable to those found for atomic spin glasses

*λ/twμ= tw1-μ[(1+t/tw)1-μ-1]/[1-µ] ≈ t/twμ


Do these TRM results conclude spin glass physics?

TRM protocol

ZFC protocol

T

T

g

Tm

H

0

t

T

tw

t

tw = waiting time

t = measuring time

tw = waiting time

t = measuring time

T

g

Tm

H

0

t

tw

t

  • No! Aging observed in TRM experiments can be attributed to superparamagnetic behaviour. 1,2

  • Simulations of non-interacting nanoparticle systems have shown aging and memory effects1

  • Aging observed due to the wide distribution of τ arising from particle volume distribution → leads to slow dynamics which can evolve during tw

  • Not the case for the ZFC relaxation procedure as system is in ‘effective equilibrium’ during tw

  • Only aging in TRM and ZFC experiments can indicate spin glass physics

1M. Sasaki, P.E. Jönsson, H. Takayama and H.Mamiya, Phys. Rev. B 71 (10)104405 (2005)

2 M Sasaki, P Jönsson, H Takayama, Nordblad P; Phys. Rev. Lett.93, 139701 (2004)


Zero Field Cooled Relaxation

  • Observe a positive relaxation of the ZFC magnetisation

  • Adding a –B ln(t/τ0) term enables scaling of the relaxation curves

  • ZFC relaxation curves can be roughly scaled with parameters similar to those for the TRM procedure

  • Indicates collective dynamics, not simply a relaxation of the superparamagnetic state


Conclusions
Conclusions

  • Concentrated dispersion of γ-Fe2O3 nanoparticles shows many similarities with atomic spin glasses

    - characteristic M vs T behaviour

    - memory effects in AC susceptibility

    - T-shift relaxation behaviour similar to Heisenberg spin-glass

  • Aging is seen in both TRM and ZFC relaxation experiments

  • We propose a new term, –B ln(t/τ0), to account for superparamagnetic relaxation in the superspin glass relaxation curves

  • Scaling of the relaxation curves gives parameters comparable with those found for atomic spin glasses


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