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Spin glass behaviour in a new ternary intermetallic, U 3 Fe 4+x Al 12-x A.P. Gonçalves 1, O. Tougait 2, H. Noël 2 1 Departamento de Química, Instituto.

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Presentation on theme: "Spin glass behaviour in a new ternary intermetallic, U 3 Fe 4+x Al 12-x A.P. Gonçalves 1, O. Tougait 2, H. Noël 2 1 Departamento de Química, Instituto."— Presentation transcript:

1 Spin glass behaviour in a new ternary intermetallic, U 3 Fe 4+x Al 12-x A.P. Gonçalves 1, O. Tougait 2, H. Noël 2 1 Departamento de Química, Instituto Tecnológico e Nuclear/CFMC-UL, Sacavém, Portugal 5 Sciences Chimiques de Rennes, Laboratoire de Chimie du Solide et Matériaux. UMR CNRS 6226, Université de Rennes 1, Avenue de Général Leclerc, 35042 Rennes, France

2 Outline Introduction Experimental Crystal structure Magnetic properties Conclusions

3 Phase equilibrium study of U-Fe-Al Introduction (1)UFe 2 Al 10 (2)U 2 Fe 4 Al 13 (3)UAl 2-x Fe x (4)U 3 Fe 4+x Al 12-x (5)UFe x Al 12-x (6)U 2 Fe 17­x Al x (7)UFe 1+x Al 1-x (8)U 2 Fe 12 Al 5 (9)UFe 2-x Al x R

4 U 3 Fe 4+x Al 12-x crystallizes in the Gd 3 Ru 4 Al 12 structure type

5 U atoms form a distorted Kagome net

6 Good candidate for spin glass due to geometrical frustration. ?

7 Samples prepared by arc-melting/annealing (850ºC, 2 weeks); Analyzed by powder XRD and Observed by SEM; Characterized by ac-susceptibility (30-10000 Hz, 1-500 Oe) and magnetization (ZFC/FC, 0-7 T) measurements between 2-300 K; Experimental

8 Crystal structure U 3 Fe 4 Al 12 P

9 AtomWyckoff positionxyzO.F.B iso, Å 2 U16h0.1972(2)0.3945(4)1/40.9(1.0)0.01* Al112k0.1589(8)0.318(2)0.9220(8)1.1(1.3)0.05* Al26h0.567(1)0.134(2)1/41.4(1.6)0.05* Al34f1/32/30.009(2)1.0(1.2)0.05* Al42b001/41.0(1.1)0.01* Fe16g1/5001.0(1.1)0.01* Fe22a0001.2(1.3)0.04* * - fixed parameter Cell parameters, Åa = 8.7516(3) c = 9.2653(4) RPRP 19.7 R WP 17.9 2 12.6 RBRB 7.86 RFRF 5.70 U 3 Co 4+x Al 12-x 8.7060(2) 9.2230(3) U 3 Co 4+x Al 12-x 8.7060(2) 9.2230(3) 0.1928(2)0.3857(3)1/4 0.1622(8)0.3244(2)0.9238(3) 0.5637(3)0.1274(3)1/4 1/32/30.0084(2) 001/4 1/500 000

10 -UFeAl 3

11 U-U = 3,553(2) Å U-Fe = 3,282(4) Å U-Al = 3,001(4) Å Fe-Al = 2,316(2) Å Fe-Fe = 4,358(1) Å

12 Magnetic properties μ

13 χ = C/(T- ) = -25.5(1) K, μ eff = 3.54(1) μ B (considered 1U:1Fe:3Al) μ eff (U 3+ ) = 3.62 μ B or μ eff (U 4+ ) = 3.58 μ B U intermetallics 2 – 3 μ B Fe contribution

14

15

16 R

17

18 T f / [T f log( )] Spin-glass: 0.004 - 0.03 (strong interactions between magnetic moments) Superparamagnets: 0.25 - 0.35 (weak interactions between clusters) U 3 Fe 4 Al 12 : 0.03 true spin-glass

19 Arrhenius law = 0 exp(-T A /T f ) Vogel-Fulcher law = 0 exp[-T A /(T f -T 0 )] 0 10 33 Hz and T A = E a /k B = 535 K Frequency dependence of the freezing temperature

20 0 10 13 Hz

21 Conclusions U 3 Fe 4 Al 12 is a true spin glass; Fe magnetic contribution; Spin glass origin related to the topological frustration of the U moments and to the disorder at the Fe sites.

22 Acknowledgements GRICES/EGIDE 2007-2008;


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