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Naji, M. |
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Motta, Antonella |
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Aletan, Dirar |
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Mohamed, Tarek |
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Ertürk, Emre |
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Taccardi, Nicola |
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Kononenko, Denys |
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Petrov, R. H. | Madrid |
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Alshaaer, Mazen | Brussels |
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Bih, L. |
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Casati, R. |
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Muller, Hermance |
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Kočí, Jan | Prague |
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Šuljagić, Marija |
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Kalteremidou, Kalliopi-Artemi | Brussels |
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Azam, Siraj |
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Ospanova, Alyiya |
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Blanpain, Bart |
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Ali, M. A. |
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Popa, V. |
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Rančić, M. |
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Ollier, Nadège |
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Azevedo, Nuno Monteiro |
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Landes, Michael |
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Rignanese, Gian-Marco |
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Teixeira, Jm
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Topics
Publications (8/8 displayed)
- 2014Analysis of a fibre-optic sensor design based on SPR in nanowire metamaterial filmscitations
- 2013Correlations among magnetic, electrical and magneto-transport properties of NiFe nanohole arrayscitations
- 2011Resonant Tunneling through Electronic Trapping States in Thin MgO Magnetic Junctionscitations
- 2009The effect of pinhole formation/growth on the tunnel magnetoresistance of MgO-based magnetic tunnel junctionscitations
- 2009Electroforming, magnetic and resistive switching in MgO-based tunnel junctionscitations
- 2008Structural, magnetic and transport properties of ion beam deposited Co thin filmscitations
- 2005Multi-step and anomalous reproducible behaviour of the electrical resistivity near the first-order magnetostructural transition of Gd-5(Si0.1Ge0.9)(4)citations
- 2004Peculiar magnetic and electrical properties near structural percolation in metal-insulator granular layerscitations
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article
Multi-step and anomalous reproducible behaviour of the electrical resistivity near the first-order magnetostructural transition of Gd-5(Si0.1Ge0.9)(4)
Abstract
Very detailed measurements of the electrical resistivity of Gd-5(Si0.1Ge0.9)(4) are here reported, with special emphasis on the vicinity of the first-order (magneto structural) martensitic transition which occurs at T-S similar to 87 K. The data cover more than fifty thermal cycles spanning the temperature ranges of 300-10 K (long cycles) and 105-10 K (short cycles). In the initial 10300 K cycles the martensitic transition takes place in three closely-spaced steps, with associated resistance (R) discontinuities and large thermal hysteresis. In a subsequent series of short cycles (10-105 K) a unique transition occurs, exhibiting a common and quite reproducible R(T) behaviour within a small temperature range (Delta T similar to 4 K) below T-S, either in heating or cooling runs. Remarkably, this 'local reproducibility' (within AT) remains in spite of the significant resistance changes which occur outside the A T-range under thermal cycling. In particular the residual resistance systematically increases under thermal cycling, but the corresponding effect is absent in the AT temperature range. This excludes microcracking as a dominant resistive mechanism in our results, pointing to an intrinsic character of the reproducible behaviour just below T-S. We also analyse the R(T) behaviour when changing from long to short thermal cycles, and the R(T) evolution towards a reversible final behaviour, after extended thermal cycling.