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  Remarkable magnetostructural coupling around the magnetic transition in CeCo0.85Fe0.15Si

Correa, V. F., Betancourth, D., Sereni, J. G., Caroca Canales, N., & Geibel, C. (2016). Remarkable magnetostructural coupling around the magnetic transition in CeCo0.85Fe0.15Si. Journal of Physics: Condensed Matter, 28(34): 346003, pp. 1-5. doi:10.1088/0953-8984/28/34/346003.

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Item Permalink: http://hdl.handle.net/21.11116/0000-0001-659F-B Version Permalink: http://hdl.handle.net/21.11116/0000-0001-65A3-5
Genre: Journal Article

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 Creators:
Correa, V F1, Author
Betancourth, D, Author
Sereni, J G, Author
Caroca Canales, N.2, Author              
Geibel, C.3, Author              
Affiliations:
1External Organizations, ou_persistent22              
2Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society, ou_1863462              
3Christoph Geibel, Physics of Quantum Materials, Max Planck Institute for Chemical Physics of Solids, Max Planck Society, ou_1863465              

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 Abstract: We report a detailed study of the magnetic properties of CeCo 0.85 Fe 0.15 Si under high magnetic fields (up to 16 Tesla) measuring different physical properties such as specific heat, magnetization, electrical resistivity, thermal expansion and magnetostriction. CeCo 0.85 Fe 0.15 Si becomes antiferromagnetic at IMG [http://ej.iop.org/images/0953-8984/28/34/346003/cmaa2c83ieqn001.gif] {{T}_{N}}≈ 6.7} K. However, a broad tail (onset at IMG [http://ej.iop.org/images/0953-8984/28/34/346003/cmaa2c83ieqn002.gif] {{{T}_{X}}≈ 13} K) in the specific heat precedes that second order transition. This tail is also observed in the temperature derivative of the resistivity. However, it is particularly noticeable in the thermal expansion coefficient where it takes the form of a large bump centered at T X . A high magnetic field practically washes out that tail in the resistivity. But surprisingly, the bump in the thermal expansion coefficient becomes a well pronounced peak fully split from the magnetic transition at T N . Concurrently, the magnetoresistance also switches from negative to positive above T N . The magnetostriction is considerable and irreversible at low temperature ( IMG [http://ej.iop.org/images/0953-8984/28/34/346003/cmaa2c83ieqn003.gif] {\frac{Δ L}{L}(16~T)∼ 4× {{10}^{-4}} at 2 K) when the magnetic interactions dominate. A broad jump in the field dependence of the magnetostriction observed at low T may be the signature of a weak ongoing metamagnetic transition. Taking altogether the results indicate the importance of the lattice effects on the development of the magnetic order in these alloys.

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Language(s): eng - English
 Dates: 2016-06-292016-06-29
 Publication Status: Published in print
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 Identifiers: DOI: 10.1088/0953-8984/28/34/346003
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Title: Journal of Physics: Condensed Matter
Source Genre: Journal
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Pages: - Volume / Issue: 28 (34) Sequence Number: 346003 Start / End Page: 1 - 5 Identifier: -