Low-Temperature Deposition of Graphite Coating on La(Fe, Co, Si)<sub>13</sub>B<sub>0.2</sub> for Room-Temperature Magnetic Refrigeration

Due to the larger magnetic entropy change Δ<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S<sub>M</sub></i> and the much lower raw material cost, La(Fe,Co,Si)<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">13</sub> materials have the potential to replace the room-temperature magnetic refrigeration prototype material Gd. In this work, we have developed a simple chemical vapor deposition (CVD) method for in-situ graphite deposition on the surface of La(Fe,Co,Si)<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">13</sub>B<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</sub>. Facilitated by the decomposition of the solid carbon-source polyethylene glycol (PEG), the CVD process could be carried out at a low temperature of 400 °C and in a short duration of 20 min, which ensures no α-Fe precipitation from and carbon atom diffusion into the La-Fe-Si material. These 400-700 nm thick coatings could significantly enhance the anti-corrosive property with a positive shift of corrosion potential Ecorr from -788 mV to above -600 mV and a reduction of the corrosion current density <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">I<sub>corr</sub></i> from 1.67×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-5</sup> to 9.14×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-6</sup> A/cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup>, accompanied by a concurrent enhancement of the thermal conductivity. More favorably, a large Δ<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S<sub>M</sub></i> of ~4 J/kgK at 286 K and a relative cooling power (RCP) value of ~98 J/kg in 0-1.5 T were maintained.

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Journal
IEEE Transactions on Magnetics
Published
2025-04-21
DOI
https://doi.org/10.1109/tmag.2025.3562599
Primary Topic
Magnetic Properties of Alloys
Type
article
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article

Low-Temperature Deposition of Graphite Coating on La(Fe, Co, Si)13B0.2 for Room-Temperature Magnetic Refrigeration

Q. Zhang, Yingwei Song, Juan Cheng, Xinguo Zhao et al.
IEEE Transactions on Magnetics
Magnetic Properties of Alloys
article

Low-Temperature Deposition of Graphite Coating on La(Fe, Co, Si)13B0.2 for Room-Temperature Magnetic Refrigeration

Q. Zhang, Yingwei Song, Juan Cheng, Xinguo Zhao, Chunhui Gao, Naikun Sun, Zhen Yan, Jiaohong Huang
article en

Abstract

Due to the larger magnetic entropy change Δ<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S<sub>M</sub></i> and the much lower raw material cost, La(Fe,Co,Si)<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">13</sub> materials have the potential to replace the room-temperature magnetic refrigeration prototype material Gd. In this work, we have developed a simple chemical vapor deposition (CVD) method for in-situ graphite deposition on the surface of La(Fe,Co,Si)<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">13</sub>B<sub xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">0.2</sub>. Facilitated by the decomposition of the solid carbon-source polyethylene glycol (PEG), the CVD process could be carried out at a low temperature of 400 °C and in a short duration of 20 min, which ensures no α-Fe precipitation from and carbon atom diffusion into the La-Fe-Si material. These 400-700 nm thick coatings could significantly enhance the anti-corrosive property with a positive shift of corrosion potential Ecorr from -788 mV to above -600 mV and a reduction of the corrosion current density <italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">I<sub>corr</sub></i> from 1.67×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-5</sup> to 9.14×10<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">-6</sup> A/cm<sup xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">2</sup>, accompanied by a concurrent enhancement of the thermal conductivity. More favorably, a large Δ<italic xmlns:mml="http://www.w3.org/1998/Math/MathML" xmlns:xlink="http://www.w3.org/1999/xlink">S<sub>M</sub></i> of ~4 J/kgK at 286 K and a relative cooling power (RCP) value of ~98 J/kg in 0-1.5 T were maintained.

IEEE Transactions on MagneticsVol. 61(6)
Shenyang Ligong University (CN), Chinese Academy of Sciences (CN), Baotou Research Institute of Rare Earths (CN)
National Natural Science Foundation of China
Affordable and clean energy
Openalex Percentile: Top 95%
Magnetic Properties of Alloys
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