2019
DOI: 10.1007/s00339-018-2354-2
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Effect of Zr substitution on the microstructure and magnetic properties of CuFeO2 ceramics

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Cited by 11 publications
(2 citation statements)
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“…The Raman peaks at 456 cm –1 are assigned to the E g (O–Cr–O bending) vibrational modes, and the result is similar to the reported CuFeO 2 . Besides, the peaks at around 576 cm –1 are probably caused by defects like interstitial oxygen atoms or Cu vacancies . The A 1g mode represents the vibrations of Cu–O bonds along the c -axis.…”
Section: Results and Discussionsupporting
confidence: 78%
“…The Raman peaks at 456 cm –1 are assigned to the E g (O–Cr–O bending) vibrational modes, and the result is similar to the reported CuFeO 2 . Besides, the peaks at around 576 cm –1 are probably caused by defects like interstitial oxygen atoms or Cu vacancies . The A 1g mode represents the vibrations of Cu–O bonds along the c -axis.…”
Section: Results and Discussionsupporting
confidence: 78%
“…For example, Dai et al performed magnetic measurements of prepared CuFe 1ÀX Zr X O 2 by using a PPMS. The temperature dependent magnetization (M-T) is recorded in the temperature range of 5-300 K under zero-field cooled (ZFC) conditions and a constant magnetic field of 0.5 T. The field dependent magnetization is recorded in a field variation of 0.5 T at 10 K and 13 K. Magnetic measurements show that the magnetic transition temperatures decrease with the increase in the Zr substitution amount, and all samples exhibit weak FM properties at 10 K and 13 K. 77 Aldirmaz et al measured the magnetism of the prepared CuZnAlNi and CuZnAlMn by using a PPMS. From a magnetic viewpoint, both CuZnAlNi and CuZnAlMn alloys exhibit paramagnetic behavior.…”
Section: Analysis Of Magnetic Materialsmentioning
confidence: 99%