Electric polarization along the<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mi>c</mml:mi></mml:math>axis in the ferroelectric helimagnetic phase of<mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:msub><mml:mi mathvariant="normal">CuFe</mml:mi><mml:mrow><mml:mn>1</mml:mn><mml:mtext>−</mml:mtext><mml:mi>x</mml:mi></mml:mrow></mml:msub><mml:msub><mml:mi mathvariant="normal">Ga</mml:mi><mml:mi>x</mml:mi></mml:msub><mml:msub><mml:mi mathvariant="normal">O</mml:mi><mml:mn>2</mml:mn></mml:msub></mml:math><mml:math xmlns:mml="http://www.w3.org/1998/Math/MathML"><mml:mo>(</mml:mo><mml:mrow><mml:mi>x</mml:mi><mml:mo>=</mml:mo><mml:mn>0.035</mml:mn></mml:mrow><mml:mo>)</mml:mo></mml:math>

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Electric polarization along thecaxis in the ferroelectric helimagnetic phase ofCuFe1−xGaxO2(x=0.035)
(CuFe1-xGaxO2(x=0.035)の螺旋磁気強誘電相におけるc軸方向の電気分極)

Chikafumi Kaneko, Taro Nakajima, Setsuo Mitsuda, Yoshikazu Tanaka, Noriki Terada.

Physical Review B 90 [8] 085109. 2014.

Created at: 2016-05-24 17:32:40 +0900 Updated at: 2026-10-30 06:31:31 +0900