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Strain-Induced Exchange Bias Effects in Chemically Ordered ${hbox {Pt}}_{3}{hbox {Fe}}$ Single Crystal

机译:化学有序$ {hbox {Pt}} _ {3} {hbox {Fe}} $单晶中的应变诱导交换偏置效应

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Magnetic hysteresis loops have been studied in chemically ordered ${hbox {Pt}}_{3}{hbox {Fe}}$ single crystals after plastic deformation with various levels of strain up to 29.8%. Plastic deformation results in changes of atomic arrangement around glide plane of superlattice dislocations and induces ferromagnetism even at room temperature. We find that magnetic hysteresis loops after field cooling are shifted toward a negative field unlike normal hysteresis loops centered at the origin after zero-field cooling. This shift rapidly decreases with increasing temperature and disappears above $T_{N1}=$ 170 K, which is paramagnetic–antiferromagnetic transition temperature of ${L}1_{2}$ superlattice structure. The results clearly demonstrate the exchange bias effects below $T_{N1}$ in deformed ${hbox {Pt}}_{3}{hbox {Fe}}$ single crystals, where ferromagnetic domains produced around glide plane are magnetically coupled with antiferromagnetic ${L}1_{2}$ matrix.
机译:磁滞回线已经在化学变形后的化学有序$ {hbox {Pt}} _ {3} {hbox {Fe}} $单晶中进行了研究,塑性变形后的应变水平高达29.8%。塑性变形会导致超晶格位错滑行面周围原子排列的变化,甚至在室温下也会引起铁磁性。我们发现,磁场冷却后的磁滞回线向负磁场移动,这不同于零磁场冷却后以原点为中心的正常磁滞回线。这种位移随着温度的升高而迅速减小,并在$ T_ {N1} = $ 170 K以上消失,这是$ {L} 1_ {2} $超晶格结构的顺磁-反铁磁转变温度。结果清楚地表明,在变形的$ {hbox {Pt}} _ {3} {hbox {Fe}} $单晶中,在$ T_ {N1} $以下的交换偏置效应,在滑移面周围产生的铁磁畴与反铁磁磁性耦合$ {L} 1_ {2} $矩阵。

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